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by Thomas M. (Thomas Matthew) St. John
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Title: Things a Boy Should Know About Electricity
Second Edition
Author: Thomas M. (Thomas Matthew) St. John
Release Date: January 14, 2014 [eBook #44665]
Language: English
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THINGS A BOY SHOULD KNOW ABOUT ELECTRICITY
[Illustration]
* * * * *
_BY THE SAME AUTHOR._
=FUN WITH MAGNETISM.= A book and complete outfit of apparatus
for _Sixty-One Experiments_.
=FUN WITH ELECTRICITY.= A book and complete outfit of
apparatus for _Sixty Experiments_.
=FUN WITH PUZZLES.= A book, key and complete outfit for _Four
Hundred Puzzles_.
=FUN WITH SOAP-BUBBLES.= A book and complete outfit of
apparatus for _Fancy Bubbles and Films_.
=FUN WITH SHADOWS.= Including book of instructions with one
hundred illustrations and a complete outfit of apparatus
for _Shadow Pictures, Pantomimes, Entertainments, etc.,
etc._
=HUSTLE-BALL.= An American game. Played by means of magic
wands and polished balls of steel.
=JINGO.= The great war game, including JINGO JUNIOR.
=HOW TWO BOYS MADE THEIR OWN ELECTRICAL APPARATUS.= A book
containing complete directions for making all kinds of
simple apparatus for the study of elementary electricity.
=THE STUDY OF ELEMENTARY ELECTRICITY AND MAGNETISM BY
EXPERIMENT.= This book is designed as a text-book for
amateurs, students, and others who wish to take up a
systematic course of simple experiments at home or in
school.
=THINGS A BOY SHOULD KNOW ABOUT ELECTRICITY.= This book
explains, in simple, straightforward language, many things
about electricity; things in which the American boy is
intensely interested; things he wants to know; things he
should know.
=ANS., OR ACCURACY, NEATNESS AND SPEED.= For teachers and
pupils. Containing study-charts, practice devices and
special methods for accurate, rapid work with figures.
_Ask Your Bookseller, Stationer, or Toy Dealer for our
Books, Games, Puzzles, Educational Amusements, Etc._
CATALOGUE UPON APPLICATION
Thomas M. St. John, 407 West 51st St., New York.
* * * * *
THINGS A BOY SHOULD KNOW ABOUT ELECTRICITY
by
THOMAS M. ST. JOHN, Met. E.
Author of "Fun With Magnetism," "Fun With Electricity,"
"How Two Boys Made Their Own Electrical Apparatus,"
"The Study of Elementary Electricity
and Magnetism by Experiment," etc.
SECOND EDITION
[Illustration]
New York
Thomas M. St. John
407 West 51st Street
1903
Copyright, 1900.
By Thomas M. St. John.
THINGS A BOY SHOULD KNOW ABOUT ELECTRICITY
TABLE OF CONTENTS
CHAPTER PAGE
I. About Frictional Electricty 7
II. About Magnets and Magnetism 21
III. How Electricity is Generated by the Voltaic Cell, 32
IV. Various Voltaic Cells, 36
V. About Push-Buttons, Switches and Binding-Posts, 43
VI. Units and Apparatus for Electrical Measurements, 48
VII. Chemical Effects of the Electric Current, 58
VIII. How Electroplating and Electrotyping are Done, 60
IX. The Storage Battery, and How it Works, 63
X. How Electricity is Generated by Heat, 68
XI. Magnetic Effects of the Electric Current, 71
XII. How Electricity is Generated by Induction, 77
XIII. How the Induction Coil Works, 80
XIV. The Electric Telegraph, and How it Sends Messages, 84
XV. The Electric Bell and Some of its Uses, 91
XVI. The Telephone and How it Transmits Speech, 95
XVII. How Electricity is Generated by Dynamos, 101
XVIII. How the Electric Current is Transformed, 109
XIX. How Electric Currents are Distributed for Use, 114
XX. How Heat is Produced by the Electric Current, 124
XXI. How Light is Produced by the Incandescent Lamp, 129
XXII. How Light is Produced by the Arc Lamp, 135
XXIII. X-Rays, and How the Bones of the Human Body are
Photographed, 141
XXIV. The Electric Motor, and How it Does Work, 147
XXV. Electric Cars, Boats and Automobiles, 154
XXVI. A Word About Central Stations, 162
XXVII. Miscellaneous Uses of Electricity, 165
TO THE READER
For the benefit of those who wish to make their own electrical
apparatus for experimental purposes, references have been made
throughout this work to the "Apparatus Book;" by this is meant the
author's "How Two Boys Made Their Own Electrical Apparatus."
For those who wish to take up a course of elementary electrical
experiments that can be performed with simple, home-made apparatus,
references have been made to "Study;" by this is meant "The Study of
Elementary Electricity and Magnetism by Experiment."
THE AUTHOR.
Things A Boy Should Know About Electricity
CHAPTER I.
ABOUT FRICTIONAL ELECTRICITY.
=1. Some Simple Experiments.= Have you ever shuffled your feet along
over the carpet on a winter's evening and then quickly touched your
finger to the nose of an unsuspecting friend? Did he jump when a bright
spark leaped from your finger and struck him fairly on the very tip of
his sensitive nasal organ?
[Illustration: Fig. 1.]
Did you ever succeed in proving to the pussy-cat, Fig. 1, that
something unusual occurs when you thoroughly rub his warm fur with your
hand? Did you notice the bright sparks that passed to your hand when it
was held just above the cat's back? You should be able to see, hear,
and feel these sparks, especially when the air is dry and you are in a
dark room.
Did you ever heat a piece of paper before the fire until it was real
hot, then lay it upon the table and rub it from end to end with your
hand, and finally see it cling to the wall?
Were you ever in a factory where there were large belts running rapidly
over pulleys or wheels, and where large sparks would jump to your hands
when held near the belts?
If you have never performed any of the four experiments mentioned, you
should try them the first time a chance occurs. There are dozens of
simple, fascinating experiments that may be performed with this kind of
electricity.
=2. Name.= As this variety of electricity is made, or generated, by
the friction of substances upon each other, it is called _frictional_
electricity. It is also called _static_ electricity, because it
generally stands still upon the surface of bodies and does not "flow in
currents" as easily as some of the other varieties. Static electricity
may be produced by induction as well as by friction.
[Illustration: Fig. 2.]
=3. History.= It has been known for over 2,000 years that certain
substances act queerly when rubbed. Amber was the first substance upon
which electricity was produced by friction, and as the Greek name for
amber is _elektron_, bodies so affected were said to be _electrified_.
When a body, like ebonite, is rubbed with a flannel cloth, we say that
it becomes _charged with electricity_. Just what happens to the ebonite
is not clearly understood. We know, however, that it will attract
light bodies, and then quickly repel them if they be conductors. Fig.
2 shows a piece of tissue-paper jumping toward a sheet of ebonite that
has been electrified with a flannel cloth.
=4. Conductors and Non-Conductors.= Electricity can be produced upon
glass and ebonite because they do not carry or conduct it away. If a
piece of iron be rubbed, the electricity passes from the iron into the
earth as fast as it is generated, because the iron is a _conductor_ of
electricity. Glass is an _insulator_ or _non-conductor_. Frictional
electricity resides upon the outside, only, of conductors. A hollow
tin box will hold as great a charge as a solid piece of metal having
the same outside size and shape. When frictional electricity passes
from one place to another, sparks are produced. Lightning is caused
by the passage of static electricity from a cloud to the earth, or
from one cloud to another. In this case air forms the conductor. (For
experiments, see "Study," Chapter VII.)
[Illustration: Fig. 3.]
=5. Electroscopes.= A piece of carbon, pith, or even a small piece of
damp tissue-paper will serve as an electroscope to test the presence of
static electricity. The pith is usually tied to a piece of silk thread
which is a non-conductor. Fig. 3 shows the ordinary form of _pith-ball
electroscope_.
The _leaf electroscope_ is a very delicate apparatus. Gold-leaf is
generally used, but aluminum-leaf will stand handling and will do for
all ordinary purposes. Fig. 4 shows a common form, the glass being
used to keep currents of air from the leaves and at the same time to
insulate them from the earth.
Electroscopes are used to show the presence, relative amount, or kind
of static electricity on a body. (See "Study," Chapter XI.)
[Illustration: Fig. 4.]
=6. Two Kinds of Electrification.= It can be shown that the
electrification produced on all bodies by friction is not the same;
for example, that generated with glass and silk is not the same as
that made with ebonite and flannel. It has been agreed to call that
produced by glass and silk _positive_, and that by ebonite and flannel
_negative_. The signs + and - are used for positive and negative.
=7. Laws of Electrification.= (1) Charges of the same kind repel each
other; (2) charges of unlike kinds attract each other; (3) either kind
of a charge attracts and is attracted by a neutral body.
=8. Static Electric Machines.= In order to produce static electricity
in quantities for experiments, some device is necessary.
The _electrophorus_ (e-lec-troph´-o-rus) is about the simplest form
of machine. Fig. 5 shows a simple electrophorus in which are two
insulators and one conductor. The ebonite sheet E S is used with a
flannel cloth to generate the electricity. The metal cover E C is
lifted by the insulating handle E R. The cover E C is placed upon the
thoroughly charged sheet E S, and then it is touched for an instant
with the finger, before lifting it by E R. The charge upon E C can then
be removed by bringing the hand near it. The bright spark that passes
from E C to the hand indicates that E C has discharged itself into the
earth. The action of the electrophorus depends upon induction. (For
experiments, details of action, induced electrification, etc., see "The
Study of Elementary Electricity and Magnetism by Experiment," Chapters
VIII. and IX.)
[Illustration: Fig. 5.]
_The first electric machine_ consisted of a ball of sulphur fastened to
a spindle which could be turned by a crank. By holding the hands or a
pad of silk upon the revolving ball, electricity was produced.
[Illustration: Fig. 6.]
[Illustration: Fig. 7.]
=9. The Cylinder Electric Machine= consists, as shown in Fig. 6, of a
glass cylinder so mounted that it can be turned by a crank. Friction
is produced by a pad of leather C, which presses against the cylinder
as it turns. Electric sparks can be taken from the large "conductors"
which are insulated from the earth. The opposite electricities unite
with sparks across D and E. If use is to be made of the electricity,
either the rubber or the prime conductor must be connected with the
ground. In the former case positive electricity is obtained; in the
latter, negative.
=10. The Plate Electrical Machine.= Fig. 7 also shows an old form of
machine. Such machines are made of circular plates of glass or ebonite,
two rubbing pads being usually employed, one on each side of the plate.
One operator is seen on an insulated stool (Fig. 7), the electricity
passing through him before entering the earth by way of the body of the
man at the right.
[Illustration: Fig. 8.]
=11. The Toepler-Holtz Machine=, in one form, is shown in Fig. 8. The
electricity is produced by the principle of induction, and not by mere
friction. This machine, used in connection with condensers, produces
large sparks.
=12. The Wimshurst Machine= is of recent date, and not being easily
affected by atmospheric changes, is very useful for ordinary laboratory
work. Fig. 9 shows one form of this machine.
=13. Influence Machines for Medical Purposes= are made in a large
variety of forms. A Wimshurst machine is generally used as an exciter
to charge the plates of the large machine when they lose their charge
on account of excessive moisture in the atmosphere. Fig. 10 shows a
large machine.
[Illustration: Fig. 9.]
=14. Uses of Electrical Machines.= Static electricity has been used for
many years in the laboratory for experimental purposes, for charging
condensers, for medical purposes, etc. It is now being used for X-ray
work, and considerable advancement has been made within a few years in
the construction and efficiency of the machines.
[Illustration: Fig. 10.]
With the modern machines large sparks are produced by merely turning
a crank, enough electricity being produced to imitate a small
thunderstorm. The sparks of home-made lightning will jump several
inches.
Do not think that electricity is generated in a commercial way by
static electric machines. The practical uses of static electricity are
very few when compared with those of current electricity from batteries
and dynamos.
=15. Condensation of Static Electricity.= By means of apparatus called
_condensers_, a terrific charge of static electricity may be stored.
Fig. 11 shows the most common form of condenser, known as the _Leyden
jar_. It consists of a glass jar with an inside and outside coating of
tin-foil.
[Illustration: Fig. 11.]
[Illustration: Fig. 12.]
_To charge_ the jar it is held in the hand so that the outside coating
shall be connected with the earth, the sparks from an electric machine
being passed to the knob at the top, which is connected by a chain to
the inside coating.
_To discharge_ the jar, Fig. 12, a conductor with an insulating handle
is placed against the outside coat; when the other end of the conductor
is swung over towards the knob, a bright spark passes between them.
This device is called a discharger. Fig. 13 shows a discharge through
ether which the spark ignites.
[Illustration: Fig. 13.]
=16. The Leyden Battery=, Fig. 14, consists of several jars connected
in such a way that the area of the inner and outer coatings is greatly
increased. The battery has a larger capacity than one of its jars. (For
Experiments in Condensation, see "Study," Chapter X.)
[Illustration: Fig. 14.]
=17. Electromotive Force of Static Electricity.= Although the sparks
of static electricity are large, the _quantity_ of electricity is very
small. It would take thousands of galvanic cells to produce a spark
an inch long. While the quantity of static electricity is small, its
potential, or electromotive force (E. M. F.), is very high. We say that
an ordinary gravity cell has an E. M. F. of a little over one volt.
Five such cells joined in the proper way would have an E. M. F. of a
little over five volts. You will understand, then, what is meant when
we say that the E. M. F. of a lightning flash is millions of volts.
=18. Atmospheric Electricity.= The air is usually electrified, even
in clear weather, although its cause is not thoroughly understood. In
1752 it was proved by Benjamin Franklin (Fig. 15), with his famous
kite experiment, that atmospheric and frictional electricities are
of the same nature. By means of a kite, the string being wet by the
rain, he succeeded, during a thunderstorm, in drawing sparks, charging
condensers, etc.
[Illustration: Fig. 15.]
[Illustration: Fig. 16.]
=19. Lightning= may be produced by the passage of electricity between
clouds, or between a cloud and the earth (Fig. 16), which, with the
intervening air, have the effect of a condenser. When the attraction
between the two electrifications gets great enough, a spark passes.
When the spark has a zigzag motion it is called _chain lightning_.
In hot weather flashes are often seen which light whole clouds, no
thunder being heard. This is called _heat lightning_, and is generally
considered to be due to distant discharges, the light of which is
reflected by the clouds. The lightning flash represents billions of
volts.
[Illustration: Fig. 17.]
=20. Thunder= is caused by the violent disturbances produced in the
air by lightning. Clouds, hills, etc., produce echoes, which, with the
original sound, make the rolling effect.
=21. Lightning-Rods=, when well constructed, often prevent violent
discharges. Their pointed prongs at the top allow the negative
electricity of the earth to pass quietly into the air to neutralize
the positive in the cloud above. In case of a discharge, or stroke of
lightning, the rods aid in conducting the electricity to the earth. The
ends of the rods are placed deep in the earth, Fig. 17.
=22. St. Elmo's Fire.= Electrification from the earth is often drawn up
from the earth through the masts of ships, Fig. 18, to neutralize that
in the clouds, and, as it escapes from the points of the masts, light
is produced.
[Illustration: Fig. 18.]
=23. Aurora Borealis=, also called Northern Lights, are luminous
effects, Fig. 19, often seen in the north. They often occur at the
same time with magnetic storms, when telegraph and telephone work may
be disturbed. The exact cause of this light is not known, but it is
thought by many to be due to disturbances in the earth's magnetism
caused by the action of the sun.
[Illustration: Fig. 19.]
CHAPTER II.
ABOUT MAGNETS AND MAGNETISM.
=24. Natural Magnets.= Hundreds of years ago it was discovered that
a certain ore of iron, called lodestone, had the power of picking up
small pieces of iron. It was used to indicate the north and south
line, and it was discovered later that small pieces of steel could be
permanently magnetized by rubbing them upon the lodestone.
=25. Artificial Magnets.= Pieces of steel, when magnetized, are called
artificial magnets. They are made in many forms. The electromagnet is
also an artificial magnet; this will be treated separately.
[Illustration: Fig. 20]
=26. The Horseshoe Magnet=, Fig. 20, is, however, the one with which we
are the most familiar. They are always painted red, but the red paint
has nothing to do with the magnetism.
The little end-piece is called the keeper, or armature; it should
always be kept in place when the magnet is not in use. The magnet
itself is made of steel, while the armature is made of soft iron. Steel
retains magnetism for a long time, while soft iron loses it almost
instantly. The ends of the magnet are called its _poles_, and nearly
all the strength of the magnet seems to reside at the poles, the curved
part having no attraction for outside bodies. One of the poles of the
magnet is marked with a line, or with the letter N. This is called the
north pole of the magnet, the other being its south pole.
[Illustration: Fig. 21.]
=27. Bar Magnets= are straight magnets. Fig. 21 shows a round bar
magnet. The screw in the end is for use in the telephone, described
later.
=28. Compound Magnets.= When several thin steel magnets are riveted
together, a compound magnet is formed. These can be made with
considerable strength. Fig. 22 shows a compound horseshoe magnet. Fig.
23 shows a form of compound bar magnet used in telephones. The use of
the coil of wire will be explained later. A thick piece of steel can
not be magnetized through and through. In the compound magnet we have
the effect of a thick magnet practically magnetized through and through.
[Illustration: Fig. 22.]
[Illustration: Fig. 23.]
=29. Magnetic and Diamagnetic Bodies.= Iron, and substances containing
iron, are the ones most readily attracted by a magnet. Iron is said to
be _magnetic_. Some substances, like nickel, for example, are visibly
attracted by very strong magnets only. Strange as it may seem, some
substances are actually repelled by strong magnets; these are called
_diamagnetic_ bodies. Brass, copper, zinc, etc., are not visibly
affected by a magnet. Magnetism will act through paper, glass, copper,
lead, etc.
[Illustration: Fig. 24.]
=30. Making Magnets.= One of the strangest properties that a magnet
has is its power to give magnetism to another piece of steel. If
a sewing-needle be properly rubbed upon one of the poles of a
magnet, it will become strongly magnetized and will retain its
magnetism for years. Strong permanent magnets are made with the aid
of electromagnets. Any number of little magnets may be made from a
horseshoe magnet without injuring it.
[Illustration: Fig. 25.]
31. Magnetic Needles and Compasses. If a bar magnet be suspended
by a string, or floated upon a cork, which can easily be done with
the magnet made from a sewing-needle, Fig. 24, it will swing around
until its poles point north and south. Such an arrangement is called
a _magnetic needle_. In the regular _compass_, a magnetic needle is
supported upon a pivot. Compasses have been used for many centuries
by mariners and others. Fig. 25 shows an ordinary pocket compass, and
Fig. 26 a form of mariner's compass, in which the small bar magnets are
fastened to a card which floats, the whole being so mounted that it
keeps a horizontal position, even though the vessel rocks.
[Illustration: Fig. 26.]
32. Action of Magnets Upon Each Other. By making two small
sewing-needle magnets, you can easily study the laws of attraction and
repulsion. By bringing the two north poles, or the two south poles,
near each other, a repulsion will be noticed. Unlike poles attract each
other. The attraction between a magnet and iron is mutual; that is,
each attracts the other. Either pole of a magnet attracts soft iron.
In magnetizing a needle, either end may be made a north pole at will;
in fact, the poles of a weak magnet can easily be reversed by properly
rubbing it upon a stronger magnet.
=33. Theory of Magnetism.= Each little particle of a piece of steel or
iron is supposed to be a magnet, even before it touches a magnet. When
these little magnets are thoroughly mixed up in the steel, they pull in
all sorts of directions upon each other and tend to keep the steel from
attracting outside bodies. When a magnet is properly rubbed upon a bar
of steel, the north poles of the little molecular magnets of the steel
are all made to point in the same direction. As the north poles help
each other, the whole bar can attract outside bodies.
By jarring a magnet its molecules are thoroughly shaken up; in fact,
most of the magnetism can be knocked out of a weak magnet by hammering
it.
=34. Retentivity.= The power that a piece of steel has to hold
magnetism is called _retentivity_. Different kinds of steel have
different retentivities. A sewing-needle of good steel will retain
magnetism for years, and it is almost impossible to knock the magnetism
out by hammering it. Soft steel has very little retentivity, because
it does not contain much carbon. Soft iron, which contains less
carbon than steel, holds magnetism very poorly; so it is not used for
permanent magnets. A little magnetism, however, will remain in the
soft iron after it is removed from a magnet. This is called _residual
magnetism_.
=35. Heat and Magnetism.= Steel will completely lose its magnetism
when heated to redness, and a magnet will not attract red-hot iron.
The molecules of a piece of red-hot iron are in such a state of rapid
vibration that they refuse to be brought into line by the magnet.
=36. Induced Magnetism.= A piece of soft iron may be induced to become
a magnet by holding it near a magnet, absolute contact not being
necessary. When the soft iron is removed, again, from the influence of
the magnet, its magnetism nearly all disappears. It is said to have
_temporary_ magnetism; it had _induced_ magnetism. If a piece of soft
iron be held near the north pole of a magnet, as in Fig. 27, poles will
be produced in the soft iron, the one nearest the magnet being the
south pole, and the other the north pole.
[Illustration: Fig. 27.]
[Illustration: Fig. 28.]
=37. Magnetic Field.= If a bar magnet be laid upon the table, and a
compass be moved about it, the compass-needle will be attracted by the
magnet, and it will point in a different direction for every position
given to the compass. This strange power, called magnetism, reaches out
on all sides of a magnet. The magnet may be said to act by induction
upon the compass-needle. The space around the magnet, in which this
inductive action takes place, is called the _magnetic field_. Fig. 28
shows some of the positions taken by a compass-needle when moved about
on one side of a bar magnet.
[Illustration: Fig. 29.]
[Illustration: Fig. 30.]
=38. Magnetic Figures= can be made by sprinkling iron filings upon a
sheet of paper under which is placed a magnet. Fig. 29 shows a magnetic
figure made with an ordinary bar magnet. The magnet was placed upon the
table and over this was laid a piece of smooth paper. Fine iron filings
were sifted upon the paper, which was gently tapped so that the filings
could arrange themselves. As each particle of iron became a little
magnet, by induction, its poles were attracted and repelled by the
magnet; and when the paper was tapped they swung around to their final
positions. Notice that the filings have arranged themselves in lines.
These lines show the positions of some of the _lines of magnetic force_
which surrounded the magnet.
These lines of force pass from the north pole of a magnet through the
air on all sides to its south pole.
[Illustration: Fig. 31.]
Fig. 30 shows a magnetic figure made from two bar magnets placed side
by side, their unlike poles being next to each other. Fig. 31 shows
the magnetic figure of a horseshoe magnet with round poles, the poles
being uppermost.
=39. The Use of Armatures.= A magnet attracts iron most strongly at its
poles, because it is at the poles that the greatest number of lines
of force pass into the air. Lines of force pass easily through soft
iron, which is said to be a good conductor of them. Air is not a good
conductor of the lines of force; in order, then, for the lines of force
to pass from the north pole of a magnet to its south pole, they must
overcome this resistance of the air, unless the armature is in place. A
magnet will gradually grow weaker when its armature is left off.
=40. Terrestrial Magnetism.= As the compass-needle points to the north
and south, the earth must act like a magnet. There is a place very far
north, about a thousand miles from the north pole of the earth, which
is called the earth's north magnetic pole. Compass-needles point to
this place, and not to the earth's real north pole. You can see, then,
that if a compass be taken north of this magnetic pole, its north pole
will point south. Lines of force pass from the earth's north magnetic
pole through the air on all sides of the earth and enter the earth's
south magnetic pole. The compass-needle, in pointing toward the north
magnetic pole, merely takes the direction of the earth's lines of
force, just as the particles of iron filings arrange themselves in the
magnetic figures.
