Induction coils, Ruhmkorff coils, and transformers, to be described

later, are closely related to this. They all create magnetic fields in

the same way and are all electro-magnets.

[Illustration: Fig. 64. Transformers]

VII

ELECTRIC HEATING

It was Washington's birthday. The schools were to have a holiday and

the Science Club was to hold a special, open meeting at which I had

been asked to present the subject of electricity in the household. I

replied to the programme committee that that was too large a subject,

but that I would talk upon electric heating. I warned them, however,

that it would be a dry study, and not an entertainment. They replied

that the father of his country had been born at a time of the year

when the weather was unfavourable to outdoor sports, and that February

usually found them acclimated to vigorous study. Neither they nor their

friends objected to study if it seemed to have a motive.

I found an audience composed of old and young, men and women, girls and

boys. Most of them had left school--many of them because their teachers

thought they were incompetent to continue.

[Illustration: Fig. 65]

Not far from here is "a wheel in the middle of a wheel ... as for their

rings they are so high that they are dreadful ... and the spirit of the

living creature is in the wheels." Those wheels are now sending the

electric current to this room for our experiments. I propose to show

that we convert electricity into heat by offering resistance to its

flow. Experience teaches us that resistance to motion always produces

heat. At Niagara Falls thousands of tons of water descend at the rate

of one hundred and sixty feet in three seconds. When the water reaches

the bottom of the falls, it is moving a little faster than a mile a

minute. The resistance which this mass meets after its fall retards its

motion and generates heat.

Hundreds of meteors fall into our atmosphere daily, travelling a

thousand times as fast as the waters of Niagara Falls. The resistance

to their motion, which our atmosphere offers, heats them white hot,

melts them, vaporizes them, burns them up, so that very few of them

reach the solid earth in a solid condition.

An iron spile driver, measuring two cubic feet, weighs about half a

ton. When it falls sixteen feet upon the end of a spile it is moving

at the rate of twenty miles an hour. The energy of this moving mass

depends upon both its weight and its velocity, and when its motion is

arrested by the spile that energy of motion is largely converted into

heat energy, from which both the spile and the spile driver get hot.

A piece of iron may be made red hot by pounding it with a trip hammer.

Count Rumford found, in 1798, while boring cannon in the arsenal at

Munich, that the resistance which the iron offered to the motion of the

boring tool furnished heat enough to boil water.

Seven hundred and seventy-eight foot pounds of mechanical energy when

converted into heat would raise one pound of water (one pint) one

degree. This is called the British thermal unit. The spile driver,

weighing 1000 pounds, falling 16 feet upon a spile, produces heat

enough to raise 1 pint of water 20 degrees.

[Illustration: Fig. 66]

Here are two binding posts, _a_ and _b_, 8 feet apart (Fig. 66),

connected by copper wires with the dynamo circuit. The volt meter

indicates 112 volts of pressure. I will close the circuit by stretching

between _a_ and _b_ 8 feet of No. 24 iron wire. (This wire is about the

thickness of a common pin.) The iron wire offers resistance to the flow

of the electric current, thereby producing heat--heat enough as you see

to make the wire white hot, indeed heat enough to raise it to something

over two thousand degrees Fahr., for now you see it has melted.

We will put in a fresh piece of wire and connect also the ammeter

in the circuit (Fig. 67). As I close the circuit the needle of the

ammeter at first indicates 20 or 30 amperes, but in a second drops to

8 amperes, and remains there a second until the wire melts and falls

apart. One hundred and twelve volts of electric pressure are able to

push 8 amperes of electricity through this wire when hot.

[Illustration: Fig. 67]

(112 volts)/(14 ohms) = 8 amperes

112 volts × 8 amperes = 896 watts

746 watts = one horse-power

Hence it required about one and one fifth horse-power to melt the wire

in a second, and the heat produced was a little less than one British

thermal unit, a unit much used by engineers.

1 pound raised 1 foot = 1 foot pound

550 foot pounds per second = 1 horse-power

778 foot pounds (1.4 H.-P.) = 1 B. T. U. (British thermal unit) =

heat required to raise 1 pound of water 1° Fahrenheit

1 volt × 1 ampere = 1 watt

746 watts = 1 horse-power

In order to hold back 112 volts of electric pressure so that not more

than eight amperes of electricity should pass, the iron wire must have

offered about 14 ohms of resistance.

