Here is the "Electricity - Basic Navy Training Courses" (NAVPERS 10622) in its
entirety. It should provide one of the Internet's best resources for people
seeking a basic electricity course - complete with examples worked out. See
Table of Contents.
¶ U.S. GOVERNMENT PRINTING OFFICE; 1945 - 618779
ELECTRICITY IN MOTION - CURRENT
(* VERY IMPORTANT NOTE:
Current flow here is defined as from negative to positive, which is
opposite of today's convention. Modern convention of positive-to-negative
current flow, with negative-to-positive electron flow requires a
"right-hand rule." See
page on RF Cafe).
Fresh water must be carried to many parts of a ship. It is fed to the
boilers, to the laundry, to the galleys, to the scuttlebutts, and to the heads. The water system is complicated-it
requires pumps and many pipe lines to do its job. The electrical system is very much like the water system.
Electricity must be "piped" to the lighting circuits, to the interior communications circuits, to the battle
circuits, and on some ships, to the propulsion circuits. The "pipes" of an electrical circuit are METAL WIRES and
the "'pumps" are the GENERATORS.
Current flowing through a wire is surprisingly like water flowing in a
pipe. If you were to put an electron into one end of a piece of copper wire, this added electron would unbalance
the charges of the molecules in the wire and would act as a repelling force on the nearest electron in the wire.
(Actually, the added electron gives one end of the wire a higher POTENTIAL than the other end.) The push by the
added electron breaks one electron away from the nucleus of the FIRST molecule and forces it on to the SECOND
molecule. The electron you put in the end of the wire then fills the empty space left in the first molecule. Now
the electron expelled from the first molecule forces an electron out of the second molecule and into the THIRD
molecule - and so on through the whole length of the Wire.
Figure 11. - Electron flow in a conductor.*
When this shifting of electrons reaches the last molecule in the wire, you have, in effect, transported one
electron the entire length of the wire. Not the same electron you started with-but, since electrons are all alike
anyway, you can say that there has been a FLOW of one electron through the wire. Figure 11 enormously magnifies
the mechanism of this moving electron. You know that ONE electron by itself is not enough electricity to be of any
use. In an actual circuit, there would be billions upon billions of moving electrons.
Measuring the size of a waterfall seems easy-if you merely say it's large or small. Actually, however, there's
more to it than meets the eye. First of all, you've got to have a UNIT OF MEASURE. Drops, ounces, pints, quarts,
gallons, or barrels are all quantity measuring units for a liquid. You'd select the one unit that fits the problem
best-neither too small nor too large. "Gallons" might do the trick.
With the unit of
measure-gallons-selected, IS it possible to determine the SIZE of a waterfall if you're told ONLY THE NUMBER OF
GALLONS spilling? How about this: "Niagara has 5,000,000 gallons of water falling." Exactly how much do you learn
from that statement? Not much! Sure, 5,000,000 gallons is a lot of water, but you must also know HOW LONG it takes
to spill that much. One year, one month, one week, one day, or one hour! Not much of a falls, if it takes a year.
But you know Niagara is a roaring giant, and the 5,000,000 gallons are spilled in ONE HOUR.
The point is,
you must know TWO things in order to measure the size or strength of a waterfall-the number of MEASURING UNITS
moving in a UNIT OF TIME. This is called TIME RATE OF FLOW. Flow of water is commonly measured in GALLONS PER
SECOND, but it could be measured in "quarts per second" or "barrels per day."
That takes care of a water system-now, how is "flow" measured in an electrical system? First, select a unit of
quantity measure. The electron won't do as a unit because it's much too small. A larger unit-made up of' 6.3
billion billions of , electrons-is the COULOMB. And the coulomb is the standard electrical UNIT OF QUANTITY
Coulombs ALONE can no more measure the STRENGTH of electrical current than can the gallon ALONE
measure the strength of a waterfall. In order to measure electrical strength, coulombs (quantity) must be hooked
up with TIME. COULOMBS PER SECOND correspond to gallons per second. And "a coulomb per second" equals an AMPERE.
The AMPERE IS THE UNIT OF MEASURE OF CURRENT STRENGTH. ONE COULOMB passing a point in a circuit in ONE SECOND is
ONE AMPERE. One ampere of current means that one coulomb (or 6.3 billion billions of electrons) passes a point in
the' circuit each and every second. Two coulombs each second would be two amperes; and 100 coulombs each second
would be 100 amperes. Likewise, 100 coulombs in 2 seconds would be only 50 amperes (50 coulombs EACH second).