=41. Declination.= As the magnetic needle does not point exactly to the
north, an angle is formed between the true north and south line and the
line of the needle. In Fig. 32 the line marked N S is the true north
and south line. The _angle of variation_, or the declination, is the
angle A between the line N S and the compass-needle.
[Illustration: Fig. 32.]
[Illustration: Fig. 33.]
=42. Dip or Inclination.= If a piece of steel be carefully balanced
upon a support, and then magnetized, it will be found that it will no
longer balance. The north pole will _dip_ or point downward. Fig. 33
shows what happens to a needle when it is held in different positions
over a bar magnet. It simply takes the directions of the lines of
force as they pass from the north to the south pole of the magnet.
As the earth's lines of force pass in curves from the north to the
south magnetic pole, you can see why the magnetic needle dips, unless
its south pole is made heavier than its north. Magnetic needles are
balanced after they are magnetized.
[Illustration: Fig. 34.]
Fig. 34 shows a simple form of dipping needle. These are often used
by geologists and miners. In the hands of the prospector, the
miner's compass, or dipping needle, proves a serviceable guide to the
discovery and location of magnetic iron ore. In this instrument the
magnetic needle is carefully balanced upon a horizontal axis within a
graduated circle, and in which the needle will be found to assume a
position inclined to the horizon. This angle of deviation is called the
_inclination_ or _dip_, and varies in different latitudes, and even at
different times in the same place.
=43. The Earth's Inductive Influence.= The earth's magnetism acts
inductively upon pieces of steel or iron upon its surface. If a piece
of steel or iron, like a stove poker, for example, be held in a north
and south line with its north end dipping considerably, it will be
in the best position for the magnetism of the earth to act upon it;
that is, it will lie in the direction taken by the earth's lines of
force. If the poker be struck two or three times with a hammer to
shake up its molecules, we shall find, upon testing it, that it has
become magnetized. By this method we can pound magnetism right out of
the air with a hammer. If the magnetized poker be held level, in an
east and west direction, it will no longer be acted upon to advantage
by the inductive influence of the earth, and we can easily hammer the
magnetism out of it again. (For experiments on magnets and magnetism
see "Study," Part I.)
CHAPTER III.
HOW ELECTRICITY IS GENERATED BY THE VOLTAIC CELL.
=44. Early Experiments.= In 1786 Galvani, an Italian physician, made
experiments to study the effect of static electricity upon the nervous
excitability of animals, and especially upon the frog. He found that
electric machines were not necessary to produce muscular contractions
or kicks of the frog's legs, and that they could be produced when two
different metals, Fig. 35, like iron and copper, for example, were
placed in proper contact with a nerve and a muscle and then made to
touch each other. Galvani first thought that the frog generated the
electricity instead of the metals.
[Illustration: Fig. 35.]
Volta proved that the electricity was caused by the contact of the
metals. He used the condensing electroscope as one means of proving
that two dissimilar metals become charged differently when in contact.
Volta also carried out his belief by constructing what is called a
_Voltaic Pile_. He thought that by making several pairs of metals so
arranged that all the little currents would help each other, a strong
current could be generated. Fig. 36 shows a _pile_, it being made by
placing a pair of zinc and copper discs in contact with one another,
then laying on the copper disc a piece of flannel soaked in brine, then
on top of this another pair, etc., etc. By connecting the first zinc
and the last copper, quite a little current was produced. This was a
start from which has been built our present knowledge of electricity.
Strictly speaking, electricity is not generated by combinations of
metals or by cells; they really keep up a difference of potential, as
will be seen.
[Illustration: Fig. 36.]
[Illustration: Fig. 37.]
[Illustration: Fig. 38.]
=45. The Simple Cell.= It has been stated that two different kinds of
electrifications may be produced by friction; one positive, the other
negative. Either can be produced, at will, by using proper materials.
Fig. 37 shows a section of a _simple cell_; Fig. 38 shows another view.
Cu is a piece of copper, and Zn a piece of zinc. When they are placed
in dilute sulphuric acid, it can be shown by delicate apparatus that
they become charged differently, because the acid acts differently
upon the plates. They become charged by chemical action, and not by
friction. The zinc is gradually dissolved, and it is this chemical
burning of the zinc that furnishes energy for the electric current in
the simple cell. The electrification, or charge, on the plates tends to
flow from the place of higher to the place of lower potential, just as
water tends to flow down hill. If a wire be joined to the two metals, a
constant current of electricity will flow through it, because the acid
continues to act upon the plates. The simple cell is a _single-fluid_
cell, as but one liquid is used in its construction.
=45a. Plates and Poles.= The metal strips used in voltaic cells are
called _plates_ or _elements_. The one most acted upon by the acid
is called the positive (+) plate. In the simple cell the zinc is the
+ plate, and the copper the negative (-) plate. The end of a wire
attached to the - plate is called the + pole, or electrode. Fig. 37
shows the negative (-) electrode as the end of the wire attached to the
+ plate.
=46. Direction of Current.= In the cell the current passes from the
zinc to the copper; that is, from the positive to the negative plate,
where bubbles of hydrogen gas are deposited. In the wire connecting the
plates, the current passes from the copper to the zinc plate. In most
cells, carbon takes the place of copper. (See "Study," § 268.)
=47. Local Currents; Amalgamation.= Ordinary zinc contains impurities
such as carbon, iron, etc., and when the acid comes in contact with
these, they form with the zinc a small cell. This tends to eat away the
zinc without producing useful currents. The little currents in the cell
from this cause are called _local currents_. (See "Study," Exp. 111, §
273.) This is largely overcome by coating the zinc with mercury. This
process is called _amalgamation_. It makes the zinc act like pure zinc,
which is not acted upon by dilute sulphuric acid when the current does
not pass. (See "Study," § 257, 274.)
=48. Polarization of Cells.= Bubbles of hydrogen gas are formed when
zinc is dissolved by an acid. In the ordinary simple cell these bubbles
collect on the copper plate, and not on the zinc plate, as might be
expected. The hydrogen is not a conductor of electricity, so this film
of gas holds the current back. The hydrogen acts like a metal and sets
up a current that opposes the zinc to the copper current. Several
methods are employed to get rid of the hydrogen. (See "Study," § 278,
279, 280.)
CHAPTER IV.
VARIOUS VOLTAIC CELLS.
=49. Single-Fluid and Two-Fluid Cells.= The simple cell (§ 45) is a
single-fluid cell. The liquid is called the _electrolyte_, and this
must act upon one of the plates; that is, chemical action must take
place in order to produce a current. The simple cell polarizes rapidly,
so something must be used with the dilute sulphuric acid to destroy the
hydrogen bubbles. This is done in the _bichromate of potash cell_.
In order to get complete depolarization--that is, to keep the carbon
plate almost perfectly free from hydrogen, it is necessary to use
_two-fluid cells_, or those to which some solid depolarizer is added to
the one fluid.
=50. Open and Closed Circuit Cells.= If we consider a voltaic cell, the
wires attached to it, and perhaps some instrument through which the
current passes, we have an _electric circuit_. When the current passes,
the circuit is _closed_, but when the wire is cut, or in any way
disconnected so that the current can not pass, the circuit is _open_ or
_broken_. (See "Study," § 266.)
_Open Circuit Cells_ are those which can give momentary currents at
intervals, such as are needed for bells, telephones, etc. These must
have plenty of time to rest, as they polarize when the circuit is
closed for a long time. The _Leclanché_ and _dry_ cells are the most
common open circuit cells.
_Closed Circuit Cells._ For telegraph lines, motors, etc., where a
current is needed for some time, the cell must be of such a nature
that it will not polarize quickly; it must give a strong and constant
current. The _bichromate_ and _gravity cells_ are examples of this
variety. (See "Study," § 286.)
=51. Bichromate of Potash Cells= are very useful for general laboratory
work. They are especially useful for operating induction coils, small
motors, small incandescent lamps, for heating platinum wires, etc.
These cells have an E.M.F. of about 2 volts. Dilute sulphuric acid is
used as the exciting fluid, and in this is dissolved the bichromate of
potash which keeps the hydrogen bubbles from the carbon plate. (See
"Apparatus Book," § 26.) Zinc and carbon are used for the plates, the +
pole being the wire attached to the carbon.
[Illustration: Fig. 39.]
Fig. 39 shows one form of bichromate cell. It furnishes a large
quantity of current, and as the zinc can be raised from the fluid, it
may be kept charged ready for use for many months, and can be set in
action any time when required by lowering the zinc into the liquid. Two
of these cells will burn a one candle-power miniature incandescent lamp
several hours. The carbon is indestructible.
=Note.= For various forms of home-made cells, see "Apparatus
Book," Chapter I., and for battery fluids see Chapter II.
=52. The Grenet Cell.= Fig. 40 is another form of bichromate cell. The
carbon plates are left in the fluid constantly. The zinc plate should
be raised when the cell is not in use, to keep it from being uselessly
dissolved.
[Illustration: Fig. 40.]
[Illustration: Fig. 41.]
=53. Plunge Batteries.= Two or more cells are often arranged so that
their elements can be quickly lowered into the acid solution. Such a
combination, Fig. 41, is called a _plunge battery_. The binding-posts
are so arranged that currents of different strengths can be taken from
the combination. The two binding-posts on the right of the battery
will give the current of one cell; the two binding-posts on the left
of the battery will give the current of two cells, and the two end
binding-posts will give the current of all three cells. When not in
use the elements must always be hung on the hooks and kept out of the
solution.
=54. Large Plunge Batteries=. Fig. 42, are arranged with a winch and
a bar above the cells; these afford a ready and convenient means of
lifting or lowering the elements and avoiding waste. In the battery
shown, Fig. 42, the zincs are 4×6 inches; the carbons have the same
dimensions, but there are two carbon plates to each zinc, thus giving
double the carbon surface.
[Illustration: Fig. 42.]
=55. The Fuller Cell=, Fig. 43, is another type of bichromate cell,
used largely for long-distance telephone service, for telephone
exchange and switch service, for running small motors, etc. It consists
of a glass jar, a carbon plate, with proper connections, a clay porous
cup, containing the zinc, which is made in the form of a cone. A little
mercury is placed in the porous cup to keep the zinc well amalgamated.
Either bichromate of potash or bichromate of soda can be used as a
depolarizer.
[Illustration: Fig. 43.]
[Illustration: Fig. 44.]
=56. The Gravity Cell=, sometimes called the _bluestone_ or _crowfoot_
cell, is used largely for telegraph, police, and fire-alarm signal
service, laboratory and experimental work, or whenever a closed circuit
cell is required. The E.M.F. is about one volt. This is a modified form
of the Daniell cell. Fig. 44 shows a home-made gravity cell.
A copper plate is placed at the bottom of the glass jar, and upon
this rests a solution of copper sulphate (bluestone). The zinc plate
is supported about four inches above the copper, and is surrounded
by a solution of zinc sulphate which floats upon the top of the blue
solution. An insulated wire reaches from the copper to the top of the
cell and forms the positive pole. (See "Apparatus Book," § 11 to 15,
for home-made gravity cell, its regulation, etc. For experiments with
two-fluid Daniell cell, see "Study," Exp. 113, § 281 to 286.)
[Illustration: Fig. 45.]
=56a. Bunsen Cells,= Fig. 45, are used for motors, small incandescent
lamps, etc. A carbon rod is inclosed in a porous cup, on the outside of
which is a cylinder of zinc that stands in dilute sulphuric acid, the
carbon being in nitric acid.
=57. The Leclanché Cell= is an open circuit cell. Sal ammoniac is used
as the exciting fluid, carbon and zinc being used for plates. Manganese
dioxide is used as the depolarizer; this surrounds the carbon plate,
the two being either packed together in a porous cup or held together
in the form of cakes. The porous cup, or pressed cake, stands in the
exciting fluid. The E. M. F. is about 1.5 volts.
[Illustration: Fig. 46.]
[Illustration: Fig. 47.]
[Illustration: Fig. 48.]
[Illustration: Fig. 49.]
Fig. 46 shows a form with porous cup. The binding-post at the top of
the carbon plate forms the + electrode, the current leaving the cell at
this point.
_The Gonda Prism Cell_ (Fig. 47), is a form of Leclanché in which the
depolarizer is in the form of a cake.
=58. Dry Cells= are open circuit cells, and can be carried about,
although they are moist inside. The + pole is the end of the carbon
plate. Zinc is used as the outside case and + plate. Fig. 48 shows the
ordinary forms.
Fig. 49 shows a number of dry cells arranged in a box with switch in
front, so that the current can be regulated at will.
[Illustration: Fig. 50.]
=59. The Edison-Lelande Cells=, Fig. 50, are made in several sizes and
types. Zinc and copper oxide, which is pressed into plates, form the
elements. The exciting fluid consists of a 25 per cent. solution of
caustic potash in water. They are designed for both open and closed
circuit work.
CHAPTER V.
ABOUT PUSH-BUTTONS, SWITCHES AND BINDING-POSTS.
=60. Electrical Connections.= In experimental work, as well as in
the everyday work of the electrician, electrical connections must
constantly be made. One wire must be joined to another, just for a
moment, perhaps, or one piece of apparatus must be put in an electric
circuit with other apparatus, or the current must be turned on or off
from motors, lamps, etc. In order to conveniently and quickly make such
connections, apparatus called push-buttons, switches and binding-posts
are used.
[Illustration: Fig. 51.]
[Illustration: Fig. 52.]
=61. Push-Buttons.= The simple act of pressing your finger upon a
movable button, or knob, may ring a bell a mile away, or do some other
equally wonderful thing. Fig. 51 shows a simple push-button, somewhat
like a simple key in construction. If we cut a wire, through which a
current is passing, then join one of the free ends to the screw A and
the other end to screw C, we shall be able to let the current pass at
any instant by pressing the spring B firmly upon A.
Push-buttons are made in all sorts of shapes and sizes. Fig. 52 gives
an idea of the general internal construction. The current enters A by
one wire, and leaves by another wire as soon as the button is pushed
and B is forced down to A. The bottom of the little button rests upon
the top of B.
Fig. 53 shows a _Table Clamp-Push_ for use on dining-tables,
card-tables, chairs, desks, and other movable furniture. Fig. 54 shows
a combination of push-button, speaking-tube, and letter-box used in
city apartment houses. Fig. 55 shows an _Indicating Push_. The buzzer
indicates, by the sound, whether the call has been heard; that is, the
person called answers back.
[Illustration: Fig. 53.]
[Illustration: Fig. 54.]
_Modifications_ of ordinary push-buttons are used for floor
push-buttons, on doors, windows, etc., for burglar-alarms, for turning
off or on lights, etc., etc. (See "Apparatus Book," Chapter III., for
home-made push-buttons.)
[Illustration: Fig. 55.]
=62. Switches= have a movable bar or plug of metal, moving on a pivot,
to make or break a circuit, or transfer a current from one conductor to
another.
Fig. 56 shows a _single point switch_. The current entering the pivoted
arm can go no farther when the switch is open, as shown. To close
the circuit, the arm is pushed over until it presses down upon the
contact-point. For neatness, both wires are joined to the under side of
the switch or to binding-posts.
[Illustration: Fig. 56.]
Fig. 57 shows a _knife switch_. Copper blades are pressed down between
copper spring clips to close the circuit. The handle is made of
insulating material.
_Pole-changing switches_, Fig. 58, are used for changing or reversing
the poles of batteries, etc.
Fig. 59 shows a home-made switch, useful in connection with resistance
coils. By joining the ends of the coils A, B, C, D, with the
contact-points 1, 2, 3, etc., more or less resistance can be easily
thrown in by simply swinging the lever E around to the left or right.
If E be turned to 1, the current will be obliged to pass through all
the coils A, B, etc., before it can pass out at Y. If E be moved to
3, coils A and B will be cut out of the circuit, thus decreasing the
resistance to the current on its way from X to Y. Current regulators
are made upon this principle. (See "Apparatus Book," Chapter IV., for
home-made switches.)
[Illustration: Fig. 57.]
[Illustration: Fig. 58.]
[Illustration: Fig. 59.]
_Switchboards_ are made containing from two or three to hundreds of
switches, and are used in telegraph and telephone work, in electric
light stations, etc., etc. (See Chapter on Central Stations.) Fig. 60
shows a switch used for incandescent lighting currents.
[Illustration: Fig. 60.]
[Illustration: Fig. 61.]
=63. Binding-Posts= are used to make connections between two pieces of
apparatus, between two or more wires, between a wire and any apparatus,
etc., etc. They allow the wires to be quickly fastened or unfastened
to the apparatus. A large part of the apparatus shown in this book has
binding-posts attached. Fig. 61 shows a few of the common forms used.
(See "Apparatus Book," Chapter V., for home-made binding-posts.)
CHAPTER VI.
UNITS AND APPARATUS FOR ELECTRICAL MEASUREMENTS.
=64. Electrical Units.= In order to measure electricity for
experimental or commercial purposes, standards or units are just as
necessary as the inch or foot for measuring distances.
=65. Potential; Electromotive Force.= If water in a tall tank be
allowed to squirt from two holes, one near the bottom, the other near
the top, it is evident that the force of the water that comes from the
hole at the bottom will be the greater. The pressure at the bottom is
greater than that near the top, because the "head" is greater.
When a spark of static electricity jumps a long distance, we say that
the charge has a high _potential_; that is, it has a high electrical
pressure. Potential, for electricity, means the same as pressure, for
water. The greater the potential, or _electromotive force_ (E.M.F.) of
a cell, the greater its power to push a current through wires. (See
"Study," § 296 to 305, with experiments.)
=66. Unit of E.M.F.; the Volt.=--In speaking of water, we say that its
pressure is so many pounds to the square inch, or that it has a fall,
or head, of so many feet. We speak of a current as having so many
volts; for example, we say that a wire is carrying a 110-volt current.
The volt is the unit of E.M.F. An ordinary gravity cell has an E.M.F.
of about one volt. This name was given in honor of Volta.
=67. Measurement of Electromotive Force.= There are several ways by
which the E.M.F. of a cell, for example, can be measured. It is usually
measured _relatively_, by comparison with the E. M. F. of some standard
cell. (See "Study," Exp. 140, for measuring the E. M. F. of a cell by
comparison with the two-fluid cell.)
[Illustration: Fig. 62.]
_Voltmeters_ are instruments by means of which E. M. F. can be read on
a printed scale. They are a variety of galvanometer, and are made with
coils of such high resistance, compared with the resistance of a cell
or dynamo, that the E. M. F. can be read direct. The reason for this
will be seen by referring to Ohm's law ("Study," § 356); the resistance
is so great that the strength of the current depends entirely upon the
E. M. F.
[Illustration: Fig. 63.]
Voltmeters measure electrical pressure just as steam gauges measure
the pressure of steam. Fig. 62 shows one form of voltmeter. Fig. 63
shows a voltmeter with illuminated dial. An electrical bulb behind the
instrument furnishes light so that the readings can be easily taken.
=68. Electrical Resistance.= Did you ever ride down hill on a
hand-sled? How easily the sled glides over the snow! What happens,
though, when you strike a bare place, or a place where some evil-minded
person has sprinkled ashes? Does the sled pass easily over bare ground
or ashes? Snow offers very little _resistance_ to the sled, while ashes
offer a great resistance.
[Illustration: Fig. 64.]
All substances do not allow the electric current to pass through
them with the same ease. Even the liquid in a cell tends to hold the
current back and offers _internal resistance_. The various wires and
instruments connected to a cell offer _external resistance_. (See
"Study," Chapter XVIII., for experiments, etc.)
=69. Unit of Resistance.= =The Ohm= is the name given to the unit of
resistance. About 9 ft. 9 in. of No. 30 copper wire, or 39 feet 1 in.
of No. 24 copper wire, will make a fairly accurate ohm.
_Resistance coils_, having carefully measured resistances, are made
for standards. (See "Apparatus Book," Chapter XVII., for home-made
resistance coils.) Fig. 64 shows a commercial form of a standard
resistance coil. The coil is inclosed in a case and has large wires
leading from its ends for connections. Fig. 65 gives an idea of
the way in which coils are wound and used with plugs to build up
_resistance boxes_, Fig. 66.
=70. Laws of Resistance.= 1. The resistance of a wire is directly
proportional to its length, provided its cross-section, material, etc.,
are uniform.
2. The resistance of a wire is inversely proportional to its area of
cross-section; or, in other words, inversely proportional to the square
of its diameter, other things being equal.
[Illustration: Fig. 65.]
3. The resistance of a wire depends upon its material, as well as upon
its length, size, etc.
4. The resistance of a wire increases as its temperature rises. (See
"Study," Chapters XVIII. and XIX., for experiments on resistance, its
measurement, etc.)
[Illustration: Fig. 66.]
=71. Current Strength.= The strength of a current at the end of a
circuit depends not only upon the _electrical pressure_, or E. M. F.,
which drives the current, but also upon the _resistance_ which has to
be overcome. The greater the resistance the weaker the current at the
end of its journey.
=72. Unit of Current Strength; The Ampere.= A current having an E. M.
F. of _one volt_, pushing its way through a resistance of _one ohm_,
would have a unit of strength, called _one ampere_. This current, one
ampere strong, would deposit, under proper conditions, .0003277 gramme
of copper in _one second_ from a solution of copper sulphate.
=73. Measurement of Current Strength.= A magnetic needle is deflected
when a current passes around it, as in instruments like the
galvanometer. The _galvanoscope_ merely indicates the presence of a
current. _Galvanometers_ measure the strength of a current, and they
are made in many forms, depending upon the nature and strength of the
currents to be measured. Galvanometers are standardized, or calibrated,
by special measurements, or by comparison with some standard
instrument, so that when the deflection is a certain number of degrees,
the current passing through it is known to be of a certain strength.
[Illustration: Fig. 67.]
Fig. 67 shows an _astatic galvanometer_. Fig. 68 shows a _tangent
galvanometer_, in which the strength of the current is proportional
to the tangent of the angle of deflection. Fig. 69 shows a _D'Arsonval
galvanometer_, in which a coil of wire is suspended between the poles
of a permanent horseshoe magnet. The lines of force are concentrated
by the iron core of the coil. The two thin suspending wires convey the
current to the coil. A ray of light is reflected from the small mirror
and acts as a pointer as in other forms of reflecting galvanometers.
[Illustration: Fig. 68.]
=74. The Ammeter=, Fig. 70, is a form of galvanometer in which the
strength of a current, in amperes, can be read. In these the strength
of current is proportional to the angular deflections. The coils are
made with a small resistance, so that the current will not be greatly
reduced in strength in passing through them.
[Illustration: Fig. 69.]
=75. Voltameters= measure the strength of a current by chemical means,
the quantity of metal deposited or gas generated being proportional
to the time that the current flows and to its strength. In the _water
voltameter_, Fig. 71, the hydrogen and oxygen produced in a given time
are measured. (See "Study," Chapter XXI.)
[Illustration: Fig. 70.]
The _copper voltameter_ measures the amount of copper deposited in a
given time by the current. Fig. 72 shows one form. The copper cathode
is weighed before and after the current flows. The weight of copper
deposited and the time taken are used to calculate the current strength.
[Illustration: Fig. 71.]
=76. Unit of Quantity=; =The Coulomb= is the quantity of electricity
given, in _one second_, by a current having a strength of one ampere.
Time is an important element in considering the work a current can do.
[Illustration: Fig. 72.]
=77. Electrical Horse-power=; =The Watt= is the unit of electrical
power. A current having the strength of one ampere, and an E. M.
F. of one volt has a unit of power. 746 watts make one electrical
horse-power. Watts = amperes × volts. Fig. 73 shows a direct reading
wattmeter based on the international volt and ampere. They save taking
simultaneous ammeter and voltmeter readings, which are otherwise
necessary to get the product of volts and amperes, and are also used on
alternating current measurements.