The behaviour of the ammeter needle showed that the wire offered very

much less resistance when cold than when hot. Indeed eight feet of No.

24 iron wire offers about one and one third ohms resistance when cold,

hence heat had increased its resistance to the passage of the electric

current tenfold.

This piece of iron wire offered resistance to the flow of the electric

current. It offered resistance to the motion of the dynamo. This

offered resistance to the steam-engine which drives the dynamo. This

caused the governor of the engine to open and pass more steam from

the boiler. This reduced the pressure at the steam gauge. This caused

the fireman to shovel more coal into the furnace. The heat of the

burning coal melts the wire, but it does it only after several changes.

First, it is converted into mechanical energy in the steam-engine with

great loss--about nine tenths being lost. Second, it is converted

into electrical energy by the dynamo, with some loss, and, third, it

is conducted to the iron wire and converted back to heat with still

further loss. It is evident that the most economical way to heat the

wire would be to take it to the furnace. Yet all electric cooking is

done by sending electric current through wires embedded in the walls of

the cooking utensils, and it is the most wasteful method of using the

energy stored in coal that has yet been devised.

[Illustration: Fig. 68]

That merely connecting the binding posts _a_ and _b_ (Fig. 67) by a

small piece of wire should throw a load upon the dynamo miles away;

should offer resistance to its motion, and make it require 1.18

horse-power more of energy to keep up its speed of revolution, is,

indeed, uncanny. I will attempt to make it seem more real. At one end

of the lecture table I have a rotary pump _P_ (Fig. 68). The end of

the rubber tube _a_, which leads to the pump is lying upon the table

outside of the tank of water, _T_. While things are in this condition

I move the crank which operates the pump with perfect ease. Now while

still turning the crank I pick up the tube _a_ and drop its free end

into the water tank. I cannot now conceal the fact, even if I were

disposed to do so, that I must work hard to keep the pump going. The

pump itself tells you by its laboured sound that it is working hard,

and the stream of water which issues from the pipe _b_ tells how much

work I am performing. The pump is discharging five and a half pints of

water per second, that is 5.5 pounds, and it raises this water 10 feet.

Hence I am doing 55 foot pounds of work per second, which requires

one tenth of a horse-power. Here is a lad who consents to try the

experiment for us. He turns the crank easily while I am holding the

tube _a_ out of the water, but when I lower it into the water he finds

the resistance so great that, tug however much he may, he is unable to

keep the pump going.

At the other end of the table I have a small hand dynamo, _D_ (Fig.

68), _M_ is an ammeter, _V_ is a volt meter, _S_ is a switch. All the

wires are good-sized copper, and offer little resistance, except that

stretched between the binding posts _a_ and _b_. This is a piece of

fine German silver wire. While the switch is open I turn the crank

of the dynamo with perfect ease. A small amount of current is going

through the volt meter, but this is too slight to offer any perceptible

resistance to the motion of the machine.

Notice that the volt meter needle moves according to the speed of

revolution. If I turn the crank once a second the needle stands at

25 volts. The electric pressure increases or decreases according to

whether I rotate the armature faster or slower. Now I will attempt

to keep the machine revolving at a constant rate while I close the

switch _S_, and surely you must see that I have hard work to do so. The

wire _a b_ has now become red hot. The volt meter shows 25 volts of

pressure, and the ammeter shows 3 amperes of current.

Twenty-five volts × 3 amperes = 75 watts, which require one tenth of

a horse-power (746 watts = 1 horse-power). The lad now takes my place

at turning the machine and finds it easy when the switch is open, but

I actually overload him by merely closing the switch. Heating the wire

red hot requires more energy than he is able to put forth.

I proposed to the president that my lecture close at this point, and

that each one in the room have a chance to _feel_ the load which was

thrown upon the dynamo each time it was required to heat the wire.

I suggested that each person should get a realizing sense of this

fact, first by doing the work himself, and second by going home and

reflecting upon this hint. When the switch is closed three amperes of

electricity pass around the circuit. This increases the magnetism in

both the field and the armature of the dynamo, and it requires one

tenth of a horse-power more to keep the armature moving within the

field against this magnetic pull.