[Illustration: Fig. 73.]
There are also forms of wattmeters, Fig. 74, in which the watts are
read from dials like those on an ordinary gas-meter, the records being
permanent.
Fig. 75 shows a voltmeter V, and ammeter A, so placed in the circuit
that readings can be taken. D represents a dynamo. A is placed so that
the whole current passes through it, while V is placed between the main
wires to measure the difference in potential. The product of the two
readings in volts and amperes gives the number of watts.
[Illustration: Fig. 74.]
=78. Chemical Meters= also measure the quantity of current that is
used; for example, one may be placed in the cellar to measure the
quantity of current used to light the house.
[Illustration: Fig. 75.]
Fig. 76 shows a chemical meter, a part of the current passing through
a jar containing zinc plates and a solution of zinc sulphate. Metallic
zinc is dissolved from one plate and deposited upon the other. The
increase in weight shows the amount of chemical action which is
proportional to the ampere hours. Knowing the relation between the
quantity of current that can pass through the solution to that which
can pass through the meter by another conductor, a calculation can be
made which will give the current used. A lamp is so arranged that it
automatically lights before the meter gets to the freezing-point; this
warms it up to the proper temperature, at which point the light goes
out again.
[Illustration: Fig. 76.]
CHAPTER VII.
CHEMICAL EFFECTS OF THE ELECTRIC CURRENT.
=79. Electrolysis.= It has been seen that in the voltaic cell
electricity is generated by chemical action. Sulphuric acid acts upon
zinc and dissolves it in the cell, hydrogen is produced, etc. When
this process is reversed, that is, when the electric current is passed
through some solutions, they are decomposed, or broken up into their
constituents. This process is called _electrolysis_, and the compound
decomposed is the _electrolyte_. (See "Study," § 369, etc., with
experiments.)
[Illustration: Fig. 77.]
Fig. 77 shows how water can be decomposed into its two constituents,
hydrogen and oxygen, there being twice as much hydrogen formed as
oxygen.
Fig. 78 shows a glass jar in which are placed two metal strips, A and
C, these being connected with two cells. In this jar may be placed
various conducting solutions to be tested. If, for example, we use
a solution of copper sulphate, its chemical formula being CuSO_{4},
the current will break it up into Cu (copper) and SO_{4}. The Cu will
be deposited upon C as the current passes from A to C through the
solution. A is called the _anode_, and C the _cathode_.
[Illustration: Fig. 78.]
Fig. 79 shows another form of jar used to study the decomposition of
solutions by the electric current.
[Illustration: Fig 79.]
=80. Ions.= When a solution is decomposed into parts by a current, the
parts are called the _Ions_. When copper sulphate (Cu SO_{4}) is used,
the ions are Cu, which is a metal, and SO_{4}, called an acid radical.
When silver nitrate (Ag NO_{3}) is used, Ag and NO_{3} are the ions.
The metal part of the compound goes to the cathode.
CHAPTER VIII.
HOW ELECTROPLATING AND ELECTROTYPING ARE DONE.
=81. Electricity and Chemical Action.= We have just seen, Chapter VII.,
that the electric current has the power to decompose certain compounds
when they are in solution. By choosing the right solutions, then, we
shall be able to get copper, silver, and other metals set free by
electrolysis.
=82. Electroplating= consists in coating substances with metal with
the aid of the electric current. If we wish to electroplate a piece
of metal with copper, for example, we can use the arrangement shown
in Fig. 78, in which C is the cathode plate to be covered, and A is
a copper plate. The two are in a solution of copper sulphate, and,
as explained in § 79, the solution will be decomposed. Copper will
be deposited upon C, and the SO_{4} part of the solution will go to
the anode A, which it will attack and gradually dissolve. The SO_{4},
acting upon the copper anode, makes CuSO_{4} again, and this keeps the
solution at a uniform strength. The amount of copper dissolved from the
copper anode equals, nearly, the amount deposited upon the cathode. The
metal is carried in the direction of the current.
If we wish to plate something with silver or gold, it will be necessary
to use a solution of silver or gold for the electrolyte, a plate of
metallic silver or gold being used for the anode, as the case may be.
Great care is used in cleaning substances to be plated, all dirt and
grease being carefully removed.
Fig. 80 shows a plating bath in which several articles can be plated
at the same time by hanging them upon a metal bar which really forms a
part of the cathode. If, for example, we wish to plate knives, spoons,
etc., with silver, they would be hung from the bar shown, each being a
part of the cathode. The vat would contain a solution of silver, and
from the other bar would be hung a silver plate having a surface about
equal to that of the combined knives, etc.
[Illustration: Fig. 80.]
Most metals are coated with copper before they are plated with silver
or gold. When plating is done on a large scale, a current from a dynamo
is used. For experimental purposes a Gravity cell will do very well.
(See "Study," § 374 to 380 with experiments.)
=83. Electrotyping.= It was observed by De La Rue in 1836 that in the
Daniell cell an even coating of copper was deposited upon the copper
plate. From this was developed the process of electrotyping, which
consists in making a copy in metal of a wood-cut, page of type, etc.
A mould or impression of the type or coin is first made in wax, or
other suitable material. These moulds are, of course, the reverse
of the original, and as they do not conduct electricity, have to be
coated with graphite. This thin coating lines the mould with conducting
material so that the current can get to every part of the mould.
These are then hung upon the cathode in a bath of copper sulphate
as described in § 82. The electric current which passes through the
vat deposits a thin layer of metallic copper next to the graphite.
When this copper gets thick enough, the wax is melted away from it,
leaving a thin shell of copper, the side next to the graphite being
exactly alike in shape to the type, but made of copper. These thin
copper sheets are too thin to stand the pressure necessary on printing
presses, so they are strengthened by backing them with soft metal which
fills every crevice, making solid plates about ¼ in. thick. These
plates or _electrotypes_ are used to print from, the original type
being used to set up another page.
CHAPTER IX.
THE STORAGE BATTERY, AND HOW IT WORKS.
=84. Polarization.= It has been stated that a simple cell polarizes
rapidly on account of hydrogen bubbles that form upon the copper plate.
They tend to send a current in the opposite direction to that of the
main current, which is thereby weakened.
[Illustration: Fig. 81.]
=85. Electromotive Force of Polarization.= It has been shown, Fig. 71,
that water can be decomposed by the electric current. Hydrogen and
oxygen have a strong attraction or chemical affinity for each other, or
they would not unite to form water. This attraction has to be overcome
before the water can be decomposed. As soon as the decomposing current
ceases to flow, the gases formed try to rush together again; in fact,
if the water voltameter be disconnected from the cells and connected
with a galvanoscope, the presence of a current will be shown. This
voltameter will give a current with an E. M. F. of nearly 1.5 volts; so
it is evident that we must have a current with a higher voltage than
this to decompose water. This E. M. F., due to polarization, is called
the E. M. F. of polarization.
=86. Secondary or Storage Batteries=, also called _accumulators_, do
not really store electricity. They must be charged by a current before
they can give out any electricity. Chemical changes are produced in the
storage cells by the charging current just as they are in voltameters,
electroplating solutions, etc.; so it is potential chemical energy
that is really stored. When the new products are allowed to go back to
their original state, by joining the electrodes of the charged cell, a
current is produced.
Fig. 81 shows two lead plates, A and B, immersed in dilute sulphuric
acid, and connected with two ordinary cells. A strong current will pass
through the liquid between A and B at first, but it will quickly become
weaker, as chemical changes take place in the liquid. This may be shown
by a galvanometer put in the circuit before beginning the experiment.
By disconnecting the wires from the cells and joining them to the
galvanometer, it will be shown that a current comes from the lead
plates. This arrangement may be called a simple storage cell. Regular
storage cells are charged with the current from a dynamo. (See "Study,"
Exp. 151.)
[Illustration: Fig. 82.]
The first storage cells were made of plain lead plates, rolled up in
such a way that they were close to each other, but did not touch. These
were placed in dilute sulphuric acid. They were charged in alternate
directions several times, until the lead became properly acted upon, at
which time the cell would furnish a current.
A great improvement was made in 1881, by Faure, who coated the plates
with red lead.
[Illustration: Fig. 83.]
The method now generally practiced is to cast a frame of lead, with
raised right-angled ribs on each side, thus forming little depressed
squares, or to punch a lead plate full of holes, which squares or holes
are then filled with a pasty mixture of red oxide of lead in positive
plates, and with litharge in negatives. In a form called the chloride
battery, instead of cementing lead oxide paste into or against a lead
framing in order to obtain the necessary active material, the latter is
obtained by a strictly chemical process.
Fig. 82 shows a storage cell with plates, etc., contained in a glass
jar. Fig. 83 shows a cell of 41 plates, set up in a lead-lined wood
tank. Fig. 84 shows three cells joined in series. Many storage cells
are used in central electric light stations to help the dynamos during
the "rush" hours at night. They are charged during the day when the
load on the dynamos is not heavy.
Fig. 85 shows another form of storage cell containing a number of
plates.
[Illustration: Fig. 84.]
=87. The Uses of Storage Batteries= are almost numberless. The current
can be used for nearly everything for which a constant current is
adapted, the following being some of its applications: Carriage
propulsion; electric launch propulsion; train lighting; yacht lighting;
carriage lighting; bicycle lighting; miners' lamps; dental, medical,
surgical, and laboratory work; phonographs; kinetoscopes; automaton
pianos; sewing-machine motors; fan motors; telegraph; telephone;
electric bell; electric fire-alarm; heat regulating; railroad switch
and signal apparatus.
By the installing of a storage plant many natural but small sources
of power may be utilized in furnishing light and power; sources which
otherwise are not available, because not large enough to supply maximum
demands. The force of the tides, of small water powers from irrigating
ditches, and even of the wind, come under this heading.
[Illustration: Fig. 85.]
As a regulator of pressure, in case of fluctuations in the load, the
value of a storage plant is inestimable. These fluctuations of load are
particularly noticeable in electric railway plants, where the demand is
constantly rising and falling, sometimes jumping from almost nothing to
the maximum, and _vice versa_, in a few seconds. If for no other reason
than the prevention of severe strain on the engines and generators,
caused by these fluctuations of demand, a storage plant will be
valuable.
CHAPTER X.
HOW ELECTRICITY IS GENERATED BY HEAT.
=88. Thermoelectricity= is the name given to electricity that is
generated by heat. If a strip of iron, I, be connected between two
strips of copper, C C, these being joined by a copper wire, C W, we
shall have an arrangement that will generate a current when heated at
either of the junctions between C and I. When it is heated at A the
current will flow as shown by arrows, from C to I. If we heat at B,
the current will flow in the opposite direction through the metals,
although it will still go from C to I as before. Such currents are
called _thermoelectric currents_.
[Illustration: Fig. 86.]
Different pairs of metals produce different results. Antimony and
bismuth are generally used, because the greatest effect is produced
by them. If the end of a strip of bismuth be soldered to the end of
a similar strip of antimony, and the free ends be connected to a
galvanometer of low resistance, the presence of a current will be shown
when the point of contact becomes hotter than the rest of the circuit.
The current will flow from bismuth to antimony across the joint. By
cooling the juncture below the temperature of the rest of the circuit,
a current will be produced in the opposite direction to the above. The
energy of the current is kept up by the heat absorbed, just as it is
kept up by chemical action in the voltaic cell.
=89. Peltier Effect.= If an electric current be passed through pairs of
metals, the parts at the junction become slightly warmer or cooler than
before, depending upon the direction of the current. This action is
really the reverse of that in which currents are produced by heat.
[Illustration: Fig. 87.]
=90. Thermopiles.= As the E.M.F. of the current produced by a single
pair of metals is very small, several pairs are usually joined in
series, so that the different currents will help each other by flowing
in the same direction. Such combinations are called thermoelectric
piles, or simply _thermopiles_.
Fig. 87 shows such an arrangement, in which a large number of elements
are placed in a small space. The junctures are so arranged that the
alternate ones come together at one side.
Fig. 88 shows a thermopile connected with a galvanometer. The heat of
a match, or the cold of a piece of ice, will produce a current, even if
held at some distance from the thermopile. The galvanometer should be
a short-coil astatic one. (See "Study," Chapter XXIV., for experiments
and home-made thermopile.)
[Illustration: Fig. 88.]
CHAPTER XI.
MAGNETIC EFFECTS OF THE ELECTRIC CURRENT.
=91. Electromagnetism= is the name given to magnetism that is developed
by electricity. We have seen that if a magnetic needle be placed in the
field of a magnet, its N pole will point in the direction taken by the
lines of force as they pass from the N to the S pole of the magnet.
[Illustration: Fig. 89.]
=92. Lines of Force about a Wire.= When a current passes through a
wire, the magnetic needle placed over or under it tends to take a
position at right angles to the wire. Fig. 89 shows such a wire and
needle, and how the needle is deflected; it twists right around from
its N and S position as soon as the current begins to flow. This shows
that the lines of force pass _around_ the wire and not in the direction
of its length. The needle does not swing entirely perpendicular to the
wire, that is, to the E and W line, because the earth is at the same
time pulling its N pole toward the N.
Fig. 90 shows a bent wire through which a current passes from C to Z.
If you look along the wire from C toward the points A and B, you will
see that _under_ the wire the lines of force pass to the left. Looking
along the wire from Z toward D you will see that the lines of force
pass opposite to the above, as the current comes _toward_ you. This is
learned by experiment. (See "Study," Exp. 152, § 385, etc.)
[Illustration: Fig. 90.]
[Illustration: Fig. 91.]
_Rule._ Hold the right hand with the thumb extended (Fig. 89) and with
the fingers pointing in the direction of the current, the palm being
toward the needle and on the opposite side of the wire from the needle.
The north-seeking pole will then be deflected in the direction in which
the thumb points.
=93. Current Detectors.= As there is a magnetic field about a wire when
a current passes through it, and as the magnetic needle is affected, we
have a means of detecting the presence of a current. When the current
is strong it is simply necessary to let it pass once over or under a
needle; when it is weak, the wire must pass several times above and
below the needle, Fig. 91, to give the needle motion. (See "Apparatus
Book," Chapter XIII., for home-made detectors.)
[Illustration: Fig. 92.]
=94. Astatic Needles and Detectors.= By arranging two magnetized
needles with their poles opposite each other, Fig. 92, an _astatic
needle_ is formed. The pointing-power is almost nothing, although
their magnetic fields are retained. This combination is used to detect
feeble currents. In the ordinary detector, the tendency of the needle
to point to the N and S has to be overcome by the magnetic field about
the coil before the needle can be moved; but in the _astatic detector_
and _galvanoscope_ this pointing-power is done away with. Fig. 93 shows
a simple _astatic galvanoscope_. Fig. 67 shows an astatic galvanometer
for measuring weak currents.
[Illustration: Fig. 93.]
=95. Polarity of Coils.= When a current of electricity passes through
a coil of wire, the coil acts very much like a magnet, although no
iron enters into its construction. The coil becomes magnetized by the
electric current, lines of force pass from it into the air, etc. Fig.
94 shows a coil connected to copper and zinc plates, so arranged with
cork that the whole can float in a dish of dilute sulphuric acid. The
current passes as shown by the arrows, and when the N pole of a magnet
is brought near the right-hand end, there is a repulsion, showing that
that end of the coil has a N pole.
_Rule._ When you face the right-hand end of the coil, the current is
seen to pass around it in an anti-clockwise direction; this produces a
N pole. When the current passes in a clockwise direction a S pole is
produced.
[Illustration: Fig. 94.]
=96. Electromagnets.= A coil of wire has a stronger field than a
straight wire carrying the same current, because each turn adds its
field to the fields of the other turns. By having the central part of
the coil made of iron, or by having the coil of insulated wire wound
upon an iron _core_, the strength of the magnetic field of the coil is
greatly increased.
Lines of force do not pass as readily through air as through iron;
in fact, lines of force will go out of their way to go through iron.
With a coil of wire the lines of force pass from its N pole through
the air on all sides of the coil to its S pole; they then pass through
the inside of the coil and through the air back to the N pole. When
the resistance to their passage through the coil is decreased by the
core, the magnetic field is greatly strengthened, and we have an
_electromagnet_.
The coil of wire temporarily magnetizes the iron core; it can
permanently magnetize a piece of steel used as a core. (See "Study,"
Chapter XXII., for experiments.)
[Illustration: Fig. 95.]
=97. Forms of Electromagnets.= Fig. 95 shows a _straight, or
bar electromagnet_. Fig. 96 shows a simple form of _horseshoe
electromagnet_. As this form is not easily wound, the coils are
generally wound on two separate cores which are then joined by a
_yoke_. The yoke merely takes the place of the curved part shown
in Fig. 96. In Fig. 97 is shown the ordinary form of horseshoe
electromagnet used for all sorts of electrical instruments. (See
"Apparatus Book," Chapter IX., for home-made electromagnets.)
=98. Yokes and Armatures.= In the horseshoe magnet there are two poles
to attract and two to induce. The lines of force pass through the yoke
on their way from one core to the other, instead of going through
the air. This reduces the resistance to them. If we had no yoke we
should simply have two straight electromagnets, and the resistance to
the lines of force would be so great that the total strength would
be much reduced. Yokes are made of soft iron, as well as the cores
and armature. The _armature_, as with permanent horseshoe magnets, is
strongly drawn toward the poles. As soon as the current ceases to flow,
the attraction also ceases.
[Illustration: Fig. 96.]
[Illustration: Fig. 97.]
[Illustration: Fig. 98.]
Beautiful magnetic figures can be made with horseshoe magnets. Fig. 98
shows that the coils must be joined so that the current can pass around
the cores in opposite directions to make unlike poles. (See "Study,"
Exp. 164 to 173.)
CHAPTER XII.
HOW ELECTRICITY IS GENERATED BY INDUCTION.
=99. Electromagnetic Induction.= We have seen that a magnet has the
power to act through space and induce another piece of iron or steel
to become a magnet. A charge of static electricity can induce a
charge upon another conductor. We have now to see how a _current_ of
electricity in one conductor can induce a current in another conductor,
not in any way connected with the first, and how a magnet and a coil
can generate a current.
[Illustration: Fig. 99.]
[Illustration: Fig. 100.]
=100. Current from Magnet and Coil.= If a bar magnet, Fig. 99, be
suddenly thrust into a hollow coil of wire, a momentary current of
electricity will be generated in the coil. No current passes when the
magnet and coil are still; at least one of them must be in motion. Such
a current is said to be _induced_, and is an _inverse_ one when the
magnet is inserted, and a _direct_ one when the magnet is withdrawn
from the coil.
=101. Induced Currents and Lines of Force.= Permanent magnets are
constantly sending out thousands of lines of force. Fig. 100 shows
a bar magnet entering a coil of wire; the number of lines of force
is increasing, and the induced current passes in an anti-clockwise
direction when looking down into the coil along the lines of force.
This produces an indirect current. If an iron core be used in the coil,
the induced current will be greatly strengthened.
[Illustration: Fig. 101.]
It takes force to move a magnet through the center of a coil, and it
is this work that is the source of the induced current. We have, in
this simple experiment, the key to the action of the dynamo and other
electrical machines.
=102. Current from two Coils.= Fig. 101 shows two coils of wire, the
smaller being connected to a cell, the larger to a galvanometer.
By moving the small coil up and down inside of the large one,
induced currents are generated, first in one direction and then in
the opposite. We have here two entirely separate circuits, in no
way connected. The _primary_ current comes from the cell, while the
_secondary_ current is an induced one. By placing a core in the small
coil of Fig. 101, the induced current will be greatly strengthened.
It is not necessary to have the two coils so that one or both of them
can move. They may be wound on the same core, or otherwise arranged as
in the induction coil. (See "Study," Chapter XXV., for experiments on
induced currents.)
CHAPTER XIII.
HOW THE INDUCTION COIL WORKS.
=103. The Coils.= We saw, § 102, that an induced current was generated
when a current-carrying coil, Fig. 101, was thrust into another coil
connected with a galvanometer. The galvanometer was used merely to show
the presence of the current. The _primary coil_ is the one connected
with the cell; the other one is called the _secondary coil_.
[Illustration: Fig. 102.]
When a current suddenly begins to flow through a coil, the effect upon
a neighboring coil is the same as that produced by suddenly bringing
a magnet near it; and when the current stops, the opposite effect is
produced. It is evident, then, that we can keep the small coil of
Fig. 101 with its core inside of the large coil, and generate induced
currents by merely making and breaking the primary circuit.
We may consider that when the primary circuit is closed, the lines of
force shoot out through the turns of the secondary coil just as they
do when a magnet or a current-carrying coil is thrust into it. Upon
opening the circuit, the lines of force cease to exist; that is, we may
imagine them drawn in again.
=104. Construction.= Fig. 102 shows one form of home-made induction
coil, given here merely to explain the action and connections. Nearly
all induction coils have some form of automatic current interrupter,
placed in the primary circuit, to rapidly turn the current off and on.
_Details of Figs. 102 and 103._ Wires 5 and 6 are the ends of the
primary coil, while wires 7 and 8 are the terminals of the secondary
coil. The primary coil is wound on a bolt which serves as the core, and
on this coil is wound the secondary which consists of many turns of
fine wire. The wires from a battery should be joined to binding-posts W
and X, and the handles, from which the shock is felt, to Y and Z. Fig.
103 shows the details of the interrupter.
[Illustration: Fig. 103.]
If the current from a cell enters at W, it will pass through the
primary coil and out at X, after going through 5, R, F, S I, B, E and
C. The instant the current passes, the bolt becomes magnetized; this
attracts A, which pulls B away from the end of S I, thus automatically
opening the circuit. B at once springs back to its former position
against SI, as A is no longer attracted; the circuit being closed, the
operation is rapidly repeated.
A _condenser_ is usually connected to commercial forms. It is placed
under the wood-work and decreases sparking at the interrupter. (See
"Apparatus Book," Chapter XI., for home-made induction coils.)
[Illustration: Fig. 104.]
Fig. 104 shows one form of coil. The battery wires are joined to the
binding-posts at the left. The secondary coil ends in two rods, and the
spark jumps from one to the other. The interrupter and a switch are
shown at the left.
Fig. 105 shows a small coil for medical purposes. A dry cell is placed
under the coil and all is included in a neat box. The handles form the
terminals of the secondary coil.
=105. The Currents.= It should be noted that the current from the
cell does not get into the secondary coil. The coils are thoroughly
insulated from each other. The secondary current is an induced one,
its voltage depending upon the relative number of turns of wire there
are in the two coils. (See Transformers.) The secondary current is
an alternating one; that is, it flows in one direction for an instant
and then immediately reverses its direction. The rapidity of the
alternations depends upon the speed of the interrupter. Coils are made
that give a secondary current with an enormous voltage; so high, in
fact, that the spark will pass many inches, and otherwise act like
those produced by static electric machines.
[Illustration: Fig. 105.]
=106. Uses of Induction Coils.= Gas-jets can be lighted at a distance
with the spark from a coil, by extending wires from the secondary
coil to the jet. Powder can be fired at a distance, and other things
performed, when a high voltage current is needed. Its use in medicine
has been noted. It is largely used in telephone work. Of late, great
use has been made of the secondary current in experiments with
vacuum-tubes, X-ray work, etc.
CHAPTER XIV.
THE ELECTRIC TELEGRAPH, AND HOW IT SENDS MESSAGES.
=107. The Complete Telegraph Line= consists of several instruments,
switches, etc., etc., but its essential parts are: The _Line_, or wire,
which connects the different stations; the _Transmitter_ or _Key_; the
_Receiver_ or _Sounder_, and the _Battery_ or _Dynamo_.
=108. The Line= is made of strong copper, iron, or soft steel wire. To
keep the current in the line it is insulated, generally upon poles, by
glass insulators. For very short lines two wires can be used, the line
wire and the return; but for long lines the earth is used as a return,
a wire from each end being joined to large metal plates sunk in the
earth.
[Illustration: Fig. 106.]
=109. Telegraph Keys= are merely instruments by which the circuit
can be conveniently and rapidly opened or closed at the will of the
operator. An ordinary push-button may be used to turn the current off
and on, but it is not so convenient as a key.
Fig. 106 shows a side view of a simple key which can be put anywhere
in the circuit, one end of the cut wire being attached to X and the
other to Y. By moving the lever C up and down according to a previously
arranged set of signals, a current will be allowed to pass to a
distant station. As X and Y are insulated from each other, the current
can pass only when C presses against Y.
Fig. 107 shows a regular key, with switch, which is used to allow the
current to pass through the instrument when receiving a message.
[Illustration: Fig. 107.]
=110. Telegraph Sounders= receive the current from some distant
station, and with its electromagnet produce sounds that can be
translated into messages.
[Illustration: Fig. 108.]
Fig. 108 shows simply an electromagnet H, the coil being connected in
series with a key K and a cell D C. The key and D C are shown by a top
view. The lever of K does not touch the other metal strap until it is
pressed down. A little above the core of H is held a strip of iron, on
armature I. As soon as the circuit is closed at K, the current rushes
through the circuit, and the core attracts I making a distinct _click_.
As soon as K is raised, I springs away from the core, if it has been
properly held. In regular instruments a click is also made when the
armature springs back again.
The time between the two clicks can be short or long, to represent
_dots_ or _dashes_, which, together with _spaces_, represent letters.
(For Telegraph Alphabet and complete directions for home-made keys,
sounders, etc., see "Apparatus Book," Chapter XIV.)
[Illustration: Fig. 109.]
[Illustration: Fig. 110.]
Fig. 109 shows a form of home-made sounder. Fig. 110 shows one form of
telegraph sounder. Over the poles of the horseshoe electromagnet is an
armature fixed to a metal bar that can rock up and down. The instant
the current passes through the coils the armature comes down until a
stop-screw strikes firmly upon the metal frame, making the down click.
As soon as the distant key is raised, the armature is firmly pulled
back and another click is made. The two clicks differ in sound, and can
be readily recognized by the operator.
=111. Connections for Simple Line.= Fig. 111 shows complete connections
for a home-made telegraph line. The capital letters are used for the
right side, R, and small letters for the left side, L. Gravity cells,
B and b, are used. The _sounders_, S and s, and the _keys_, K and k,
are shown by a top view. The broad black lines of S and s represent the
armatures which are directly over the electromagnets. The keys have
switches, E and e.
The two stations, R and L, may be in the same room, or in different
houses. The _return wire_, R W, passes from the copper of b to the zinc
of B. This is important, as the cells must help each other; that is,
they are in series. The _line wire_, L W, passes from one station to
the other, and the return may be through the wire, R W, or through the
earth; but for short lines a wire is best.
[Illustration: Fig. 111.]
=112. Operation of Simple Line.= Suppose two boys, R (right) and L
(left) have a line. Fig. 111 shows that R's switch, E, is open, while
e is closed. The entire circuit, then, is broken at but one point. As
soon as R presses his key, the circuit is closed, and the current from
both cells rushes around from B, through K, S, L W, s, k, b, R W, and
back to B. This makes the armatures of S and s come down with a click
at the same time. As soon as the key is raised, the armatures lift and
make the up-click. As soon as R has finished, he closes his switch E.
As the armatures are then held down, L knows that R has finished, so
he opens his switch e, and answers R. Both E and e are closed when the
line is not in use, so that either can open his switch at any time and
call up the other. Closed circuit cells must be used for such lines. On
very large lines dynamos are used to furnish the current.
=113. The Relay.= Owing to the large resistance of long telegraph
lines, the current is weak when it reaches a distant station, and not
strong enough to work an ordinary sounder. To get around this, relays
are used; these are very delicate instruments that replace the sounder
in the line wire circuit. Their coils are usually wound with many turns
of fine wire, so that a feeble current will move its nicely adjusted
armature. The relay armature merely acts as an automatic key to open
and close a local circuit which includes a battery and sounder. The
line current does not enter the sounder; it passes back from the relay
to the sending station through the earth.
[Illustration: Fig. 112.]
Fig. 112 gives an idea of simple relay connections. The key K, and
cell D C, represent a distant sending station. E is the electromagnet
of the relay, and R A is its armature. L W and R W represent the line
and return wires. R A will vibrate toward E every time K is pressed,
and close the local circuit, which includes a local battery, L B, and
a sounder. It is evident that as soon as K is pressed the sounder will
work with a good strong click, as the local battery can be made as
strong as desired.
Fig. 113 shows a regular instrument which opens and closes the local
circuit at the top of the armature.
[Illustration: Fig. 113.]
=114. Ink Writing Registers= are frequently used instead of sounders.
Fig. 114 shows a writing register that starts itself promptly at the
opening of the circuit, and stops automatically as soon as the circuit
returns to its normal condition. A strip of narrow paper is slowly
pulled from the reel by the machine, a mark being made upon it every
time the armature of an inclosed electromagnet is attracted. When the
circuit is simply closed for an instant, a short line, representing a
_dot_, is made.
Registers are built both single pen and double pen. In the latter case,
as the record of one wire is made with a fine pen, and the other with
a coarse pen, they can always be identified. The record being blocked
out upon white tape in solid black color, in a series of clean-cut dots
and dashes, it can be read at a glance, and as it is indelible, it may
be read years afterward. Registers are made for local circuits, for
use in connection with relays, or for direct use on main lines, as is
usually desirable in fire-alarm circuits.
[Illustration: Fig. 114.]
CHAPTER XV.
THE ELECTRIC BELL AND SOME OF ITS USES.
[Illustration: Fig. 115.]
[Illustration: Fig. 116.]
=115. Automatic Current Interrupters= are used on most common bells,
as well as on induction coils, etc. (See § 104.) Fig. 115 shows a
simple form of interrupter. The wire 1, from a cell D C, is joined to
an iron strip I a short distance from its end. The other wire from D C
passes to one end of the electromagnet coil H. The remaining end of H
is placed in contact with I as shown, completing the circuit. As soon
as the current passes, I is pulled down and away from the upper wire
2, breaking the circuit. I, being held by its left-hand end firmly in
the hand, immediately springs back to its former position, closing the
circuit again. This action is repeated, the rapidity of the vibrations
depending somewhat upon the position of the wires on I. In regular
instruments a platinum point is used where the circuit is broken; this
stands the sparking when the armature vibrates.
=116. Electric Bells= may be illustrated by referring to Fig. 116,
which shows a circuit similar to that described in § 115, but which
also contains a key K, in the circuit. This allows the circuit to
be opened and closed at a distance from the vibrating armature. The
circuit must not be broken at two places at the same time, so wires
should touch at the end of I before pressing K. Upon pressing K the
armature I will vibrate rapidly. By placing a small bell near the end
of the vibrating armature, so that it will be struck by I at each
vibration, we should have a simple electric bell. This form of electric
bell is called a _trembling_ bell, on account of its vibrating armature.
[Illustration: Fig. 117.]
[Illustration: Fig. 118.]
Fig. 117 shows a form of trembling bell with cover removed. Fig. 118
shows a _single-stroke_ bell, used for fire-alarms and other signal
work. In this the armature is attracted but once each time the current
passes. As many taps of the bell can be given as desired by pressing
the push-button. Fig. 119 shows a gong for railway crossings, signals,
etc. Fig. 120 shows a circuit including cell, push-button, and bell,
with extra wire for lengthening the line.
[Illustration: Fig. 119.]
_Electro-Mechanical Gongs_ are used to give loud signals for special
purposes. The mechanical device is started by the electric current when
the armature of the electromagnet is attracted. Springs, weights, etc.,
are used as the power. Fig. 121 shows a small bell of this kind.
[Illustration: Fig. 120.]
=117. Magneto Testing Bells=, Fig. 122, are really small hand-power
dynamos. The armature is made to revolve between the poles of strong
permanent magnets, and it is so wound that it gives a current with a
large E. M. F., so that it can ring through the large resistance of a
long line to test it.
_Magneto Signal Bells_, Fig. 123, are used as generator and bell in
connection with telephones. The generator, used to ring a bell at a
distant station, stands at the bottom of the box. The bell is fastened
to the lid, and receives current from a distant bell.
[Illustration: Fig. 121.]
[Illustration: Fig. 122.]
[Illustration: Fig. 123.]
[Illustration: Fig. 124.]
=118. Electric Buzzers= have the same general construction as electric
bells; in fact, you will have a buzzer by removing the bell from an
ordinary electric bell. Buzzers are used in places where the loud sound
of a bell would be objectionable. Fig. 124 shows the usual form of
buzzers, the cover being removed.
CHAPTER XVI.
THE TELEPHONE, AND HOW IT TRANSMITS SPEECH.
=119. The Telephone= is an instrument for reproducing sounds at a
distance, and electricity is the agent by which this is generally
accomplished. The part spoken to is called the _transmitter_, and
the part which gives sound out again is called the _receiver_. Sound
itself does not pass over the line. While the same apparatus can be
used for both transmitter and receiver, they are generally different in
construction to get the best results.
[Illustration: Fig. 125.]
[Illustration: Fig. 126.]
[Illustration: Fig. 127.]
=120. The Bell or Magneto-transmitter= generates its own current, and
is, strictly speaking, a dynamo that is run by the voice. It depends
upon induction for its action.
[Illustration: Fig. 128.]
Fig. 125 shows a coil of wire, H, with soft iron core, the ends of the
wires being connected to a delicate galvanoscope. If one pole of the
magnet H M be suddenly moved up and down near the core, an alternating
current will be generated in the coil, the circuit being completed
through the galvanoscope. As H M approaches the core the current will
flow in one direction, and as H M is withdrawn it will pass in the
opposite direction. The combination makes a miniature alternating
dynamo.
[Illustration: Fig. 129.]
If we imagine the soft iron core of H, Fig. 125, taken out, and one
pole of H M, or preferably that of a bar magnet stuck through the coil,
a feeble current will also be produced by moving the soft iron back and
forth near the magnet's pole. This is really what is done in the Bell
transmitter, soft iron in the shape of a thin disc (D, Fig. 126) being
made to vibrate by the voice immediately in front of a coil having
a permanent magnet for a core. The disc, or _diaphragm_, as it is
called, is fixed near, but it does not touch, the magnet. It is under
a constant strain, being attracted by the magnet, so its slightest
movement changes the strength of the magnetic field, causing more or
less lines of force to shoot through the turns of the coil and induce a
current. The coil consists of many turns of fine, insulated wire. The
current generated is an alternating one, and although exceedingly small
can force its way through a long length of wire.
[Illustration: Fig. 130.]
Fig. 127 shows a section of a regular transmitter, and Fig. 128 a form
of compound magnet frequently used in the transmitter. Fig. 129 shows a
transmitter with cords which contain flexible wires.
[Illustration: Fig. 131.]
=121. The Receiver=, for short lines, may have the same construction as
the Bell transmitter. Fig. 130 shows a diagram of two Bell receivers,
either being used as the transmitter and the other as the receiver.
As the alternating current goes to the distant receiver, it flies
through the coil first in one direction and then in the other. This
alternately strengthens and weakens the magnetic field near the
diaphragm, causing it to vibrate back and forth as the magnet pulls
more or less. The receiver diaphragm repeats the vibrations in the
transmitter. Nothing but the induced electric current passes over the
wires.
[Illustration: Fig. 132.]
=122. The Microphone.= If a current of electricity be allowed to
pass through a circuit like that shown in Fig. 131, which includes a
battery, a Bell receiver, and a microphone, any slight sound near the
microphone will be greatly magnified in the receiver. The microphone
consists of pieces of carbon so fixed that they form loose contacts.
Any slight movement of the carbon causes the resistance to the current
to be greatly changed. The rapidly varying resistance allows more or
less current to pass, the result being that this pulsating current
causes the diaphragm to vibrate. The diaphragm has a constantly varying
pull upon it when the carbons are in any way disturbed by the voice, or
by the ticking of a watch, etc. This principle has been made use of in
carbon transmitters, which are made in a large variety of forms.
[Illustration: Fig. 133.]
=123. The Carbon Transmitter= does not, in itself, generate a
current like the magneto-transmitter; it merely produces changes in
the strength of a current that flows through it and that comes from
some outside source. In Fig. 132, X and Y are two carbon buttons, X
being attached to the diaphragm D. Button Y presses gently against X,
allowing a little current to pass through the circuit which includes
a battery, D C, and a receiver, R. When D is caused to vibrate by the
voice, X is made to press more or less against Y, and this allows more
or less current to pass through the circuit. This direct undulating
current changes the pull upon the diaphragm of R, causing it to vibrate
and reproduce the original sounds spoken into the transmitter. In
regular lines, of course, a receiver and transmitter are connected at
each end, together with bells, etc., for signaling.
[Illustration: Fig. 134.]
=124. Induction Coils in Telephone Work.= As the resistance of long
telephone lines is great, a high electrical pressure, or E.M.F. is
desired. While the current from one or two cells is sufficient to work
the transmitter properly, and cause undulating currents in the short
line, it does not have power enough to force its way over a long line.
To get around this difficulty, an induction coil, Fig. 133, is used
to transform the battery current, that flows through the carbon
transmitter and primary coil, into a current with a high E. M. F. The
battery current in the primary coil is undulating, but always passes in
the same direction, making the magnetic field around the core weaker
and stronger. This causes an alternating current in the secondary coil
and main line. In Fig. 133 P and S represent the primary and secondary
coils. P is joined in series with a cell and carbon transmitter; S
is joined to the distant receiver. One end of S can be grounded, the
current completing the circuit through the earth and into the receiver
through another wire entering the earth.
[Illustration: Fig. 135.]
=125. Various forms= of telephones are shown in Figs. 134, 135, 136.
Fig. 134 shows a form of desk telephone; Fig. 135 shows a common form
of wall telephone; Fig. 136 shows head-telephones for switchboard
operators.
[Illustration: Fig. 136.]
CHAPTER XVII.
HOW ELECTRICITY IS GENERATED BY DYNAMOS.
=126. The Dynamo=, _Dynamo-Electric Machine_ or _Generator_, is a
machine for converting mechanical energy into an electric current,
through electromagnetic induction. The dynamo is a machine that will
convert steam power, for example, into an electric current. Strictly
speaking, a dynamo creates electrical pressure, or electromotive force,
and not electricity, just as a force-pump creates water-pressure, and
not water. They are generally run by steam or water power.
[Illustration: Fig. 137.]
=127. Induced Currents.= We have already spoken about currents being
induced by moving a coil of wire in a magnetic field. We shall now
see how this principle is used in the dynamo which is a generator of
induced currents.
[Illustration: Fig. 138.]
Fig. 137 shows how a current can be generated by a bar magnet and
a coil of wire. Fig. 138 shows how a current can be generated by a
horseshoe magnet and a coil of wire having an iron core. The ends of
the coil are to be connected to an astatic galvanoscope; this forms a
closed circuit. The coil may be moved past the magnet, or the magnet
past the coil.
[Illustration: Fig. 139.]
[Illustration: Fig. 140.]
[Illustration: Fig. 141.]
[Illustration: Fig. 142.]
Fig. 139 shows how a current can be generated by two coils, H being
connected to an astatic galvanoscope and E to a battery. By suddenly
bringing E toward H or the core of E past that of H, a current is
produced. We have in this arrangement the main features of a dynamo.
We can reverse the operation, holding E in one position and moving H
rapidly toward it. In this case H would represent the armature and E
the field-magnet. When H is moved toward E, the induced current in H
flows in one direction, and when H is suddenly withdrawn from E the
current is reversed in H. (See "Study," Chapter XXV., for experiments.)
[Illustration: Fig. 143.]
=128. Induced Currents by Rotary Motion.= The motions of the coils in
straight lines are not suitable for producing currents strong enough
for commercial purposes. In order to generate currents of considerable
strength and pressure, the coils of wire have to be pushed past
magnets, or electromagnets, with great speed. In the dynamo the coils
are so wound that they can be given a rapid rotary motion as they fly
past strong electromagnets. In this way the coil can keep on passing
the same magnets, in the same direction, as long as force is applied to
the shaft that carries them.
[Illustration: Fig. 144.]
=129. Field-Magnets; Armature; Commutator.= What we need then, to
produce an induced current by a rotary motion, is a strong magnetic
field, a rotating coil of wire properly placed in the field, and some
means of leading the current from the machine.
[Illustration: Fig. 145.]
[Illustration: Fig. 146.]
If a loop of wire, Fig. 140, be so arranged on bearings at its ends
that it can be made to revolve, a current will flow through it in
one direction during one-half of the revolution, and in the opposite
direction during the other half, it being insulated from all external
conductors. This agrees with the experiments suggested in § 127, when
the current generated in a coil passed in one direction during its
motion _toward_ the strongest part of the field, and in the opposite
direction when the coil passed _out_ of it. A coil must be cut by
lines of force to generate a current. A current inside of the machine,
as in Fig. 140, would be of no value; it must be led out to external
conductors where it can do work. Some sort of sliding contact is
necessary to connect a revolving conductor with outside stationary
ones. The magnet, called the _field-magnet_, is merely to furnish lines
of magnetic force. The one turn of wire represents the simplest form of
_armature_.
Fig. 141 shows the ends of a coil joined to two rings, X, Y, insulated
from each other, and rotating with the coil. The two stationary pieces
of carbon, A, B, called _brushes_, press against the rings, and to
these are joined wires, which complete the circuit, and which lead out
where the current can do work. The arrows show the direction of the
current during one-half of a revolution. The rings form a _collector_,
and this arrangement gives an _alternating current_.
[Illustration: Fig. 147.]
In Fig. 142 the ends of the coil are joined to the two halves of a
cylinder. These halves, X and Y, are insulated from each other, and
from the axis. The current flows from X onto the brush A, through some
external circuit, to do the work, and thence back through brush B onto
Y. By the time that Y gets around to A, the direction of the current in
the loop has reversed, so that it passes toward Y, but it still enters
the outside circuit through A, because Y is then in contact with A.
This device is called a _commutator_, and it allows a constant or
_direct current_ to leave the machine.
[Illustration: Fig. 148.]
In regular machines, the field-magnets are electromagnets, the whole
or a part of the current from the dynamo passing around them on its
way out, to excite them and make a powerful field between the poles.
To lessen the resistance to the lines of force on their way from the
N to the S pole of the field-magnets, the armature coils are wound on
an iron core; this greatly increases the strength of the field, as
the lines of force have to jump across but two small air-gaps. There
are many loops of wire on regular armatures, and many segments to the
commutator, carefully insulated from each other, each getting its
current from the coil attached to it.
=130. Types of Dynamos.= While there is an almost endless number of
different makes and shapes of dynamos, they may be divided into two
great types; the _continuous_ or _direct current_, and the _alternating
current_ dynamo. Direct current machines give out a current which
constantly flows in one direction, and this is because a commutator is
used. Alternating currents come from collectors or rings, as shown in
Fig. 141; and as an alternating current cannot be used to excite the
fields, an outside current from a small direct current machine must be
used. These are called exciters.
[Illustration: Fig. 149.]
In direct current machines enough residual magnetism is left in the
field to induce a slight current in the armature when the machine is
started. This immediately adds strength to the field-magnets, which, in
turn, induce a stronger current in the armature.
=131. Winding of Dynamos.= There are several ways of winding dynamos,
depending upon the special uses to be made of the current.
The _series wound_ dynamo, Fig. 143, is so arranged that the entire
current passes around the field-magnet cores on its way from the
machine. In the _shunt wound_ dynamo, Fig. 144, a part, only, of the
current from the machine is carried around the field-magnet cores
through many turns of fine wire. The _compound wound_ dynamo is really
a combination of the two methods just given. In _separately-excited_
dynamos, the current from a separate machine is used to excite the
field-magnets.
=132. Various Machines.= Fig. 145 shows a hand power dynamo
which produces a current for experimental work. Fig. 146 shows a
magneto-electrical generator which produces a current for medical use.
Figs. 147, 148 show forms of dynamos, and Fig. 149 shows how arc lamps
are connected in series to dynamos.
[Illustration]
CHAPTER XVIII.
HOW THE ELECTRIC CURRENT IS TRANSFORMED.
=133. Electric Current and Work.= The amount of work a current can do
depends upon two factors; the strength (amperes), and the pressure,
or E. M. F. (volts). A current of 10 amperes with a pressure of 1,000
volts = 10 × 1,000 = 10,000 watts. This furnishes the same amount of
energy as a current of 50 amperes at 200 volts; 50 × 200 = 10,000 watts.
=134. Transmission of Currents.= It is often necessary to carry a
current a long distance before it is used. A current of 50 amperes
would need a copper conductor 25 times as large (sectional area) as one
to carry the 10 ampere current mentioned in § 133. As copper conductors
are very expensive, electric light companies, etc., generally try to
carry the current on as small a wire as possible. To do this, the
voltage is kept high, and the amperage low. Thus, as seen in § 133,
the current of 1,000 volts and 10 amperes could be carried on a much
smaller wire than the other current of equal energy. A current of
1,000 volts, however, is not adapted for lights, etc., so it has to be
changed to lower voltage by some form of transformer before it can be
used.
=135. Transformers=, like induction coils, are instruments for changing
the E. M. F. and strength of currents. There is very little loss of
energy in well-made transformers. They consist of two coils of wire on
one core; in fact, an induction coil may be considered a transformer,
but in this a direct current has to be interrupted. If the secondary
coil has 100 times as many turns of wire as the primary, a current of
100 volts can be taken from the secondary coil when the primary current
is but 1 volt; but the _strength_ (amperes) of this new current will be
but one-hundredth that of the primary current.
By using the coil of fine wire as the primary, we can lower the voltage
and increase the strength in the same proportion.
[Illustration: Fig. 150.]
[Illustration: Fig. 151.]
Fig. 150 shows about the simplest form of transformer with a solid iron
core, on which are wound two coils, the one, P, being the primary, and
the other, S, the secondary. Fig. 151 shows the general appearance of
one make of transformer. The operation of this apparatus, as already
mentioned, is to reduce the high pressure alternating current sent out
over the conductors from the dynamo, to a potential at which it can
be employed with convenience and safety, for illumination and other
purposes. They consist of two or more coils of wire most carefully
insulated from one another. A core or magnetic circuit of soft iron,
composed of very thin punchings, is then formed around these coils,
the purpose of the iron core being to reduce the magnetic resistance
and increase the inductive effect. One set of these coils is connected
with the primary or high-pressure wires, while the other set, which are
called the secondary coils, is connected to the house or low-pressure
wires, or wherever the current is required for use. The rapidly
alternating current impulses in the primary or high-pressure wires
induce secondary currents similar in form but opposite in direction
in the secondary coils. These current impulses are of a much lower
pressure, depending upon the ratio of the number of turns of wire
in the respective coils, it being customary to wind transformers in
such a manner as to reduce from 1,000 or 2,000-volt primaries to 50
or 100-volt secondaries, at which voltage the secondary current is
perfectly harmless.
[Illustration: Fig. 152.]
=136. Motor-Dynamos.= Fig. 152. These consist essentially of two
belt-type machines on a common base, direct coupled together, one
machine acting as a motor to receive current at a certain voltage,
and the other acting as a dynamo to give out the current usually
at a different voltage. As they transform current from one voltage
to another, motor-dynamos are sometimes called Double Field Direct
Current Transformers. The larger sizes have three bearings, one bearing
being between the two machines, while the smaller sizes have but two
bearings, the two armatures being fastened to a common spider.
[Illustration: Fig. 153.]