I further desired to announce that during this hour I had delivered to

them the second key to the Electrical Show which I had promised a few

days ago. The second key is:

Heat (and light) is produced by offering resistance to the flow of the

electric current. The first key is the electro-magnet. These two unlock

all the mysteries of the show.

The president closed the formal exercises with the facetious remark

that I had warned them before the lecture that they must work, so now

each would be expected to take a turn at the cranks of the pump and

dynamo.

VIII

APPLICATIONS OF ELECTRIC HEATING

The programme committee decided that each member of the Science Club

should busy himself looking for _applications of electric heating_ and

should consult me freely about the matter. My telephone was kept busy,

my laboratory was in great demand, and we were all getting a good deal

more education than the school was giving us credit for.

The boys generally came to me in pairs, and each pair having worked up

some illustration of heat produced by electricity reported it to the

club. These were spread by the secretary in due form upon the minutes

of the club and constituted "The Proceedings of the Science Club."

[Illustration: Fig. 69]

1. _The Electric Sad Iron_ (Fig. 69).--Removing three screws the iron

comes apart, revealing a lot of No. 24 German silver wire wound upon a

sheet of mica. This is put between other sheets of mica (Fig. 70) and

tucked away within the body of the iron. German silver offers about

twice the resistance of iron when it is cold, but, at the temperature

of the sad iron when in use, there is not much difference between the

resistance of the two metals. German silver wire, however, does not

rust as iron wire would, and hence it is chosen. German silver is an

alloy of copper, zinc, and nickel.

[Illustration: Fig. 70]

We put the 112-volt current upon this wire of the iron, and according

to the ammeter it passed 4 amperes. Its resistance must therefore have

been 28 ohms.

(112 volts)/(28 ohms) = 4 amperes

Electricity costs us about 10 cents per kilowatt hour. That is 10

cents for 1000 watts for an hour, or 1 cent for a hundred watts for an

hour, or, on a 100-volt current, 1 cent for an ampere for an hour. It,

therefore, costs about 4 cents or, more accurately, 4-1/2 cents an hour

to heat this iron.

Persons sometimes carry electric irons with them, when they travel, to

iron pocket handkerchiefs and other small articles while stopping at

a hotel. Before connecting an iron in a chandelier one must know the

voltage used in the building. If the voltage in use in the building is

not the same as that stamped upon the iron, it is not safe to connect

it. Not knowing this, many persons have had the embarrassment of

"blowing a fuse" and extinguishing their own lights, and perhaps those

of others in the same building, and very likely also ruining the iron.

Suppose we take for example this iron stamped _110 V; 400 Watts_. (A

slight variation of 5 or 10 volts will not injure an iron.) The wire in

this iron we found to offer about 28 ohms resistance when hot, and it

lets pass 4 amperes. This is about all the current which it is able to

carry without melting. Now suppose a 220-volt current is used in the

building where it is proposed to connect the iron. This would force

through the wire enough current to melt it. The wire was seen to be

at a very dull-red heat when examined in a dark room. Its temperature

was about nine hundred degrees. At this temperature its resistance is

about three times what it is when cold. We estimated by measurements

that the iron contained about twenty-five feet of the wire. The boys

then took twenty-five feet of No. 24 German silver wire and stretched

it between two nails driven up in the laboratory (Fig. 71, _a b_). The

dynamo current was then sent through this. The end, _c_, of the wire

from the dynamo was provided with a metal clip which could be slid

along on the German silver wire. Sliding this to the left, and thus

shortening the distance on the German silver wire through which the

current must pass, increased the amount of current and heated the wire

hotter. The resistance decreases as the wire is shortened.

[Illustration: Fig. 71]

The boys wound this wire upon a piece of asbestos board (Fig. 72),

about nine inches square and one eighth of an inch thick, taking

care to keep the successive turns half an inch apart. Asbestos paper

was wrapped around this. The two ends of the wire were left free for

connections. This they called a "hot plate."

[Illustration: Fig. 72]

2. _Electric Hot Plate_ (Fig. 73).--This when opened was found to have

wire coiled up inside in the same manner as the sad iron. Indeed the

sad iron supported bottom side up makes a perfectly good hot plate.