_Applications._ The uses to which motor-dynamos are put are very
various. They are extensively used in the larger sizes as "Boosters,"
for giving the necessary extra force on long electric supply circuits
to carry the current to the end with the same pressure as that which
reaches the ends of the shorter circuits from the station.
Motor-dynamos have the advantage over dynamotors, described later, of
having the secondary voltage easily and economically varied over wide
ranges by means of a regulator in the dynamo field.
=137. Dynamotors.= Fig. 153. In Dynamotors the motor and dynamo
armatures are combined in one, thus requiring a single field only.
The primary armature winding, which operates as a motor to drive the
machine, and the secondary or dynamo winding, which operates as a
generator to produce a new current, are upon the same armature core,
so that the armature reaction of one winding neutralizes that of the
other. They therefore have no tendency to spark, and do not require
shifting of the brushes with varying load. Having but one field and two
bearings, they are also more efficient than motor-dynamos.
_Applications._ They have largely displaced batteries for telegraph
work. The size shown, occupying a space of about 8-inch cube, and
having an output of 40 watts, will displace about 800 gravity cells,
occupying a space of about 10 feet cube. The cost of maintenance of
such a battery per year, exclusive of rent, is about $800, whereas the
1-6 dynamotor can be operated at an annual expense of $150.
Dynamotors are largely used by telephone companies for charging storage
batteries, and for transforming from direct to alternating current, for
ringing telephone bells. Electro-cautery, electroplating, and electric
heating also give use to dynamotors.
CHAPTER XIX.
HOW ELECTRIC CURRENTS ARE DISTRIBUTED FOR USE.
[Illustration: Fig. 154.]
[Illustration: Fig. 155.]
[Illustration: Fig. 156.]
=138. Conductors and Insulators.= To carry the powerful current from
the generating station to distant places where it is to give heat,
power, or light, or even to carry the small current of a single cell
from one room to another, _conductors_ must be used. To keep the
current from passing into the earth before it reaches its destination
_insulators_ must be used. The form of conductors and insulators used
will depend upon the current and many other conditions. It should be
remembered that the current has to be carried to the lamp or motor,
through which it passes, and then back again to the dynamo, to form a
complete circuit. A break anywhere in the circuit stops the current.
Insulators are as important as conductors.
[Illustration: Fig. 157.]
[Illustration: Fig. 158.]
=139. Mains, Service Wires, etc.= From the switchboard the current
flows out through the streets in large conductors, or _mains_, the
supply being kept up by the dynamos, just as water-pressure is kept up
by the constant working of pumps. Branches, called _service wires_, are
led off from the mains to supply houses or factories, one wire leading
the current into the house from one main, and a similar one leading it
out of the house again to the other main.
[Illustration: Fig. 159.]
[Illustration: Fig. 160.]
In large buildings, pairs of wires, called _risers_, branch out from
the service wires and carry the current up through the building. These
have still other branches--_floor mains_, _etc._, that pass through
halls, etc., smaller branches finally reaching the lamps. The sizes of
all of these wires depend upon how much current has to pass through
them. The mains in large cities are usually placed underground. In some
places they are carried on poles.
[Illustration: Fig. 161.]
=140. Electric Conduits= are underground passages for electric wires,
cables, etc. There are several ways of insulating the conductors.
Sometimes they are placed in earthenware or iron tubes, or in wood that
has been treated to make it water-proof. At short distances are placed
man-holes, where the different lengths are joined, and where branches
are attached.
[Illustration: Fig. 162.]
Fig. 154 shows creosoted wooden pipes; Fig. 155 shows another form of
wooden pipe. Fig. 156 shows a coupling-box used to join Edison tubes.
The three wires, used in the three-wire system, are insulated from each
other, the whole being surrounded by an iron pipe of convenient length
for handling. Fig. 157 shows sections of man-holes and various devices
used in conduit work.
[Illustration: Fig. 163.]
=141. Miscellaneous Appliances.= When the current enters a house for
incandescent lighting purposes, for example, quite a number of things
are necessary. To measure the current a meter is usually placed in the
cellar. In new houses the insulated conductors are usually run through
some sort of tube which acts as a double protection, all being hidden
from view. Fig. 158 shows a short length of iron tube with a lining of
insulating material. Wires are often run through tubes made of rubber
and various other insulating materials.
Where the current is to be put into houses after the plastering has
been done, the wires are usually run through _mouldings_ or supported
by _cleats_. Fig. 159 shows a cross-section of moulding. The insulated
wires are placed in the slots, which are then covered.
[Illustration: Fig. 164.]
[Illustration: Fig. 165.]
[Illustration: Fig. 166.]
[Illustration: Fig. 167.]
Fig. 160 shows a form of porcelain cleat. These are fastened to
ceilings or walls, and firmly hold the insulated wires in place. Fig.
161 shows a wood cleat. Fig. 162 shows small porcelain _insulators_.
These may be screwed to walls, etc., the wire being then fastened to
them. Fig. 163 shows how telegraph wires are supported and insulated.
Fig. 164 shows how wires may be carried by tree and insulated from them.
[Illustration: Fig. 168.]
[Illustration: Fig. 169.]
[Illustration: Fig. 170.]
=142. Safety Devices.= We have seen that when too large a current
passes through a wire, the wire becomes heated and may even be melted.
Buildings are wired to use certain currents, and if from any cause much
more current than the regular amount should suddenly pass through the
service wires into the house, the various smaller wires would become
overheated, and perhaps melt or start a fire. An accidental short
circuit, for example, would so reduce resistance that too much current
would suddenly rush through the wires. There are several devices by
which the over-heating of wires is obviated.
[Illustration: Figs. 171 to 175.]
Fig. 165 shows a _safety fuse_, or _safety cut-out_, which consists of
a short length of easily fusible wire, called _fuse wire_, placed in
the circuit and supported by a porcelain block. These wires are tested,
different sizes being used for different currents. As soon as there
is any tendency toward over-heating, the fuse _blows_; that is, it
promptly melts and opens the circuit before any damage can be done to
the regular conductors. Fig. 166 shows a cross-section of a _fuse plug_
that can be screwed into an ordinary socket. The fuse wire is shown
black.
Fig. 167 shows a _fuse link_. These are also of fusible material, and
so made that they can be firmly held under screw-heads. For heavy
currents _fuse ribbons_ are used, or several wires or links may be
used side by side. Fig. 168 shows a _fusible rosette_. Fig. 169 shows
two fuse wires fixed between screw-heads, the current passing through
them in opposite directions, both sides of the circuit being included.
Fig. 170 shows various forms of cut-outs.
[Illustration: Fig. 176.]
=143. Wires and Cables= are made in many sizes. Figs. 171 to 175 show
various ways of making small conductors. They are made very flexible,
for some purposes, by twisting many small copper wires together, the
whole being then covered with insulating material.
[Illustration: Fig. 177.]
Figs. 176, 177, show sections of submarine cables. Such cables consist
of copper conductors insulated with pure gutta-percha. These are then
surrounded by hempen yarn or other elastic material, and around the
whole are placed galvanized iron armor wires for protection. Each core,
or conductor, contains a conductor consisting of a single copper wire
or a strand of three or more twisted copper wires.
=144. Lamp Circuits.= As has been noted before, in order to have the
electric current do its work, we must have a complete circuit. The
current must be brought back to the dynamo, much of it, of course,
having been used to produce light, heat, power, etc. For lighting
purposes this is accomplished in two principal ways.
[Illustration: Fig. 178.]
Fig. 178 shows a number of lamps so arranged, "in series," that the
same current passes through them all, one after the other. The total
resistance of the circuit is large, as all of the lamp resistances are
added together.
[Illustration: Fig. 179.]
Fig. 179 shows lamps arranged side by side, or "in parallel," between
the two main wires. The current divides, a part going through each lamp
that operates. The total resistance of the circuit is not as large
as in the series arrangement, as the current has many small paths in
going from one main wire to the other. Fig. 179 also shows the ordinary
_two-wire system_ for incandescent lighting, the two main wires having
usually a difference of potential equal to 50 or 110 volts. These
comparatively small pressures require fairly large conductors.
_The Three-Wire System_, Fig. 180, uses the current from two dynamos,
arranged with three main wires. While the total voltage is 220, one of
the wires being neutral, 110 volts can be had for ordinary lamps. This
voltage saves in the cost of conductors.
[Illustration: Fig. 180.]
[Illustration: Fig. 181.]
_The Alternating System_, Fig. 181, uses transformers. The high
potential of the current allows small main wires, from which branches
can be run to the primary coil of the transformer. The secondary coil
sends out an induced current of 50 or 110 volts, while that in the
primary may be 1,000 to 10,000 volts.
CHAPTER XX.
HOW HEAT IS PRODUCED BY THE ELECTRIC CURRENT.
=145. Resistance and Heat.= We have seen that all wires and conductors
offer resistance to the electric current. The smaller the wire the
greater its resistance. Whenever resistance is offered to the current,
heat is produced. By proper appliances, the heat of resistance can be
used to advantage for many commercial enterprises. Dynamos are used to
generate the current for heating and lighting purposes.
[Illustration: Fig. 182.]
Fig. 182 shows how the current from two strong cells can be used to
heat a short length of very fine platinum or German-silver wire.
The copper conductors attached to the cells do not offer very much
resistance.
It will be seen from the above that in all electrical work the sizes
of the wires used have to be such that they do not overheat. The coils
of dynamos, motors, transformers, ampere-meters, etc., etc., become
somewhat heated by the currents passing through them, great care being
taken that they are properly designed and ventilated so that they will
not burn out.
[Illustration: Fig. 183.]
[Illustration: Fig. 184.]
=146. Electric Welding.= Fig. 183 shows one form of electric welding
machine. The principle involved in the art of electric welding is
that of causing currents of electricity to pass through the abutting
ends of the pieces of metal which are to be welded, thereby generating
heat at the point of contact, which also becomes the point of greatest
resistance, while at the same time mechanical pressure is applied
to force the parts together. As the current heats the metal at the
junction to the welding temperature, the pressure follows up the
softening surface until a complete union or weld is effected; and, as
the heat is first developed in the interior of the parts to be welded,
the interior of the joint is as efficiently united as the visible
exterior. With such a method and apparatus, it is found possible to
accomplish not only the common kinds of welding of iron and steel, but
also of metals which have heretofore resisted attempts at welding, and
have had to be brazed or soldered.
[Illustration: Figs. 185 to 189.]
The introduction of the electric transformer enables enormous currents
to be so applied to the weld as to spend their energy just at the point
where heating is required. They need, therefore, only to be applied
for a few seconds, and the operation is completed before the heat
generated at the weld has had time to escape by conduction to any other
part.
Although the quantity of the current so employed in the pieces to be
welded is enormous, the potential at which it is applied is extremely
low, not much exceeding that of the batteries of cells used for ringing
electric bells in houses.
[Illustration: Fig. 190.]
=147. Miscellaneous Applications.= Magneto Blasting Machines are now
in very common use for blasting rocks, etc. Fig. 184 shows one, it
being really a small hand dynamo, occupying less than one-half a cubic
foot of space. The armature is made to revolve rapidly between the
poles of the field-magnet by means of a handle that works up and down.
The current is carried by wires from the binding-posts to fuses. The
heat generated by resistance in the fuse ignites the powder or other
explosive.
_Electric soldering irons_, _flat-irons_, _teakettles_, _griddles_,
_broilers_, _glue pots_, _chafing-dishes_, _stoves_, etc., etc., are
now made. Figs. 185 to 189 show some of these applications. The coils
for producing the resistance are inclosed in the apparatus.
[Illustration: Fig. 191.]
Fig. 190 shows a complete electric kitchen. Any kettle or part of the
outfit can be made hot by simply turning a switch. Fig. 191 shows an
electric heater placed under a car seat. Many large industries that
make use of the heating effects of the current are now being carried
on.
CHAPTER XXI.
HOW LIGHT IS PRODUCED BY THE INCANDESCENT LAMP.
[Illustration: Fig. 192.]
[Illustration: Fig. 193.]
=148. Incandescence.= We have just seen that the electric current
produces heat when it flows through a conductor that offers
considerable resistance to it. As soon as this was discovered men
began to experiment to find whether a practical light could also be
produced. It was found that a wire could be kept hot by constantly
passing a current through it, and that the light given out from it
became whiter and whiter as the wire became hotter. The wire was said
to be _incandescent_, or glowing with heat. As metal wires are good
conductors of electricity, they had to be made extremely fine to offer
enough resistance; too fine, in fact, to be properly handled.
=149. The Incandescent Lamp.= Many substances were experimented upon
to find a proper material out of which could be made a _filament_
that would give the proper resistance and at the same time be strong
and lasting. It was found that hair-like pieces of carbon offered the
proper resistance to the current. When heated in the air, however,
carbon burns; so it became necessary to place the carbon filaments in a
globe from which all the air had been pumped before passing the current
through them. This proved to be a success.
[Illustration: Fig. 194.]
[Illustration: Fig. 195.]
[Illustration: Fig. 196.]
Fig. 192 shows the ordinary form of lamp. The _carbon filament_ is
attached, by carbon paste, to short platinum wires that are sealed in
the glass, their lower ends being connected to short copper wires that
are joined to the terminals of the lamp. When the lamp is screwed
into its socket, the current can pass up one side of the filament
and down the other. The filaments used have been made of every form
of carbonized vegetable matter. Bamboo has been largely used, fine
strips being cut by dies and then heated in air-tight boxes containing
fine carbon until they were thoroughly carbonized. This baking of the
bamboo produces a tough fiber of carbon. Various forms of thread have
been carbonized and used. Filaments are now made by pressing finely
pulverized carbon, with a binding material, through small dies. The
filaments are made of such sizes and lengths that will adapt them to
the particular current with which they are to be used. The longer the
filament, the greater its resistance, and the greater the voltage
necessary to push the current through it.
[Illustration: Fig. 197.]
[Illustration: Fig. 198.]
After the filaments are properly attached, the air is pumped from the
bulb or globe. This is done with some form of mercury pump, and the air
is so thoroughly removed from the bulb that about one-millionth only of
the original air remains. Before sealing off the lamp, a current is
passed through the filament to drive out absorbed air and gases, and
these are carried away by the pump. By proper treatment the filaments
have a uniform resistance throughout, and glow uniformly when the
current passes.
[Illustration: Fig. 199.]
[Illustration: Fig. 200.]
=150. Candle-Power.= A lamp is said to have 4, 8, 16 or more
candle-power. A 16-candle-power lamp, for example, means one that will
give as much light as sixteen standard candles. A standard sperm candle
burns two grains a minute. The candle-power of a lamp can be increased
by forcing a strong current through it, but this shortens its life.
_The Current_ used for incandescent lamps has to be strong enough to
force its way through the filament and produce a heat sufficient to
give a good light. The usual current has 50 or 110 volts, although
small lamps are made that can be run by two or three cells. If the
voltage of the current is less than that for which the lamp was made,
the light will be dim. The filament can be instantly burned out by
passing a current of too high pressure through it.
Even with the proper current, lamps soon begin to deteriorate, as small
particles of carbon leave the filament and cling to the glass. This is
due to the evaporation, and it makes the filament smaller, and a higher
pressure is then needed to force the current through the increased
resistance; besides this, the darkened bulb does not properly let the
light out. The current may be direct or alternating.
[Illustration: Fig. 201.]
[Illustration: Fig. 202.]
=151. The Uses= to which incandescent lamps are put are almost
numberless. Fig. 193 shows a decorative lamp. Fancy lamps are made in
all colors. Fig. 194 shows a conic candle lamp, to imitate a candle.
What corresponds to the body of the candle (see figure B to C) is a
delicately tinted opal glass tube surmounted (see figure A to B) by a
finely proportioned conic lamp with frosted globe. C to D in the figure
represents the regular base, and thus the relative proportions of the
parts are shown. Fig. 195 shows another form of candelabra lamp. Fig.
196 shows small dental lamps. Fig. 197 shows a small lamp with mirror
for use in the throat. Fig. 198 shows lamp with half shade attached,
used for library tables. Fig. 199 shows an electric pendant for several
lamps, with shade. Fig. 200 shows a lamp guard. Fig. 201 shows a lamp
socket, into which the lamp is screwed. Fig. 202 shows incandescent
bulbs joined in parallel to the + and - mains. Fig. 203 shows how the
lamp cord can be adjusted to desired length. Fig. 204 shows a lamp
with reflector placed on a desk. Fig. 205 shows a form of shade and
reflector.
[Illustration: Fig. 203.]
[Illustration: Fig. 204.]
[Illustration: Fig. 205.]
CHAPTER XXII.
HOW LIGHT IS PRODUCED BY THE ARC LAMP.
=152. The Electric Arc.= When a strong current passes from one carbon
rod to another across an air-space, an _electric arc_ is produced.
When the ends of two carbon rods touch, a current can pass from one to
the other, but the imperfect contact causes resistance enough to heat
the ends red-hot. If the rods be separated slightly, the current will
continue to flow, as the intensely heated air and flying particles of
carbon reduce the resistance of the air-space.
Fig. 206 shows two carbon rods which are joined to the two terminals
of a dynamo. The upper, or positive, carbon gradually wears away and
becomes slightly hollow. The heated _crater_, as it is called, is the
hottest part. The negative carbon becomes pointed. The arc will pass in
a vacuum, and even under water.
[Illustration: Fig. 206.]
As the electric arc is extremely hot, metals are easily vaporized in
it; in fact, even the carbon rods themselves slowly melt and vaporize.
This extreme heat is used for many industrial purposes.
[Illustration: Fig. 207.]
[Illustration: Fig. 208.]
"The phenomenon of the electric arc was first noticed by Humphrey
Davy in 1800, and its explanation appears to be the following: Before
contact the difference of potential between the points is insufficient
to permit a spark to leap across even 1/10000 of an inch of air-space,
but when the carbons are made to touch, a current is established.
On separating the carbons, the momentary extra current due to
self-induction of the circuit, which possesses a high electromotive
force, can leap the short distance, and in doing so volatilizes a small
quantity of carbon between the points. Carbon vapor, being a partial
conductor, allows the current to continue to flow across the gap,
provided it be not too wide; but as the carbon vapor has a very high
resistance it becomes intensely heated by the passage of the current,
and the carbon points also grow hot. Since, however, solid matter is a
better radiator than gaseous matter, the carbon points emit far more
light than the arc itself, though they are not so hot. It is observed,
also, that particles of carbon are torn away from the + electrode,
which becomes hollowed out to a cup-shape, and some of these are
deposited on the - electrode."
[Illustration: Fig. 209.]
=153. Arc Lamps.= As the carbons gradually wear away, some device is
necessary to keep their ends the right distance apart. If they are too
near, the arc is very small; and if too far apart, the current can not
pass and the light goes out. The positive carbon gives the more intense
light and wears away about twice as fast as the - carbon, so it is
placed above the - carbon, to throw the light downwards.
[Illustration: Fig. 210.]
[Illustration: Fig. 211.]
Arc lamps contain some device by which the proper distance between
the carbons can be kept. Most of them grip the upper carbon and pull
it far enough above the lower one to establish the arc. As soon as
the distance between them gets too great again, the grip on the upper
carbon is loosened, allowing the carbon to drop until it comes in
contact with the lower one, thus starting the current again. These
motions are accomplished by electromagnets. Fig. 207 shows a form of
arc lamp with _single carbons_ that will burn from 7 to 9 hours.
[Illustration: Fig. 212.]
[Illustration: Fig. 213.]
[Illustration: Fig. 214.]
Fig. 208 shows the mechanism by which the carbons are regulated. Fig.
209 shows a form of _double carbon_, or _all-night_ lamp, one set of
carbons being first used, the other set being automatically switched in
at the proper time.
[Illustration: Fig. 215.]
Figs. 210, 211 show forms of _short arc lamps_, for use under low
ceilings, so common in basements, etc.
Fig. 212 shows a _hand-feed focussing_ type of _arc lamp_. In regular
street lamps, the upper carbon only is fed by mechanism, as it burns
away about twice as fast as the lower one, thus bringing the arc lower
and lower. When it is desired to keep the arc at the focus of a
reflector, both carbons must be fed.
Fig. 213 shows a _theatre arc lamp_, used to throw a strong beam of
light from the balcony to the stage.
Fig. 214 shows the arc lamp used as a search-light. The reflector
throws a powerful beam of light that can be seen for miles; in
fact, the light is used for signalling at night. Fig. 215 shows how
search-lights are used at night on war-vessels.
CHAPTER XXIII.
X-RAYS, AND HOW THE BONES OF THE HUMAN BODY ARE PHOTOGRAPHED.
[Illustration: Fig. 216.]
[Illustration: Fig. 217.]
=154. Disruptive Discharges.= We have seen, in the study of induction
coils, that a spark can jump several inches between the terminals
of the secondary coil. The attraction between the two oppositely
charged terminals gets so great that it overcomes the resistance of
the air-space between them, a brilliant spark passes, and they are
discharged. This sudden discharge is said to be _disruptive_, and it
is accompanied by a flash of light and a loud report. The _path_ of
the discharge may be nearly straight, or crooked, depending upon the
nature of the material in the gap between the terminals.
[Illustration: Fig. 218.]
[Illustration: Fig. 219.]
=155. Effect of Air Pressure on Spark.= The disruptive spark takes
place in air at ordinary pressures. The nature of the spark is greatly
changed when the pressure of the air decreases. Fig. 216 shows an
air-tight glass tube so arranged that the air can be slowly removed
with an air-pump. The upper rod shown can be raised or lowered to
increase the distance between it and the lower rod, these acting as the
terminals of an induction coil. Before exhausting any air, the spark
will jump a small distance between the rods and act as in open air. As
soon as a small amount of air is removed, a change takes place. The
spark is not so intense and has no definite path, there being a general
glow throughout the tube. As the air pressure becomes still less, the
glow becomes brighter, until the entire tube is full of purple light
that is able to pass the entire length of it; that is, the discharge
takes place better in rarefied air than it does in ordinary air.
=156. Vacuum-Tubes.= As electricity passes through rarefied gases much
easier than through ordinary air, regular tubes, called _vacuum-tubes_,
are made for such study. Fig. 217 shows a plain tube of this kind,
platinum terminals being fused in the glass for connections. These
tubes are often made in complicated forms, Fig. 218, with colored
glass, and are called _Geissler tubes_. They are often made in such a
way that the electrodes are in the shape of discs, etc., and are called
_Crookes tubes_, Fig. 219. A slight amount of gas is left in the tubes.
[Illustration: Fig. 220.]
[Illustration: Fig. 220-A.]
=157. Cathode Rays.= The _cathode_ is the electrode of a vacuum-tube
by which the current leaves the tube, and it has been known for some
time that some kind of influence passes in straight lines from this
point. Shadows, Fig. 219, are cast by such rays, a screen being placed
in their path.
=158. X-Rays.= Professor Roentgen of Würzburg discovered that when the
cathode rays are allowed to fall upon a solid body, the solid body
gives out still other rays which differ somewhat from the original
cathode rays. They can penetrate, more or less, through many bodies
that are usually considered opaque. The hand, for example, may be used
as a negative for producing a photograph of the bones, as the rays do
not pass equally well through flesh and bone.
[Illustration: Fig. 221.]
Fig. 220 shows a Crookes tube fitted with a metal plate, so that
the cathode rays coming from C will strike it. The X-rays are given
out from P. These rays are invisible and are even given out where
the cathode rays strike the glass. Some chemical compounds are made
luminous by these rays; so screens are made and coated with them in
order that the shadows produced by the X-rays can be seen by the
eye. Professor Roentgen named these the X-rays. Fig. 220-A shows a
_fluoroscope_ that contains a screen covered with proper chemicals.
[Illustration: Fig. 222.]
[Illustration: Fig. 223.]
=159. X-Ray Photographs.= Bone does not allow the X-rays to pass
through it as readily as flesh, so if the hand be placed over a
sensitized photographic plate, Fig. 221, and proper connections be
made with the induction coil, etc., the hand acts as a photographic
negative. Upon developing the plate, as in ordinary photography,
a picture or shadow of the bones will be seen. Fig. 222 shows the
arrangement of battery, induction coil, focus tube, etc., for examining
the bones of the human body.
Fig. 223 shows the bones of a fish. Such photographs have been very
valuable in discovering the location of bullets, needles, etc., that
have become imbedded in the flesh, as well as in locating breaks in the
bones.
CHAPTER XXIV.
THE ELECTRIC MOTOR, AND HOW IT DOES WORK.
=160. Currents and Motion.= We have seen, Chapter XII., that when coils
of wire are rapidly moved across a strong magnetic field, a current
of electricity is generated. We have now to deal with the opposite of
this; that is, we are to study how _motion_ can be produced by allowing
a current of electricity to pass through the armature of a machine.
[Illustration: Fig. 224.]
[Illustration: Fig. 225.]
Fig. 224 shows, by diagram, a coil H, suspended so that it can move
easily, its ends being joined to a current reverser, and this, in turn,
to a dry cell D C. A magnet, H M, will attract the core of H when
no current passes. When the current is allowed to pass first in one
direction and then in the opposite direction, by using the reverser,
the core of H will jump back and forth from one pole of H M to the
other. There are many ways by which motion can be produced by the
current, but to have it practical, the motion must be a rotary one.
(See "Study," Chapter XXVI., for numerous experiments.)
[Illustration: Fig. 226.]
=161. The Electric Motor= is a machine for transforming electric
energy into mechanical power. The construction of motors is very
similar to that of dynamos. They have field-magnets, armature coils,
commutator, etc.; in fact, the armature of an ordinary direct current
dynamo will revolve if a current be passed through it, entering by one
brush and leaving by the other. There are many little differences of
construction, for mechanical and electrical reasons, but we may say
that the general construction of dynamos and motors is the same.
Fig. 225 shows a coil of wire, the ends of which are connected to
copper and zinc plates. These plates are floated in dilute sulphuric
acid, and form a simple cell which sends a current through the wire, as
shown by the arrows.
[Illustration: Fig. 227.]
We have seen that a current-carrying wire has a magnetic field and
acts like a magnet; so it will be easily seen that if a magnet be held
near the wire it will be either attracted or repelled, the motion
depending upon the poles that come near each other. As shown in the
figure, the N pole of the magnet repels the field of the wire, causing
it to revolve. We see that this action is just the reverse to that in
galvanometers, where the coil is fixed, and the magnet, or magnetic
needle, is allowed to move. As soon as the part of the wire, marked A
in Fig. 225, gets a little distance from the pole, the opposite side
of the wire, B, begins to be attracted by it, the attraction getting
stronger and stronger, until it gets opposite the N pole. If the N pole
were still held in place, B would vibrate back and forth a few times,
and finally come to rest near the pole. If, however, as soon as B gets
opposite N the S pole of the magnet be quickly turned toward B, the
coil will be repelled and the rotary motion will continue.
[Illustration: Fig. 228.]
[Illustration: Figs. 229 to 231.]
[Illustration: Fig. 232.]
[Illustration: Fig. 233.]
Let us now see how this helps to explain electric motors. We may
consider the wire of Fig. 225 as one coil of an armature, and the
plates, C and Z, as the halves of a commutator. In this arrangement, it
must be noted, the current always flows through the armature coil in
the same direction, the rotation being kept up by reversing the poles
of the field-magnet. In ordinary simple motors the current is reversed
in the armature coils, the field-magnets remaining in one position
without changing the poles. This produces the same effect as the above.
The current is reversed automatically as the brushes allow the current
to enter first one commutator bar and then the opposite one as the
armature revolves. The regular armatures have many coils and many
commutator bars, as will be seen by examining the illustrations shown.
The ordinary galvanometer may be considered a form of motor. By
properly opening and closing the circuit, the rotary motion of the
needle can be kept up as long as current is supplied. Even an electric
bell or telegraph sounder may be considered a motor, giving motion
straight forward and back.
=162. The Uses of Motors= are many. It would be impossible to mention
all the things that are done with the power from motors. A few
illustrations will give an idea of the way motors are attached to
machines.
Fig. 226 shows one form of motor, the parts being shown in Fig. 227.
[Illustration: Fig. 234.]
Fig. 228 shows a fan motor run by a battery. They are generally run
by the current from the street. Figs. 229-231 show other forms of fan
motors. Fig. 232 shows an electric hat polisher. A church organ bellows
is shown in Fig. 233, so arranged that it can be pumped by an electric
motor. Fig. 234 shows a motor direct connected to a drill press.
=163. Starting Boxes.= If too much current were suddenly allowed to
pass into the armature of a motor, the coils would be over-heated,
and perhaps destroyed, before it attained its full speed. A rapidly
revolving armature will take more current, without being overheated,
than one not in motion. A motor at full speed acts like a dynamo, and
generates a current which tends to flow from the machine in a direction
opposite to that which produces the motion. It is evident, then, that
when the armature is at rest, all the current turned on passes through
it without meeting with this opposing current.
[Illustration: Fig. 235.]
[Illustration: Fig. 236.]
Fig. 235 shows a starting, stopping, and regulating box, inside of
which are a number of German-silver resistance coils properly connected
to contact-points at the top. By turning the knob, the field of the
motor is immediately charged first through resistance, then direct, and
then the current is put on the armature gradually through a series of
coils, the amount of current depending upon the distance the switch is
turned. Fig. 236 shows a cross section of the same.
CHAPTER XXV.
ELECTRIC CARS, BOATS, AND AUTOMOBILES.
=164. Electric Cars=, as well as boats, automobiles, etc., etc., are
moved by the power that comes from electric motors, these receiving
current from the dynamos placed at some "central station." We have
already seen how the motor can do many kinds of work. By properly
gearing it to the car wheels, motion can be given to them which will
move the car.
[Illustration: Fig. 237.]
Fig. 237 shows two dynamos which will be supposed to be at a power
house and which send out a current to propel cars. From the figure
it will be seen that the wires over the cars, called trolley-wires,
are connected to the positive (+) terminals of the dynamos, and that
the negative (-) terminals are connected to the tracks. In case a
wire were allowed to join the trolley-wire and track, we should have
a short circuit, and current would not only rush back to the dynamo
without doing useful work, but it would probably injure the machines.
When some of the current is allowed to pass through a car, motion is
produced in the motors, as has been explained. As the number of cars
increases, more current passes back to the dynamos, which must do more
work to furnish such current.
_Trolley-poles_, fastened to the top of the cars and which end in
grooved wheels, called _trolley-wheels_, are pressed by springs against
the trolley-wires. The current passes down these through switches to
_controllers_ at each end of the car, one set being used at a time.
[Illustration: Fig. 238.]
[Illustration: Fig. 239.]
=165. The Controllers=, as the name suggests, control the speed of the
car by allowing more or less current to pass through the motors. The
motors, resistance coils and controllers are so connected with each
other that the amount of current used can be regulated.
[Illustration: Fig. 240.]
[Illustration: Fig. 241.]
When the motorman turns the handle of the controller to the first
notch, the current passes through all of the resistance wires placed
under the car, then through one motor after the other. The motors being
joined in series by the proper connections at the controller, the
greatest resistance is offered to the current and the car runs at the
slowest speed at this first notch. As more resistance is cut out by
turning the handle to other notches, the car increases its speed; but
as the resistance wires become heated and the heat passes into the air,
there is a loss of energy. It is not economical to run a car at such a
speed that energy is wasted as heat. As soon as the resistance is all
cut out, the current simply passes through the motors joined in series.
This gives a fairly slow speed and one that is economical because all
the current tends to produce motion.
By allowing the current to pass through the motors joined in parallel,
that is, by allowing each to take a part of the current, the resistance
is greatly reduced, and a higher speed attained. This is not instantly
done, however, as too much strain would be put upon the motors. As soon
as the next notch is reached, the motors are joined in parallel and
the resistance also thrown in again. By turning the handle still more,
resistance is gradually cut out, and the highest speed produced when
the current passes only through the motors in parallel.
[Illustration: Fig. 242.]
[Illustration: Fig. 243.]
Fig. 238 represents a controller, by diagram, showing the relative
positions of the controller cylinder, reversing and cut-out cylinders,
arrangements for blowing out the short electric arcs formed, etc. A
ratchet and pawl is provided, which indicates positively the running
notches, at the same time permitting the cylinder to move with ease.
Fig. 239 shows a top view of the controller.
[Illustration: Fig. 244.]
=166. Overhead and Underground Systems.= When wires for furnishing
current are placed over the tracks, as in Fig. 237, we have the
overhead system. In cities the underground system is largely used.
The location of the conducting wires beneath the surface of the
street removes all danger to the public, and protects them from all
interference, leaving the street free from poles and wires.
Fig. 240 shows a cross-section of an underground conduit. The rails,
R R, are supported by cast-iron yokes, A, placed five feet apart, and
thoroughly imbedded in concrete. The conduit has sewer connections
every 100 feet. Conducting bars, C C, are placed on each side of
the conduit, and these are divided into sections of about 500 feet.
Insulators, D D, are placed every 15 feet. They are attached to, and
directly under, the slot-rails, the stem passing through the conductor
bar.
[Illustration: Fig. 245.]
Figs. 240 and 241 show the plow E. The contact plates are carried on
coiled springs to allow a free motion. Two guide-wheels, F F, are
attached to the leg of the plow. The conducting wires are carried up
through the leg of the plow.
=167. Appliances.= A large number of articles are needed in the
construction of electric railroads. A few, only, can be shown that are
used for the overhead system. Fig. 242 shows a pole insulator. Fig. 243
shows a feeder-wire insulator. Fig. 244 shows a line suspension. Fig.
245 shows a form of right-angle cross which allows the trolley-wheels
of crossing lines to pass. Fig. 246 shows a switch. In winter a part of
the current is allowed to pass through electric heaters placed under
the seats of electric cars.
[Illustration: Fig. 246.]
=168. Electric Boats= are run by the current from storage batteries
which are usually placed under the seats. An electric motor large
enough to run a small boat takes up very little room and is generally
placed under the floor. This leaves the entire boat for the use of
passengers. The motor is connected to the shaft that turns the screw.
Fig. 247 shows one design.
=169. Electric Automobiles= represent the highest type of electrical
and mechanical construction. The _running-gear_ is usually made of the
best cold-drawn seamless steel tubing, to get the greatest strength
from a given weight of material. The wheels are made in a variety of
styles, but nearly all have ball bearings and pneumatic tires. In the
lightest styles the wheels have wire spokes.
The _electric motors_, supported by the running-gear, are geared to
the rear wheels. The motors are made as nearly dust-proof as possible.
_Storage batteries_ are put in a convenient place, depending upon the
design of the carriage, and from these the motors receive the current.
These can be charged from the ordinary 110-volt lighting circuits or
from private dynamos. The proper plugs and attachments are usually
furnished by the various makers for connecting the batteries with the
street current, which is shut off when the batteries are full by an
automatic switch.
[Illustration: Fig. 247.]
_Controllers_ are used, as on electric cars, the lever for starting,
stopping, etc., being usually placed on the left-hand side of the seat.
The _steering_ is done by a lever that moves the front wheels. Strong
brakes, and the ability to quickly reverse the motors, allow electric
carriages to be stopped suddenly in case of accidents.
Electric automobiles are largely used in cities, or where the current
can be easily had. The batteries must be re-charged after they have
run the motors for a certain time which depends upon the speed and
road, as well as upon the construction. Where carriages are to be run
almost constantly, as is the case with those used for general passenger
service in cities, duplicate batteries are necessary, so that one or
two sets can be charged while another is in use. Fig. 248 shows one
form of electric vehicle, the storage batteries being placed under and
back of the seat.
[Illustration: Fig. 248.]
CHAPTER XXVI.
A WORD ABOUT CENTRAL STATIONS.
=170. Central Stations=, as the word implies, are places where, for
example, electricity is generated for the incandescent or arc lights
used in a certain neighborhood; where telephone or telegraph messages
are sent to be resent to some other station; where operators are kept
to switch different lines together, so that those on one line can
talk to those on another, etc., etc. There are many kinds of central
stations, each requiring a large amount of special apparatus to carry
on the work. Fig. 249 gives a hint in regard to the way car lines
get their power from a central power station. As a large part of the
apparatus required in ordinary central stations has already been
described, it is not necessary to go into the details of such stations.
[Illustration: Fig. 249.]
In lighting stations, for example, we have three principal kinds of
apparatus. Boilers produce the steam that runs the steam engines, and
these run the dynamos that give the current. Besides these there are
many other things needed. The electrical energy that goes over the
wires to furnish light, heat, and power, really comes indirectly from
the coal that is used to boil water and convert it into steam. The
various parts of the central station merely aid in this transformation
of energy.
[Illustration: Fig. 250.]
[Illustration: Fig. 251.]
The dynamos are connected to the engines by belts, or they are direct
connected. Figs. 250, 251, show dynamos connected to engines without
belts.
The current from the dynamos is led to large switchboards which contain
switches, voltmeters, ammeters, lightning arresters, and various other
apparatus for the proper control and measurement of the current. From
the switchboard it is allowed to pass through the various street mains,
from which it is finally led to lamps, motors, etc.
Water-power is frequently used to drive the dynamos instead of steam
engines. The water turns some form of water-wheel which is connected
to the dynamos. At Niagara Falls, for example, immense quantities of
current are generated for light, heat, power, and industrial purposes.
[Illustration]
CHAPTER XXVII.
MISCELLANEOUS USES OF ELECTRICITY.
=171. The Many Uses= to which the electric current is put are almost
numberless. New uses are being found for it every day. Some of the
common applications are given below.
=172. Automatic Electric Program Clocks=, Fig. 252, are largely used
in all sorts of establishments, schools, etc., for ringing bells at
certain stated periods. The lower dial shown has many contact-points
that can be inserted to correspond to given times. As this revolves,
the circuits are closed, one after the other, and it may be so set that
bells will be rung in different parts of the house every five minutes,
if desired.
[Illustration: Fig. 252.]
[Illustration: Fig. 253.]
=173. Call Boxes= are used to send in calls of various kinds to
central stations. Fig. 253 shows one form. The number of different
calls provided includes messenger, carrier, coupé, express wagon,
doctor, laborer, police, fire, together with three more, which may be
made special to suit the convenience of the individual customer. The
instruments are provided with apparatus for receiving a return signal,
the object of which is to notify the subscriber that his call has been
received and is having attention.
[Illustration: Fig. 254.]
[Illustration: Fig. 255.]
Fig. 254 shows another form of call box, the handle being moved around
to the call desired. As it springs back to the original position, an
interrupted current passes through the box to the central station,
causing a bell to tap a certain number of times, giving the call and
location of the box.
=174. Electric Gas-Lighters.= Fig. 255 shows a _ratchet burner_. The
first pull of the chain turns on the gas through a four-way gas-cock,
governed by a ratchet-wheel and pawl. The issuing gas is lighted by a
wipe-spark at the tip of the burner. Alternate pulls shut off the gas.
As the lever brings the attached wire A, in contact with the wire B,
a bright spark passes, which ignites the gas, the burner being joined
with a battery and induction or spark coil.
_Automatic burners_ are used when it is desired to light gas at
a distance from the push-button. Fig. 256 shows one form. Two
electromagnets are shown, one being generally joined to a white
push-button for turning on the gas and lighting it, the other being
joined to a black button which turns off the gas when it is pressed.
The armatures of the magnets work the gas-valve. Sparks ignite the gas,
as explained above.
[Illustration: Fig. 256.]
[Illustration: Fig. 257.]
=175. Door Openers.= Fig. 257 shows one form. They contain
electromagnets so arranged that when the armature is attracted by the
pushing of a button anywhere in the building, the door can be pushed
open.
=176. Dental Outfits.= Fig. 258 shows a motor arranged to run dental
apparatus. The motor can be connected to an ordinary incandescent light
socket. In case the current gives out, the drills, etc., can be run by
foot power.
[Illustration: Fig. 258.]
=177. Annunciators= of various kinds are used in hotels, factories,
etc., to indicate a certain room when a bell rings at the office.
The bell indicates that some one has called, and the annunciator
shows the location of the call by displaying the number of the room
or its location. Fig. 259 shows a small annunciator. They contain
electromagnets which are connected to push-buttons located in the
building, and which bring the numbers into place as soon as the current
passes through them.
[Illustration: Fig. 259.]
INDEX.
Numbers refer to paragraphs. See Table of Contents for the titles of
the various chapters.
Action of magnets upon each other, 32.
Adjuster, for lamp cords, 151.
Air pressure, effect of spark upon, 155.
Aluminum-leaf, for electroscopes, 5.
Alternating current, 129, 130;
system of wiring for, 144.
Amalgamation of zincs, 47.
Amber, electrification upon, 3.
Ammeter, the, 74;
how placed in circuit, 77.
Ampere, the, 72.
Annunciators, 177.
Anode, 79, 82.
Apparatus for electrical measurements, Chap. VI.
Appliances, for distribution of currents, 141;
for electric railways, 167;
for heating by electricity, 147.
Arc, the electric, 152.
Arc lamp, the, 153;
how light is produced by, Chap. XXII.;
double carbon, 153;
hand-feed focussing, 153;
for search-lights, 153;
short, for basements, 153;
single carbon, 153;
for theater use, 153.
Armature, of dynamo, 127, 129;
of electromagnets, 98;
of horseshoe magnet, 26;
of motors, 161;
uses of, 39.
Artificial magnets, 25.
Astatic, detectors, 94;
galvanometer, 73;
needles, 94.
Aurora borealis, 23.
Automatic, current interrupters, 104, 115;
gas lighters, 174;
program clocks, 172.
Automobiles, 169;
controllers for, 169;
motors for, 169;
steering of, 169;
storage batteries for, 169.
Bamboo filaments, 149.
Bar magnets, 27;
magnetic figures of, 38.
Batteries, large plunge, 54;
plunge, 53;
secondary, 86;
storage, and how they work, Chap. IX.
Bell, the electric, and some of its uses, Chap. XV.;
electric, 116;
magneto testing, 117;
trembling, etc., 116.
Bell transmitter, 120.
Belts, electricity generated by friction upon, 1.
Benjamin Franklin, 18.
Bichromate of potash cells, 51, etc.
Binding-posts, Chap. V.;
common forms of, 63.
Blasting, by electricity, 147;
electric machines for, 147.
Bluestone cell, 56.
Boats, electric, 168.
Boilers, use of in central stations, 170.
Bones, photographed by x-rays, Chap. XXIII.
Boosters, 136.
Brushes, 129.
Bunsen cells, 56_a_.
Burner, automatic, 174;
for gas-lights, 174;
ratchet, 174.
Buzzers, electric, 118.
Cables and wires, 143.
Call boxes, electric, 173.
Carbon, in arc lamps, 152, 153;
filament, 149;
transmitter, 123.
Carpet, electricity generated upon, 1.
Cars, electric, 164;
controllers for, 165;
heating by electricity, 167;
overhead system for, 166;
underground system for, 166.
Cat, electricity generated upon, 1.
Cathode, definition of, 79;
rays, 157.
Cells, Bunsen, 56_a_;
bichromate of potash, 51;
closed circuit, 50;
dry, 58;
Edison-Lelande, 59;
electricity generated by, Chap. III.;
Fuller, 55;
Gonda, 57;
gravity, 56;
Grenet, 52;
Leclanché, 57;
open circuit, 50;
plates and poles of, 45_a_;
polarization of, 48;
simple, 45, 49;
single-fluid, 49;
two-fluid, 49;
various voltaic, Chap. IV.
Central stations, 170;
a word about, Chap. XXVI.
Chain lightning, 19.
Chafing-dishes, electrical, 147.
Charging condensers, 15.
Chemical action, and electricity, 81.
Chemical effects of electric current, Chap. VII.
Chemical meters, 78.
Church organs, pumped by motors, 162.
Circuits, electric, 50;
for lamps, 144.
Cleats, porcelain, 141;
wooden, 141.
Clocks, automatic electric, 172.
Closed circuit cells, 50.
Coils, induction, and how they work, Chap. XIII.;
induction, construction of, 104;
method of joining, 98;
primary and secondary, 103;
resistance, 69;
rotation of, 95;
of transformers, 135.
Collectors on dynamos, 129.
Commutators, 129.
Compasses, magnetic, 31.
Compound, magnets, 28;
wound dynamo, 131.
Condensation of static electricity, 15.
Condensers, 15;
for induction coils, 104.
Conductors, and insulators, 4, 138.
Conduits, electric, 140.
Connections, electrical, 60;
for telegraph lines, 111.
Controllers, for automobiles, 169;
for electric cars, 165.
Copper sulphate, effects of current on, 82;
formula of, 79.
Copper voltameters, 75.
Cords, adjustable for lamps, 151.
Coulomb, the, 76.
Crater of hot carbons, 152.
Crookes tubes, 156, 158.
Current, detectors, 93;
direction of in cell, 46;
from magnet and coil, 100;
from two coils, 102;
induced, 127;
of induction coils, 105;
interrupters, automatic, 104, 115;
local, 47;
primary and secondary, 102;
transformation of, Chap. XVIII.;
transmission of, 134.
Currents, and motion, 160;
how distributed for use, Chap. XIX.
Current strength, 71;
measurement of, 73;
unit of, 72.
Cylinder electric machines, 9.
Daniell cell, 56.
D'Arsonval galvanometer, 73.
Declination, 41.
Decorative incandescent lamps, 151.
Dental, lamps, 151;
outfits, 176.
Detectors, astatic, 94;
current, 93.
Diamagnetic bodies, 29.
Diaphragm for telephones, 120.
Dip, of magnetic needle, 42.
Direct current, 129, 130.
Direction of current in cell, 46.
Discharging condensers, 15.
Disruptive discharges, 154.
Distribution of currents for use, Chap. XIX.
Door opener, electric, 175.
Dots and dashes, 110.
Drill press, run by motor, 162.
Dry cells, 58.
Dynamo, the, 126;
alternating current, 130;
commutator of, 129;
compound wound, 131;
direct current, 130;
lamps connected to, 132;
series wound, 131;
shunt wound, 131;
used as motor, 161;
use of in central stations, 170;
used with water power, 170.
Dynamos, electricity generated by, Chap. XVII.;
types of, 130;
various machines, 132;
winding of, 131.
Dynamotors, 137.
Earth, inductive influence of, 43;
lines of force about, 40, 42.
Ebonite, electricity by friction upon, 3, 4.
Edison-Lelande cells, 59.
Electric, automobiles, 169;
bell, and some of its uses, Chap. XV.;
boats, 168;
buzzers, 118;
cars, 164;
conduits, 140;
fans, 162;
flat-irons, 146;
gas lighters, 174;
griddles, 147;
kitchen, 147;
lights, arc, Chap. XXII.;
lights, incandescent, Chap. XXI.;
machines, static, 7 to 13;
machines, uses of, 14;
motor, the, 161;
motor, and how it does work, Chap. XXIV.;
soldering irons, 146;
telegraph, and how it sends messages, Chap. XIV.;
telephone, and how it transmits speech, Chap. XVI.;
welding, 146.
Electric current, and work, 133;
and chemical action, 81;
chemical effects of, Chap. VII.;
how distributed for use, Chap. XIX.;
magnetic effects of, Chap. XI.;
how transformed, Chap. XVIII.
Electrical, connections, 60;
horse-power, 77;
measurements, Chap. VI.;
resistance, 68;
resistance, unit of, 69;
units, Chap. VI.