The particular hot plate which we examined had a three-point switch

which gave three different heats for the plate. (See Fig. 74.) When the

switch _S_ is upon the first point the current goes through 112 ohms of

resistance and 1 ampere passes:

(112 volts)/(112 ohms) = 1 ampere

[Illustration: Fig. 73]

[Illustration: Fig. 74]

This warms the plate slightly--enough to keep food warm which has been

already cooked. This costs about one cent an hour.

When the switch is placed upon the second point the current goes

through 56 ohms of resistance and 2 amperes pass.

(112 volts)/(56 ohms) = 2 amperes.

This makes the plate warmer and is adapted to certain cooking

processes. It costs about two cents an hour.

When the switch is placed upon the third point the current goes through

28 ohms of resistance and 4 amperes pass.

(112 volts)/(28 ohms) = 4 amperes.

[Illustration: Fig. 75]

We placed upon this hot plate a basin containing 1 pint of water

(equals 1 pound) and heated it from the temperature of the room (68

degrees) to boiling (212 degrees) in 7 minutes and then put an egg in

and boiled it 3 minutes. Using 4 amperes for 10 minutes cost two thirds

of a cent. If it takes 7 minutes to boil a pint of water it would

require 1 hour to boil a gallon upon this hot plate using 4 amperes, or

448 watts. That is, it costs us about 4.5 cents a gallon to boil water

by electricity. The cost is usually put at three and a half cents per

gallon, but much depends upon conditions.

3. _Traveller's Cooker_ (Fig. 75).--This consists of a hot plate with a

covered basin permanently attached to it.

4. _Electric Coffee Percolator_ (Fig. 76) consists of a hot plate

with a coffee percolator to sit upon it. The coffee percolator might

sit upon any other hot plate or this hot plate might serve any other

purpose, but people do not seem to think of that.

[Illustration: Fig. 76]

5. _Electric Chafing-Dish_ (Fig. 77) consists merely of an electric hot

plate with a chafing-dish attached. The electric coffee percolators and

chafing dishes require from 300 to 600 watts according to size. If used

on the 110-volt current they take about 3 to 6 amperes, and if adapted

to the 220-volt current they take from 1-1/2 to 3 amperes, but cost the

same to operate in either case. They have connected with them flexible

cords and plugs to screw into the lamp sockets.

[Illustration: Fig. 77]

6. _Electric Broilers_ are merely hot plates, generally corrugated to

conduct off the melted fat. One that we examined had a switch for three

heats: low, requiring 360 watts--costs 3.6 cents per hour; medium,

requiring 600 watts--cost 6 cents per hour; high, requiring 1280

watts--cost 12.8 cents per hour.

7. _Electric Oven._--This one has double walls to retain the heat and

has two large hot plates, one on the bottom and one on the top. It is

large enough to hold four loaves of bread. It required 1520 watts for

40 minutes to heat it to the baking temperature and one hour to bake

the bread. Hence the cost of the electricity is about 25 cents, about

what the bread would cost in the market.

8. _Electric Incubator._--This is simply a well-ventilated oven warmed

by an electric hot plate and automatically controlled so that it keeps

a constant temperature of 103 degrees. Under these conditions chickens

hatch from hens' eggs in three weeks. An incubator for 5 dozen eggs was

found to take 25 cents' worth of electricity for the whole process of

incubation.

9. _Electric Toaster._--The wire coiled up in sad irons and hot plates

becomes hot enough to scorch cloth and paper, and even set fire to them

if they come in direct contact. We proved this by opening the iron and

touching paper to the wire while it was carrying the current. We also

lighted a cigar by touching it to the wire. Electric toasters have the

hot German silver wire simply covered by a screen.

10. _Electric Cigar Lighters_ (Fig. 78).--The one we examined hung by

a flexible cord from the chandelier. It had a small disk on the side

which contained a lot of fine wire covered by perforated mica. The wire

became red hot when the push button in the handle was pressed. It took

half an ampere of 110-volt current, and operated only while the button

was pushed. As near as we could calculate it cost .0003 of a cent to

light a cigar.

[Illustration: Fig. 78]

[Illustration: Fig. 79]

11. _Electric Curling Iron_ (Fig. 79).--One who has flat hair needs no

curling iron, but those who have round hair may curl it temporarily, if

they will unscrew an electric light bulb and screw into its socket the

plug of an electric curling iron. The flexible cord contains two wires

insulated from each other. One of these wires is attached to the outer

shell of the plug, the other wire is attached to the central button of

the plug. These make connections with the two separate dynamo wires in

the socket. The current comes down one of the wires in the flexible

cord, passes through a coil of fine German silver wire inside of the

curling iron, and returns by the other wire in the flexible cord. The

small wire in the curling iron offers 220 ohms of resistance when hot

and passes half an ampere of the 110-volt current.

(110 volts)/(220 ohms) = .5 ampere.

12. _Electric Soldering Irons_ (Fig. 80).--Or coppers, as they should

be called, are ideal implements for soldering. They remain continually

at the proper temperature and are free from corrosion. They require

from 55 to 220 watts. On the 110-volt current they take from one half

to two amperes.

[Illustration: Fig. 80]

13. _Electric Heating Pad_ (Fig. 81).--This consists of resistance

wire inside of a pad of soft material. It maintains a temperature of

180 degrees, and is an excellent substitute for a hot water bag. It

contains about two hundred and twenty ohms of resistance and requires

the same current as a 16-candle-power lamp.

[Illustration: Fig. 81]

14. _Electric Fuses_ (Fig. 82).--Fuses are made of short pieces of wire

or thin sheet metal. The metal is an alloy of lead and tin which melts

at a low temperature. They derive their name from the fact that they

readily fuse or melt. A building is wired in various separate circuits.

The size of the copper wires used in each circuit is determined by the

amount of current which the circuit is expected to carry. Each circuit

is protected by one or more fuses. These melt and cut off the current

whenever too much passes for the copper conductor to carry without

getting hot. The fuse wire melts at about six hundred degrees, while

the copper will not melt until it reaches nearly two thousand degrees.

This temperature is sufficient to set fire to wood, paper, and cloth.

When any fuse melts, the current is cut off from all chandeliers,

etc., in the particular circuit controlled by the fuse. This produces

consternation among people who do not understand the function of a

fuse. They become panic-stricken and begin to trample their neighbours

to death in the theatre or on the electric train when they hear that a

fuse is "blown" (which is the electrician's way of saying that it has

melted). Everyone should know that a fuse is a safety device. It is

always enclosed in a box lined with sheet iron or asbestos, so that it

is impossible for the flash, which occurs when the circuit is broken,

to set fire to anything.

[Illustration: Fig. 82]

[Illustration: Fig. 83]

15. _Electric Gas Lighter_ (Fig. 83).--These usually have two or three

small, dry battery cells in the handle. By pushing a button in the

handle connection is made between this battery and a short piece of

resistance wire in the tip. This wire gets red hot and lights the gas.

It is a surprise to many that we can light illuminating gas without

bringing a flame to it, and it is equally surprising that some flames,

or at least sparks, may not be able to light the gas. The fact is that

it is wholly a matter of _temperature and kind of gas_. Iron heated to

dull red will not light the illuminating gas now being furnished in

New York City, while iron at a bright red heat will do so. Iron may be

hot enough to light illuminating gas but too cool to light gasolene

vapour, which requires a dazzling white heat. Iron which is just under

the temperature at which it gives any light may set fire to wood and

paper. After it has cooled a good deal below that, it will set fire to

sulphur, and when it has cooled so that one may hold it in the hand,

it is still hot enough to set fire to phosphorus. The glowing end of

a lighted cigar, the spark made by striking flint, or the spark from

a spark coil with a feeble battery, all fail to set fire to gasolene

vapour, simply because they are not hot enough.

Fresh battery cells must occasionally be put in the handle of the

electric gas lighter.

Four facts regarding the resistance of wires it is well to remember:

1. The longer the wire the more resistance it offers to the electric

current.

2. The smaller the diameter of the wire the more resistance it offers.

3. Some materials offer more resistance than others, for example, iron

about six times as much as copper and German silver about twelve times

as much as copper.

4. The common metals offer more resistance when hot than when cold,

about double the resistance when heated to five hundred degrees. It is

the reverse with carbon, which offers more resistance when cold than

when hot. The carbon filament lamp offers about double the resistance

when cold as when lighted to full brilliancy.

The Library of Work and Play: Electricity and Its Everyday Uses · 第 4 / 15 段