Electricity, about frictional, Chap. I.;
and chemical action, 81;
atmospheric, 18;
heat produced by, Chap. XX.;
history of, 3;
how generated upon cat, 1;
how generated by dynamos, Chap. XVII.;
how generated by heat, Chap. X.;
how generated by induction, Chap. XII.;
how generated by voltaic cell, Chap. III.;
origin of name, 2.
Electrification, kinds of, 6;
laws of, 7.
Electrolysis, 79.
Electrolyte, 79.
Electromagnetic induction, 99.
Electromagnetism, 91.
Electromagnets, 96;
forms of, 97.
Electro-mechanical gong, 116.
Electromotive force, defined, 65, 71;
measurement of, 67;
of polarization, 85;
of static electricity, 17;
unit of, 66.
Electrophorus, the, 8.
Electroplating, 82.
Electroscopes, 5.
Electrotyping, 83.
Experiments, early, with currents, 44;
some simple, 1.
External resistance, 68.
Fan motors, 162.
Field, magnetic, 37.
Field-magnets, 129.
Figures, magnetic, 38.
Filaments, carbon, 149;
bamboo, etc., 149.
Fire, St. Elmo's, 22.
Flat-irons, electric, 147.
Floor mains, 139.
Fluoroscope, 158.
Force, and induced currents, 101;
lines of magnetic, 38;
lines of about a wire, 92, 96;
lines of about a magnet, 37, 38.
Frictional electricity, about, Chap, I.;
location of charge of, 4;
sparks from, 4.
Fuller cell, the, 55.
Fuse, link, 142;
plug, 142;
ribbons, 142;
wire, 142.
Fusible rosettes, 142.
Galvani, early experiments of, 44.
Galvanometers, 73;
astatic, 73;
considered as motor, 161;
D'Arsonval, 73;
tangent, 73.
Galvanoscope, 73;
astatic, 94.
Gas lighters, electric, 174.
Geissler tubes, 156.
Generators, electric, 126.
Glass, electricity generated upon, 4.
Glue pots, electric, 147.
Gold-leaf, for electroscopes, 5.
Gold plating, 82.
Gonda cell, 57.
Gong, electro-mechanical, 116.
Gravity cell, the, 56;
replaced by dynamotors, 137.
Grenet cell, 52.
Griddles, electric, 147.
Guard, for lamps, 151.
Heat, how generated by electricity, Chap. X.;
and magnetism, 35;
and resistance, 145.
Heat lightning, 19.
Heaters, for cars, 167.
History of electricity, 3.
Horse-power, electrical, 77.
Horseshoe, permanent magnets, 26;
electromagnets, 97, 98.
Human body, bones of, photographed by x-rays, Chap. XXIII.
Hydrogen, action of in cell, 48;
attraction of for oxygen, 85.
Incandescence, 148.
Incandescent lamp, 149;
candle-power of, 150;
current for, 150;
light produced by, Chap. XXI.;
construction of, 149;
uses of, 151.
Inclination of magnetic needle, 42.
Indicating push-button, 61.
Induced currents, 127;
and lines of force, 101;
by rotary motion, 128;
of induction coils, 105;
of transformers, 135.
Induced magnetism, 36.
Induction, electricity generated by, Chap. XII.;
electromagnetic, 99.
Induction coils, condensers for, 104;
construction of, 104;
currents of, 105;
how they work, Chap. XIII.;
in telephone work, 124;
uses of, 106.
Inductive influence of earth, 43.
Influence machines for medical purposes, 13.
Ink writing registers, 114.
Insulating tubing, 141.
Insulators, 141;
and conductors, 4, 138;
feeder-wire, 167;
for poles, 167;
porcelain, 141.
Internal resistance, 68.
Interrupters, automatic current, 104, 115.
Ions, 80.
Iron, electricity upon, by friction, 4.
Jar, Leyden, 15.
Jarring magnets, effects of, 33.
Keeper of magnets, 26.
Keys, telegraph, 109.
Kinds of electrification, 6.
Kitchen, electric, 147.
Knife switch, 62.
Lamp, incandescent, candle-power of, 150;
cord, adjustable, 151;
current for, 150;
dental, 151;
for desks, 151;
for throat, 151;
guard for, 151;
incandescent, 149;
socket, 151;
with half shade, 151.
Lamp, the arc, 153;
how light is produced by, Chap. XXII.;
double carbon, 153;
hand-feed focussing, 153;
for search-lights, 153;
single carbon, 153;
short, for basements, 153;
for theater use, 153.
Lamp circuits, alternating system, 144.
Lamps, in parallel, 144;
lamps in series, 144;
three-wire system, 144;
two-wire system, 144.
Laws, of electrification, 7;
of magnetic attraction, 32;
of resistance, 70.
Leaf electroscopes, 5.
Leclanché cell, 57.
Leyden, battery, 16;
jar, 15.
Light, how produced by arc lamp, Chap. XXII.;
how produced by incandescent lamp, Chap. XXI.
Lightning, 19;
rods, 21.
Line, telegraph, Chap. XIV.;
connections for, 111;
operation of, 112.
Line suspension, for trolley-wires, 167.
Line wire, 111.
Lines of force, conductors of, 39, 96;
about the earth, 40, 42;
and induced currents, 101;
about a magnet, 38;
about a wire, 92.
Local currents, 47.
Magnetic, bodies, 29;
declination, 41;
effects of electric current, Chap. XI.;
field, 37;
figure of one bar magnet, 38;
figure of two bar magnets, 38;
figure of horseshoe magnet, 38;
needle, dip of, 42;
needles and compasses, 31.
Magnetism, and heat, 35;
induced, 36;
laws of, 32;
residual, 34;
retentivity, 34;
temporary, 36;
terrestrial, 40;
theory of, 33.
Magneto, signal bells, 117;
testing bells, 117;
transmitter, 120.
Magnets, action upon each other, 32;
artificial, 25;
bar, 27;
compound, 28;
effects of jarring, 33;
electro, 96;
electro, forms of, 97;
horseshoe, 26;
and magnetism, about, Chap. II.;
making of, 30;
natural, 24.
Mains, electric, 139.
Man-holes, in conduits, 140.
Measurements, electric, Chap. VI.;
of current strength, 73;
of E.M.F., 67.
Meters, chemical, 78;
permanent record, 77.
Microphone, the, 122.
Motion and currents, 160.
Motor, acting like dynamo, 163;
armature of, 161;
controlling speed of, 165;
electric, 161;
electric, and how it does work, Chap. XXIV.;
fans, 162;
for automobiles, 169;
for boats, 168;
for pumping bellows, 162;
for running drill press, 162;
parts of, 162;
starting boxes for, 163;
uses of, 162.
Motor-dynamos, 136.
Mouldings, for wires, 141.
Name, electricity, origin of, 2.
Natural magnets, 24.
Needles, astatic, 94;
dipping, 42;
magnetic, 31.
Negative electrification, 5.
Non-conductors, 4.
North pole, magnetic of earth, 40;
of magnets, 26.
Northern lights, 23.
Ohm, the, 69.
Open circuit cells, 50.
Openers, for doors, 175.
Outfits, dental, 175.
Overhead trolley system, 166.
Oxygen, attraction for hydrogen, 85.
Parallel arrangement of lamps, 144.
Peltier effect, 89.
Pendant, electric, 151.
Pith-ball electroscope, 5.
Plate electrical machine, 10.
Plates of cells, 45_a_.
Plunge batteries, 53;
large, 54.
Polarity of coils, 95.
Polarization, 84;
electromotive force of, 85;
of cells, 48.
Pole-changing switch, 62.
Poles, of cells, 45_a_;
of horseshoe magnet, 26.
Positive electrification, 6.
Potential, defined, 65.
Push-buttons, Chap. V.;
indicating, 61;
modifications of, 61;
table clamp, 61.
Quantity of electricity, 76;
unit of, 76.
Rays, cathode, 157;
x-rays, 158.
Receiver, telephone, 121.
Reflectors, for lamps, 151.
Registers, ink writing, 114.
Relay, the, 113.
Residual magnetism, 34.
Resistance, coils and boxes, 69;
electrical, 68;
external, 68;
and heat, 145;
internal, 68;
laws of, 70;
unit of, 69.
Retentivity, 34.
Risers, in buildings, 139.
Rods, lightning, 21.
Roentgen, Prof., 158.
Rosette, fusible, 142.
Running-gear, of automobiles, 169.
Safety, devices, 142;
fuse, 142;
fuse link, 142;
fuse plug, 142;
fuse ribbon, 142;
fuse wire, 142.
Search-lights, 153;
signals sent by, 153.
Secondary batteries, 86;
uses of, 87.
Series arrangement of lamps, 144.
Series wound dynamo, 131.
Service wires, 139.
Shunt-wound dynamo, 131.
Signal bells, magneto, 117.
Simple cell, the, 45, 49.
Single-fluid cells, 49.
Single-point switch, 62.
Single-stroke bell, 116.
Socket, for incandescent lamps, 151.
Soldering irons, electric, 147.
Sounders, telegraph, 110;
home-made, 110.
Spark, effect of air pressure on, 155.
Sparks, from cells, 17;
from frictional electricity, 4.
St. Elmo's fire, 22.
Starting boxes, for motors, 163.
Static electric machines, 8.
Static electricity, condensation of, 15;
electromotive force of, 17;
to test presence of, 5;
uses of, 14.
Steam engines, in central stations, 170.
Steel, inductive influence of earth upon, 43;
retentivity of, 26.
Storage batteries, the, and how they work, Chap. IX.;
for automobiles, 169;
for boats, 168;
for natural sources of power, 87.
Stoves, electric, 147.
Strength of current, 71;
measurement of, 73;
unit of, 72.
Switchboards, 62.
Switches, Chap. V.;
knife, 62;
pole-changing, 62;
single point, 62;
for trolley lines, 167.
Table clamp-push, 61.
Tangent galvanometer, 73.
Teakettles, electric, 147.
Telegraph, electric, and how it sends messages, Chap. XIV.;
ink writing registers, 114;
keys, 109;
relay, 113;
sounders, 110.
Telegraph line, 107, 108;
operation of, 112;
simple connections of, 111.
Telephone, the, and how it transmits speech, Chap. XVI.;
receiver, 121;
transmitter, 120;
use of induction coil with, 124;
various forms of, 125.
Temporary magnetism, 36.
Terrestrial magnetism, 40.
Theory of magnetism, 33.
Thermoelectricity, 88.
Thermopiles, 90.
Three-wire system, 144.
Throat, lamp for, 151.
Thunder, 20.
Toepler-Holtz machines, 11.
Transformers, 135.
Transforming electric current, Chap. XVIII.;
for electric welding, 146.
Transmission of currents, 134.
Transmitter, Bell, 120;
carbon, 123.
Trembling bell, 116.
Trolley-wires, 164;
-poles, 164;
-wheels, 164.
Tubes, Crookes, 156, 158;
Geissler, 156;
vacuum, 156.
Two-fluid cells, 49.
Two-wire system, 144.
Underground trolley system 166;
conduits for, 166.
Unit, of current strength, 72;
of electromotive force, 66;
of quantity, 76;
of resistance, 69.
Units, electrical, Chap. VI.
Uses, of armatures, 39;
of electricity, miscellaneous, Chap. XXVII.;
of induction coils, 106;
of motors, 162;
of storage batteries, 87.
Vacuum-tubes, 156.
Variation, angle of, 41.
Volt, the, 66.
Volta, 66;
early experiments of, 44.
Voltaic cell, electricity generated by, Chap. III.
Voltaic pile, 44.
Voltameters, 75;
copper, 75;
water, 75.
Voltmeters, 67, 77.
Water, decomposition of, 79;
power, source of energy, 170;
voltameters, 73.
Watt, the, 77.
Wattmeters, 77.
Welding, electric, 146.
Wimshurst electric machine, 12.
Wires and cables, 143.
Wiring, for alternating system, 144;
three-wire system, 144;
two-wire system, 144.
Work, and electric current, 133.
X-ray photographs, 159.
X-rays, 156;
and how the bones of the human body are photographed, Chap. XXIII.
Yokes, 97, 98.
Zincs, amalgamation of, 47.
THINGS A BOY SHOULD KNOW ABOUT ELECTRICITY.
By THOMAS M. ST. JOHN, Met. E.
The book contains 180 pages, and 260 illustrations; it measures
5 x 7½ in., and is bound in cloth.
PRICE, POST-PAID, $1.00.
=CONTENTS:= _Chapter_ I. About Frictional Electricity.--II.
About Magnets and Magnetism.--III. How Electricity
is Generated by the Voltaic Cell.--IV. Various
Voltaic Cells.--V. About Push-Buttons, Switches and
Binding-Posts.--VI. Units and Apparatus for Electrical
Measurements.--VII. Chemical Effects of the Electric
Current.--VIII. How Electroplating and Electrotyping are
Done.--IX. The Storage Battery and How it Works.--X. How
Electricity is Generated by Heat.--XI. Magnetic Effects of
the Electric Current.--XII. How Electricity is Generated
by Induction.--XIII. How the Induction Coil Works.--XIV.
The Electric Telegraph, and How it Sends Messages.--XV. The
Electric Bell and Some of its Uses.--XVI. The Telephone,
and How it Transmits Speech.--XVII. How Electricity
is Generated by Dynamos.--XVIII. How the Electric
Current is Transformed.--XIX. How Electric Currents are
Distributed for Use.--XX. How Heat is Produced by the
Electric Current.--XXI. How Light is Produced by the
Incandescent Lamp.--XXII. How Light is Produced by the Arc
Lamp.--XXIII. X-Rays, and How the Bones of the Human Body
are Photographed.--XXIV. The Electric Motor and How it Does
Work.--XXV. Electric Cars, Boats and Automobiles.--XXVI. A
Word About Central Stations.--XXVII. Miscellaneous Uses of
Electricity.
This book explains, in simple, straightforward language, many things
about electricity; things in which the American boy is intensely
interested; things he wants to know; things he should know.
It is free from technical language and rhetorical frills, but it tells
how things work, and why they work.
It is brimful of illustrations--the best that can be had--illustrations
that are taken directly from apparatus and machinery, and that show
what they are intended to show.
This book does not contain experiments, or tell how to make apparatus;
our other books do that. After explaining the simple principles of
electricity, it shows how these principles are used and combined to
make electricity do every-day work.
_Everyone Should Know About Electricity._
A VERY APPROPRIATE PRESENT
THIRD EDITION
How Two Boys Made Their Own Electrical Apparatus.
Containing complete directions for making all kinds of
simple electrical apparatus for the study of elementary
electricity. By PROFESSOR THOMAS M. ST. JOHN, New York City.
The book measures 5 × 7½ in., and is beautifully bound in
cloth. It contains 141 pages and 125 illustrations. Complete
directions are given for making 152 different pieces of
Apparatus for the practical use of students, teachers, and
others who wish to experiment.
PRICE, POST-PAID, $1.00.
The shocking coils, telegraph instruments, batteries, electromagnets,
motors, etc., etc., are so simple in construction that any boy of
average ability can make them; in fact, the illustrations have been
made directly from apparatus constructed by young boys.
The author has been working along this line for several years, and he
has been able, _with the help of boys_, to devise a complete line of
simple electrical apparatus.
=_THE APPARATUS IS SIMPLE because the designs and methods
of construction have been worked out practically in the
school-room, absolutely no machine-work being required._=
=_THE APPARATUS IS PRACTICAL because it has been designed
for real use in the experimental study of elementary
electricity._=
=_THE APPARATUS IS CHEAP because most of the parts can be
made of old tin cans and cracker boxes, bolts, screws, wires
and wood._=
=Address, THOMAS M. ST. JOHN,=
=407 West 51st Street,=
=New York.=
How Two Boys Made Their Own Electrical Apparatus.
=CONTENTS:= _Chapter_ I. Cells and Batteries.--II. Battery Fluids
and Solutions.--III. Miscellaneous Apparatus and Methods of
Construction.--IV. Switches and Cut-Outs.--V. Binding-Posts and
Connectors.--VI. Permanent Magnets,--VII. Magnetic Needles and
Compasses.--VIII. Yokes and Armatures.--IX. Electro-Magnets.--X.
Wire-Winding Apparatus.--XI. Induction Coils and Their
Attachments.--XII. Contact Breakers and Current Interrupters.--XIII.
Current Detectors and Galvanometers.--XIV. Telegraph Keys and
Sounders.--XV. Electric Bells and Buzzers.--XVI. Commutators and
Current Reversers.--XVII. Resistance Coils.--XVIII. Apparatus for
Static Electricity.--XIX. Electric Motors.--XX. Odds and Ends.--XXI.
Tools and Materials.
"The author of this book is a teacher and wirier of great ingenuity,
and we imagine that the effect of such a book as this falling into
juvenile hands must be highly stimulating and beneficial. It is
full of explicit details and instructions in regard to a great
variety of apparatus, and the materials required are all within the
compass of very modest pocket-money. Moreover, it is systematic and
entirely without rhetorical frills, so that the student can go right
along without being diverted from good helpful work that will lead
him to build useful apparatus and make him understand what he is
about. The drawings are plain and excellent. We heartily commend the
book."--_Electrical Engineer._
"Those who visited the electrical exhibition last May cannot have
failed to notice on the south gallery a very interesting exhibit,
consisting, as it did, of electrical apparatus made by boys. The
various devices there shown, comprising electro-magnets, telegraph keys
and sounders, resistance coils, etc., were turned out by boys following
the instructions given in the book with the above title, which is
unquestionably one of the most practical little works yet written that
treat of similar subjects, for with but a limited amount of mechanical
knowledge, and by closely following the instructions given, almost any
electrical device may be made at very small expense. That such a book
fills a long-felt want may be inferred from the number of inquiries
we are constantly receiving from persons desiring to make their own
induction coils and other apparatus."--_Electricity._
"At the electrical show in New York last May one of the most
interesting exhibits was that of simple electrical apparatus made by
the boys in one of the private schools in the city. This apparatus,
made by boys of thirteen to fifteen years of age, was from designs
by the author of this clever little book, and it was remarkable to
see what an ingenious use had been made of old tin tomato-cans,
cracker-boxes, bolts, screws, wire, and wood. With these simple
materials telegraph instruments, coils, buzzers, current detectors,
motors, switches, armatures, and an almost endless variety of apparatus
were made, In this book Mr. St. John has given directions in simple
language for making and using these devices, and has illustrated
these directions with admirable diagrams and cuts. The little volume
is unique, and will prove exceedingly helpful to those of our young
readers who are fortunate enough to possess themselves of a copy. For
schools where a course of elementary science is taught, no better
text-book in the first-steps in electricity is obtainable."--_The Great
Round World._
Exhibit of Experimental Electrical Apparatus
AT THE ELECTRICAL SHOW, MADISON SQUARE GARDEN, NEW YORK.
While only 40 pieces of simple apparatus were shown in this exhibit, it
gave visitors something of an idea of what young boys can do if given
proper designs.
[Illustration: "HOW TWO BOYS MADE THEIR OWN ELECTRICAL APPARATUS"
Gives Proper Designs--Designs for over 150 Things.]
Fun With Photography
BOOK AND COMPLETE OUTFIT.
[Illustration]
=PHOTOGRAPHY= is now an educational amusement, and to many it is the
most fascinating of all amusements. The magic of sunshine, the wonders
of nature, and the beauties of art are tools in the hand of the amateur
photographer.
A great many things can be done with this outfit, and it will give an
insight into this most popular pastime.
=THE OUTFIT= contains everything necessary for making
ordinary prints--together with other articles to be used
in various ways. The following things are included:
One Illustrated Book of Instructions, called "Fun With
Photography;" 1 Package of Sensitized Paper; 1 Printing
Frame, including Glass, Back, and Spring; 1 Set of Masks for
Printing Frame; 1 Set of Patterns for Fancy Shapes; 1 Book
of Negatives (Patent Pending) Ready for Use; 6 Sheets of
Blank Negative Paper; 1 Alphabet Sheet; 1 Package of Card
Mounts; 1 Package of Folding Mounts; 1 Package of "Fixo."
=CONTENTS OF BOOK:=--=Chapter I.
Introduction.=--Photography.--Magic Sunshine.--The
Outfit.--=II. General Instructions.=--The
Sensitized Paper.--How the Effects are
Produced.--Negatives.--Prints.--Printing Frames.--Our
Printing Frame.--Putting Negatives in Printing
Frame.--Printing.--Developing.--Fixing.--Drying.--Trimming.--Fancy
Shapes.--Mounting.--=III. Negatives and How to Make
Them.=--The Paper.--Making Transparent Paper.--Making
the Negatives.--Printed Negatives.--Perforated
Negatives.--Negatives Made from Magazine Pictures.--Ground
Glass Negatives.--=IV. Nature Photography.=--Aids
to Nature Study.--Ferns and Leaves.--Photographing
Leaves.--Perforating Leaves.--Drying Leaves, Ferns,
etc., for Negatives.--Flowers.--=V. Miscellaneous
Photographs.=--Magnetic Photographs.--Combination
Pictures.--Initial Pictures.--Name Plates.--Christmas,
Easter and Birthday Cards.
_The Book and Complete Outfit will be sent, by mail or
express, Charges Prepaid, upon receipt of 65 Cents, by_
=THOMAS M. ST. JOHN, 407 W. 51st St., New York.=
Fun With Magnetism.
BOOK AND COMPLETE OUTFIT FOR SIXTY-ONE EXPERIMENTS IN MAGNETISM...
[Illustration]
Children like to do experiments; and in this way, better than in any
other, _a practical knowledge of the elements of magnetism_ may be
obtained.
These experiments, although arranged to _amuse_ boys and girls, have
been found to be very _useful in the class-room_ to supplement the
ordinary exercises given in text-books of science.
To secure the _best possible quality of apparatus_, the horseshoe
magnets were made at Sheffield, England, especially for these sets.
They are new and strong. Other parts of the apparatus have also been
selected and made with great care, to adapt them particularly to these
experiments.--_From the author's preface._
=CONTENTS.=--Experiments With Horseshoe Magnet.--Experiments
With Magnetized Needles.--Experiments With Needles,
Corks, Wires, Nails, etc.--Experiments With Bar
Magnets.--Experiments With Floating Magnets.--Miscellaneous
Experiments.--Miscellaneous Illustrations showing what very
small children can do with the Apparatus.--Diagrams showing
how Magnetized Needles may be used by little children to
make hundreds of pretty designs upon paper.
=AMUSING EXPERIMENTS.=--Something for Nervous People to
Try.--The Jersey Mosquito.--The Stampede.--The Runaway.--The
Dog-fight.--The Whirligig.--The Naval Battle.--A
String of Fish.--A Magnetic Gun.--A Top Upsidedown.--A
Magnetic Windmill.--A Compass Upsidedown.--The Magnetic
Acrobat.--The Busy Ant-hill.--The Magnetic Bridge.--The
Merry-go-Round.--The Tight-rope Walker.--A Magnetic Motor
Using Attractions and Repulsions.
_The Book and Complete Outfit will be sent, Post-paid,
upon receipt of 35 Cents, by_
=THOMAS M. ST. JOHN, 407 W. 51st St., New York.=
FUN WITH SHADOWS
BOOK AND COMPLETE OUTFIT FOR SHADOW PICTURES, PANTOMIMES,
ENTERTAINMENTS, Etc., Etc.
[Illustration]
=Shadow Making= has been a very popular amusement for several
centuries. There is a great deal of _fun_ and instruction in it, and
its long life is due to the fact that it has always been a source of
keen delight to grown people as well as to children.
In getting material together for this little book, the author has been
greatly aided by English, French and American authors, some of whom are
professional shadowists. It has been the author's special effort to get
the subject and apparatus into a practical, cheap form for boys and
girls.
=THE OUTFIT= contains everything necessary for all ordinary
shadow pictures, shadow entertainments, shadow plays, etc.
The following articles are included:
One book of Instructions called "Fun with Shadows"; 1 Shadow
Screen; 2 Sheets of Tracing Paper; 1 Coil of Wire for
Movable Figures; 1 Cardboard Frame for Circular Screen; 1
Cardboard House for Stage Scenery; 1 Jointed Wire Fish-pole
and Line; 2 Bent Wire Scenery Holders; 4 Clamps for Screen;
1 Wire Figure Support; 1 Wire for Oar; 2 Spring Wire Table
Clamps; 1 Wire Candlestick Holder; 5 Cardboard Plates
containing the following printed figures that should be cut
out with shears: 12 Character Hats; 1 Boat; 1 Oar-blade; 1
Fish; 1 Candlestick; 1 Cardboard Plate containing printed
parts for making movable figures.
=CONTENTS OF BOOK:= One Hundred Illustrations and Diagrams,
including Ten Full-page Book Plates, together with Six
Full-page Plates on Cardboard.
_Chapter_ I. Introduction.--II. General Instructions.--III.
Hand Shadows of Animals.--IV. Hand Shadows of Heads,
Character Faces, etc.--V. Moving Shadow Figures and How
to Make Them.--VI. Shadow Pantomimes.--VII. Miscellaneous
Shadows.
_The Book and Complete Outfit will be sent, =POST-PAID=,
upon receipt of 35 cents, by_
=THOMAS M. ST. JOHN, 407 West 51st St., New York City.=
Fun With Electricity.
BOOK AND COMPLETE OUTFIT FOR SIXTY EXPERIMENTS IN ELECTRICITY....
[Illustration]
Enough of the principles of electricity are brought out to make the
book instructive as well as amusing. The experiments are systematically
arranged, and make a fascinating science course. No chemicals, no
danger.
The book is conversational and not at all "schooly," Harry and Ned
being two boys who perform the experiments and talk over the results as
they go along.
"The book reads like a story."--"An appropriate present for a
boy or girl."--"Intelligent parents will appreciate 'Fun With
Electricity.'"--"Very complete, because it contains both book and
apparatus."--"There is no end to the fun which a boy or girl can have
with this fascinating amusement."
=THERE IS FUN IN THESE EXPERIMENTS.=--Chain Lightning.--An
Electric Whirligig.--The Baby Thunderstorm.--A Race
with Electricity.--An Electric Frog Pond.--An Electric
Ding-Dong.--The Magic Finger.--Daddy Long-Legs.--Jumping
Sally.--An Electric Kite.--Very Shocking.--Condensed
Lightning.--An Electric Fly-Trap.--The Merry Pendulum.--An
Electric Ferry-Boat.--A Funny Piece of Paper.--A Joke on the
Family Cat.--Electricity Plays Leap-Frog.--Lightning Goes
Over a Bridge.--Electricity Carries a Lantern.--And _=40
Others=_.
The =_OUTFIT_= contains 20 different articles. The =_BOOK
OF INSTRUCTION=_ measures 5 x 7½ inches, and has 38
illustrations, 55 pages, good paper and clear type.
_The Book, and Complete Outfit will be sent, by mail or
express, Charges Prepaid, upon receipt of 65 Cents, by_
=THOMAS M. ST. JOHN, 407 W. 51st St., New York.=
Fun With Puzzles.
BOOK, KEY, AND COMPLETE OUTFIT FOR FOUR HUNDRED PUZZLES...
The BOOK measures 5 × 7½ inches. It is well printed, nicely bound,
and contains 15 chapters, 80 pages, and 128 illustrations. The KEY is
illustrated. It is bound with the book, and contains the solution of
every puzzle. The COMPLETE OUTFIT is placed in a neat box with the
book. It consists of numbers, counters, figures, pictures, etc., for
doing the puzzles.
=CONTENTS:= _Chapter_ (1) Secret Writing. (2) Magic
Triangles, Squares, Rectangles, Hexagons, Crosses, Circles,
etc. (3) Dropped Letter and Dropped Word Puzzles. (4) Mixed
Proverbs, Prose and Rhyme. (5) Word Diamonds, Squares,
Triangles, and Rhomboids. (6) Numerical Enigmas. (7)
Jumbled Writing and Magic Proverbs. (8) Dissected Puzzles.
(9) Hidden and Concealed Words. (10) Divided Cakes, Pies,
Gardens, Farms, etc. (11) Bicycle and Boat Puzzles. (12)
Various Word and Letter Puzzles. (13) Puzzles with Counters.
(14) Combination Puzzles. (15) Mazes and Labyrinths.
"Fun With Puzzles" is a book that every boy and girl should have. It
is amusing, instructive,--educational. It is just the thing to wake up
boys and girls and make them think. They like it, because it is real
fun. This sort of educational play should be given in every school-room
and in every home.
"Fun With Puzzles" will puzzle your friends, as well as yourself; it
contains some real brain-splitters. Over 300 new and original puzzles
are given, besides many that are hundreds of years old.
=Secret Writing.= Among the many things that "F. W. P." contains, is
the key to _secret writing_. It shows you a very simple way to write
letters to your friends, and it is simply impossible for others to read
what you have written, unless they know the secret. This, alone is a
valuable thing for any boy or girl who wants to have some fun.
_The Book, Key, and Complete Outfit will be sent, postpaid,
upon receipt of 35 cents, by_
=THOMAS M. ST. JOHN, 407 West 51st St., New York City.=
Fun With Soap-Bubbles.
BOOK AND COMPLETE OUTFIT FOR FANCY BUBBLES AND FILMS....
[Illustration]
=THE OUTFIT= contains everything necessary for thousands of beautiful
bubbles and films. All highly colored articles have been carefully
avoided, as cheap paints and dyes are positively dangerous in
children's mouths. The outfit contains the following articles:
One Book of Instructions, called "Fun With Soap-Bubbles," 1 Metal Base
for Bubble Stand, 1 Wooden Rod for Bubble Stand, 3 Large Wire Rings for
Bubble Stand, 1 Small Wire Ring, 3 Straws, 1 Package of Prepared Soap,
1 Bubble Pipe, 1 Water-proof Bubble Horn. The complete outfit is placed
in a neat box with the book. (Extra Horns, Soap, etc., furnished at
slight cost.)
=CONTENTS OF BOOK.=--Twenty-one
Illustrations.--Introduction.--The Colors of
Soap-bubbles.--The Outfit.--Soap Mixture.--Useful
Hints.--Bubbles Blown With Pipes.--Bubbles Blown
With Straws.--Bubbles Blown With the Horn.--Floating
Bubbles.--Baby Bubbles.--Smoke Bubbles.--Bombshell
Bubbles.--Dancing Bubbles.--Bubble Games.--Supported
Bubbles.--Bubble Cluster.--Suspended Bubbles.--Bubble
Lamp Chimney.--Bubble Lenses.--Bubble Basket.--Bubble
Bellows.--To Draw a Bubble Through a Ring.--Bubble
Acorn.--Bubble Bottle.--A Bubble Within a Bubble.--Another
Way.--Bubble Shade.--Bubble Hammock.--Wrestling
Bubbles.--A Smoking Bubble.--Soap Films.--The Tennis
Racket Film.--Fish-net Film.--Pan-shaped Film.--Bow and
Arrow Film.--Bubble Dome.--Double Bubble Dome.--Pyramid
Bubbles.--Turtle-back Bubbles.--Soap-bubbles and Frictional
Electricity.
"There is nothing more beautiful than the airy-fairy soap-bubble with
its everchanging colors."
_THE BEST POSSIBLE AMUSEMENT FOR OLD
AND YOUNG._
_The Book and Complete Outfit will be sent, =POST-PAID=,
upon receipt of 35 cents, by_
=THOMAS M. ST. JOHN, 407 West 51st St., New York City.=
The Study of Elementary Electricity and
Magnetism by Experiment.
By THOMAS M. ST. JOHN, Met. E.
The book contains 220 pages and 168 illustrations;
it measures 5 × 7½ in. and is bound in green cloth.
PRICE, POST-PAID, $1.25.
This book is designed as a text-book for amateurs, students, and others
who wish to take up a systematic course of elementary electrical
experiments at home or in school. Full directions are given for.......
_Two Hundred Simple Experiments._
The experiments are discussed by the author, after the student has been
led to form his own opinion about the results obtained and the points
learned.
In selecting the apparatus for the experiments in this book, the author
has kept constantly in mind the fact that the average student will not
buy the expensive pieces usually described in text-books.
The two hundred experiments given can be performed with
simple apparatus; in fact, the student should make at least
a part of his own apparatus, and for the benefit of those
who wish to do this, the author has given, throughout the
work, explanations that will aid in the construction of
certain pieces especially adapted to these experiments. For
those who have the author's "How Two Boys Made Their Own
Electrical Apparatus," constant references have been made to
it as the "Apparatus Book," as this contains full details
for making almost all kinds of simple apparatus needed
in "The Study of Elementary Electricity and Magnetism by
Experiment."
_If you wish to take up a systematic course of experiments--experiments
that may be performed with simple, inexpensive apparatus,--this book
will serve as a valuable guide._
Condensed List of Apparatus
FOR
"The Study of Elementary Electricity and Magnetism by Experiment."
_Number_ 1. Steel Needles; package of twenty-five.--2. Flat Cork.--3.
Candle.--4-15. Annealed Iron Wires; assorted lengths.--16. Horseshoe
Magnet; best quality; English.--17. Iron Filings.--18. Parts for
Compass.--19, 20. Wire Nails; soft steel.--21, 22. Spring Steel; for
bar magnets.--23. Iron Ring.--24. Sifter; for iron filings.--25.
Spring Steel; for flexible magnet.--26, 27. Ebonite Sheets; with
special surface.--28. Ebonite Rod.--29. Ebonite Rod; short.--30.
Flannel Cloth.--31. Tissue Paper.--32. Cotton Thread.--33. Silk
Thread.--34. Support Base.--35. Support Rod.--36. Support Wire.--37.
Wire Swing.--38. Sheet of Glass.--39. Hairpin.--40. Circular
Conductor.--41. Circular Conductor.--42. Electrophorus Cover.--43.
Insulating Table.--44. Insulated Copper Wire.--45. Rubber Band.--46.
Bent Wire Clamps.--47. Cylindrical Conductor.--48. Discharger; for
condenser.--49. Aluminum-Leaf.--50. Wires.
51. Dry Cell.--52. Mercury.--53. Insulated Copper Wire; for
connections.--54. Spring Connectors; two dozen.--55. Parts
for Key.--56. Metal Connecting Plates.--57. Parts for Current
Reverser.--58. Parts for Galvanoscope.--59. Parts for Astatic
Galvanoscope.--60-63. Zinc Strips.--64. Carbon Rod.--65, 66. Glass
Tumblers.--67, 68. Copper Strips.--69. Galvanized Iron Nail.--70,
71. Wooden Cross-Pieces.--72. Brass Screws; one dozen.--73. Porous
Cup.--74. Zinc Rod.--75. Copper Plate.--76. Iron Strip.--77, 78. Lead
Strips.--79. Parts for Resistance Coil.--80. Parts for Wheatstone's
Bridge.--81. German-Silver Wire; Size No. 30.--82. German-Silver Wire;
No. 28.--83--85. Plate Binding-Posts.--86. Copper Sulphate.--87. Copper
Burs; one dozen.--88. Combination Rule.--89. Coil of Wire; on spool
for electromagnet.--90. Coil of Wire; on spool for electromagnet.--91.
Carbon Rod.--92, 93. Soft Iron Cores with Screws.--94. Combined
Base and Yoke.--95. Combination Connecting Plates.--96. Long Iron
Core.--97. Round Bar Magnet, 5 × 3/8 in.--98. Thin Electromagnet.--99.
Degree-Card; for galvanoscope.--100. Scale for Bridge.--101, 102. Soft
Iron Cores with Heads.--103, 104. Flat Bar Magnets; these are 6 × ½ × ¼
in.; highly polished steel; poles marked.--105. Compass.
=_Illustrated Price Catalogue upon Application._=
Electrical Apparatus For Sale
A COMPLETE ELECTRIC AND MAGNETIC CABINET FOR STUDENTS, SCHOOLS AND
AMATEURS. SIX EXTRAORDINARY OFFERS
=This Cabinet of Electrical Experiments= contains three main parts:
(_A_) Apparatus; (_B_) Text-Book; (_C_) Apparatus List.
(_A_) =The Apparatus= furnished consists of one hundred and five
pieces. Over three hundred separate articles are used in making up this
set. Most of it is ready for use when received. Seven pieces, however,
are not assembled; but the parts can be readily finished and put
together. (Sold, also, _all_ pieces assembled.)
(_B_) =The Text-Book=--called "The Study of Elementary Electricity
and Magnetism by Experiment"--gives full directions for two hundred
experiments. (See table of contents, etc.) Price, post-paid, $1.25.
(_C_) =The Apparatus List= is an illustrated book devoted entirely to
this special set of apparatus. Not given with first offer.
_THE APPARATUS IS SIMPLE because the designs and methods of
construction have been worked out with great care._
_THE APPARATUS IS PRACTICAL because it has been designed
for real use in "The Study of Elementary Electricity and
Magnetism by Experiment."_
_THE APPARATUS IS CHEAP because the various parts are
so designed that they can be turned out in quantity by
machinery._
=1st Offer:= Pieces 1 to 50 $1.00
=2d Offer:= Pieces 51 to 105, with part (_C_) 3.50
=3d Offer:= Pieces 1 to 105, with part (_C_) 4.00
=4th Offer:= Complete Cabinet, parts (_A_), (_B_), (_C_) 5.00
=5th Offer:= Apparatus only, all pieces assembled 4.60
=6th Offer:= Complete Cabinet, all pieces assembled 5.60
=_Express charges must be paid by you. Estimates given._=
A "Special Catalogue," pertaining to the above, with complete
price-list, will be mailed upon application.
=THOMAS M. ST. JOHN, 407 West 51st St., New York City=
Fun With Telegraphy
BOOK AND COMPLETE OUTFIT.
[Illustration]
=TELEGRAPHY= is of the greatest importance to all civilized nations,
and upon it depend some of the world's most important enterprises.
Every boy and girl can make practical use of telegraphy in one way or
another, and the time it takes to learn it will be well spent.
=THE OUTFIT.=--Mr. St. John has worked for a number of years to produce
a telegraph outfit that would be simple, cheap, and practical for those
who wish to make a study of telegraphy. After making and experimenting
with nearly one hundred models, many of which were good, he has at last
perfected an instrument so simple, original, and effective that it is
now being made in large quantities.
The sounders are so designed that they will work properly with any dry
cell of ordinary strength, and this is a great advantage for practice
lines. Dry batteries are cheap and clean, and there are no dangers from
acids.
The outfit consists of the following articles, placed in a neat box:
One Book of Instruction, called "Fun With Telegraphy"; one Telegraph
"Key"; one Telegraph "Sounder"; Insulated Copper Wires for connections.
The "key" and "sounder" are mounted, with proper "binding-posts," upon
a base of peculiar construction, which aids in giving a large volume of
sound.
=CONTENTS OF BOOK.=--Telegraphy.--The Outfit.--A Complete Telegraph
Line.--Connections.--The Telegraph Key.--The Sounder.--The Battery.--A
Practice Line.--A Two-instrument Line.--Operation of Line.--The Morse
Telegraph Alphabet.--Aids to Learning Alphabet.--Cautions.--Office
Calls.--Receiving Messages.--Remember.--Extra Parts.
=ABOUT BATTERIES.=--For those who cannot easily secure batteries, we
will furnish small dry cells, post-paid, at 15 cents each, in order to
deliver the outfits complete to our customers. This price barely covers
the total cost to us, postage alone being 6 cents.
_=FUN WITH TELEGRAPHY, including Book, Key, Sounder,
and Wire (no battery), post-paid, 50 cents, by=_
=THOMAS M. ST. JOHN, 848 Ninth Ave., New York=
Tool Sets for Students
The following tool sets have been arranged especially for those who
wish to make use of the designs contained in "How Two Boys Made Their
Own Electrical Apparatus," "Real Electric Toy-Making for Boys,"
"Electric Instrument-Making," etc. It is very poor economy to waste
valuable time and energy in order to save the cost of a few extra tools.
=NOTE.=--Save money by buying your tools in sets. We do not pay express
or freight charges at the special prices below.
=FOR $1.00.=--One _Steel Punch_; round, knurled head.--One light
_Hammer_; polished, nickel-plated, varnished handle.--One _Iron Clamp_;
japanned, 2¼ in.--One _Screw-Driver_; tempered and polished blade,
cherry stained hardwood handle, nickel ferrule.--One _Wrench_; retinned
skeleton frame, gilt adjusting wheel.--One _Awl_; tempered steel
point, turned and stained wood handle, with ferrule.--One _Vise_; full
malleable, nicely retinned, 1-3/8 in. jaws, full malleable screw with
spring.--One pair _Steel Pliers_; 4 in. long, polished tool steel,
unbreakable, best grooved jaw.--One pair of _Shears_; carbonized steel
blades, hardened edge, nickel-plated, heavy brass nut and bolt.--One
_File_; triangular, good steel.--One _File Handle_; good wood, brass
ferrule.--One _Foot Rule_; varnished wood, has English and metric
system.--One _Soldering Set_; contains soldering iron, solder, resin,
sal ammoniac, and directions. One _Center-Punch_; finely tempered steel.
=FOR $2.00.=--All that is contained in the $1.00 set of tools, together
with the following: One pair of _Tinner's Shears_; cut, 2¾ in., cast
iron, hardened, suitable for cutting thin metal.--One _Hollow Handle
Tool Set_; very useful; polished handle holds 10 tools, gimlet,
brad-awls, chisel, etc.--One _Try Square_; 6-in. blue steel blade,
marked in 1/8s, strongly riveted.--One 1-lb. _Hammer_; full size,
polished head, wedged varnished hardwood handle.--One _Hack Saw_; steel
frame, 9½-in. polished steel blade, black enamel handle; very useful.
=FOR $3.50.=--Two _Steel Punches_; different sizes, one solid round,
knurled head, polished; the other, point and head brightly polished,
full nickel, center part knurled.--One _Light Hammer_; polished and
nickel plated, varnished handle.--One regular _Machinist's Hammer_;
ball peen, solid cast steel, with varnished hardwood handle; a
superior article.--Two _Iron Clamps_; one opens 2¼ in., the other
3 in., japanned.--One _Screw-Driver_; tempered and polished blade,
firmly set in cherry stained hardwood handle with nickel ferrule.--One
_Wrench_; retinned, skeleton frame, gilt adjusting wheel.--One _Awl_;
tempered steel blade, ground to point, firmly set in turned and stained
handle with ferrule.--One _Steel Vise_; 2¼-in., jaws, steel screw,
bright polished jaws and handle; a good strong vise.--One pair of
_Steel Pliers_; 6 in. long, bright steel, flat nose, 2 wire-cutters,
practically unbreakable.--One pair of _Shears_; carbonized steel
blades, hardened edges, nickel plated, heavy brass nut and bolt.--One
_File_; triangular and of good steel.--One _File Handle_; good wood,
with brass ferrule.--One _Foot Rule_; varnished wood, has both the
English and metric systems.--One _Soldering Set_; contains soldering
iron, solder, resin, sal ammoniac, and directions; a very handy
article.--One _Center-Punch_; finely tempered steel.--One pair of
_Tinner's Shears_; these are best grade, inlaid steel cutting edges,
polished and tempered, japanned handles; thoroughly reliable.--One
_Hollow Handle Tool Set_; very useful; the polished handle holds 10
tools, gimlet, chisel, brad-awl, etc.--One _Try Square_; 6-in. blue
steel blade, marked both sides in 1/8s, strongly riveted with brass
rivets.--One _Hack Saw_; steel frame, 9½-in. polished steel blade,
black enamel handle; very useful for sawing small pieces of wood.
=FOR $5.00= will be included everything in the $3.50 offer, and the
following: One _Glue-Pot_; medium size, with brush and best wood
glue; inside pot has hinge cover.--One _Ratchet Screw-Driver_; great
improvement over ordinary screw-drivers; well made and useful.--One
_Hand Drill_; frame malleable iron; hollow screw top holding 6 drills;
bores from 1-16 to 3-16-in. holes; solid gear teeth; 3-jawed nickel
plated chuck; a superior tool, and almost a necessity.
=GIVE THE BOY A SET OF TOOLS=
=THOMAS M. ST. JOHN, 848 Ninth Ave., New York=
REAL ELECTRIC TOY-MAKING FOR BOYS
_By_ THOMAS M. ST. JOHN, Met. E.
This book contains 140 pages and over one hundred
original drawings, diagrams, and full-page plates.
It measures 5 x 7½ in., and is bound in cloth.
Price, post-paid, $1.00
=CONTENTS:= _Chapter_ I. Toys Operated by Permanent Magnets.--II.
Toys Operated by Static Electricity.--III. Making Electromagnets for
Toys.--IV. Electric Batteries.--V. Circuits and Connections.--VI. Toys
Operated by Electromagnets. VII. Making Solenoids for Toys.--VIII.
Toys Operated by Solenoids.--IX. Electric Motors.--X. Power,
Speed, and Gearing.--XI. Shafting and Bearings.--XII. Pulleys and
Winding-Drums.--XIII. Belts and Cables.--XIV. Toys Operated by
Electric Motors.--XV. Miscellaneous Electric Toys.--XVI. Tools.--XVII.
Materials.--XVIII. Various Aids to Construction.
While planning this book, Mr. St. John definitely decided that he would
not fill it with descriptions of complicated, machine-made instruments
and apparatus, under the name of "Toy-Making," for it is just as
impossible for most boys to get the parts for such things as it is
for them to do the required machine work even after they have the raw
materials.
Great care has been taken in designing the toys which are described
in this book, in order to make them so simple that any boy of average
ability can construct them out of ordinary materials. The author can
personally guarantee the designs, for there is no guesswork about
them. Every toy was made, changed, and experimented with until it was
as simple as possible; the drawings were then made from the perfected
models.
As the result of the enormous amount of work and experimenting which
were required to originate and perfect so many new models, the author
feels that this book may be truly called "Real Electric Toy-Making for
Boys."
=Every Boy Should Make Electrical Toys.=
The Electric Shooting Game>
A MOST ORIGINAL AND FASCINATING GAME PATENT APPLIED FOR AND COPYRIGHTED
[Illustration]
_=SHOOTING BY ELECTRICITY=_
=The Electric Shooting Game= is an entirely new idea, and one that
brings into use that most mysterious something--_electricity_. The
game is so simple that small children can play it, and as there are
no batteries, acids, or liquids of any kind, there is absolutely no
danger. The electricity is of such a nature that it is perfectly
harmless--but very active.
The "_game-preserve_" is neat and attractive, being printed in colors,
and the birds and animals are well worth hunting. Each has a fixed
value--and some of them must not be shot at all--so there is ample
opportunity for a display of skill in bringing down those which count
most.
"_Electric bullets_" are actually shot from the "_electric gun_" by
electricity. This instructive game will furnish a vast amount of
amusement to all.
_=The "Game-Preserve,"--the "Electric Gun,"--the
"Shooting-Box,"--the "Electric Bullets,"--in fact, the
entire electrical outfit, together with complete illustrated
directions, will be sent in a neat box, Post-Paid, upon
receipt of 50 cents, by=_
=THOMAS M. ST. JOHN, 848 Ninth Ave., New York=
* * * * *
Transcriber's note:
Obvious punctuation errors were corrected.
Page 46, "turnnd" changed to "turned" (be turned to 1)
Page 66, word "a" added to text (in a glass jar)
***END OF THE PROJECT GUTENBERG EBOOK THINGS A BOY SHOULD KNOW ABOUT
ELECTRICITY***
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