AMPERAGE is the measure of the RATE OF FLOW of electrons.
An ordinary light. bulb requires one-half an
ampere. But a 36-inch naval searchlight requires 150 amperes. This shows that the current to a searchlight is 300
times as large as the current to an ordinary light bulb. The searchlight is about 300 times as strong as the lamp.
Copper wire is used to carry' current because copper has many FREE ELECTRONS (easily dislodged electrons). Of
course, every copper nucleus tries to hang on to its own electrons including the free ones. And the attraction for
the free electrons must be OVERCOME before current can flow.
The property of "hanging on" is called RESISTANCE. All matter, including a copper wire, has a certain
amount of resistance. When a current flows, the resistance of the circuit must be overcome by the potential of the
circuit. If the POTENTIAL is large, or the RESISTANCE small-strong current flows. On the other hand, if the
POTENTIAL is small. or the RESISTANCE large-LITTLE current flows.
CONDUCTORS AND INSULATORS
Just what makes some materials carry current more easily than others is not thoroughly known. Most scientists
believe that it is because molecules differ in the number of their free electrons-electrons which can be broken
away from a molecule and forced along to the next molecule. It seems that the molecules of most METALS are loosely
hung together-they have many free electrons. That is, the attraction between electrons and nucleus is weak, and it
is easy to push out electrons. In other words, most metals have LOW resistances and are called GOOD CONDUCTORS.
Most NON-METALS are just the opposite of this-they have tight molecules which have few tree electrons. In fact,
for all practical purposes, some of the non-metals have no free electrons. It is almost impossible to force
electrons through substances of this kind. Such non-metals have a HIGH resistance. They are extremely POOR
CONDUCTORS and are called INSULATORS.
It is wrong to say that all substances are either conductors or
insulators. There is no sharp dividing line. Electricians simply use the BEST conductors for wires to CARRY
current, and the POOREST conductors for insulators to PREVENT the passage of current. Below is a table listing
some of the best conductors and some of the best insulators (poorest conductors).
Imagine that you are to run power from the dynamo room to the bridge searchlight. For your wire, you would
choose a good conductor. Silver is too. costly, so you'd probably select copper. You would not be able to use a
bare wire because in running through bulkheads, along overheads, and through decks, a good part of your
se3.rchlight cur-rent would escape through the steel of the ship (a good conductor). To prevent this loss, you
would use a wire coated by an insulator-probably rubber. The copper carries the current and the rubber prevents
the current from escaping out of the wire.
The amount of current that is wanted in any wire depends on the use of the circuit and the type of the wire.
It would be foolish to send one-half an ampere to a searchlight needing 150 amperes. The amount of current can be
controlled in two ways. First, by the amount of POTENTIAL DIFFERENCE and second, by the amount of RESISTANCE.
Up to this point, potential has meant the charging of a body or the charging of one end of a wire. This charging
results in a DIFFERENCE of potential between two bodies or between two ends of a wire. If you refer back to figure
8, you will see that this difference in potential is easy to calculate. From 0 to +4 is a difference of 4. From -2
to +3 is a difference of 5. (Note: -2 to 0 is 2, and 0 to +3 is 3. And 2 + 3 = 5.) To be ABSOLUTELY correct, you
should call this POTENTIAL DIFFERENCE. Electricians often shorten this term to the one word POTENTIAL.
Increasing the pressure in a water pipe increases the flow of water. Likewise, increasing potential difference on
a circuit increases the flow of current. Compare the drawings in figure 12.
If the resistance to flow
remains the same; you can see that when you double the pressure on the water in a tank, you force twice as much
water through the pipe. :When the pressure is tripled, the amount of water is tripled. Also, when you double the
potential difference, the current is doubled.
Figure 12. - Potential difference and current.
For a difference in potential of 2, only one ampere flows, but for a potential difference (p.d.) of 4, two
amperes flow. Calculate how many amperes will flow for a potential difference of 6. Then check figure 12 to see if
you are correct. These ideas are stated in a fundamental law of electricity -
CURRENT IS DIRECTLY PROPORTIONAL TO POTENTIAL DIFFERENCE.
The second factor in controlling current is the amount of resistance. If the potential difference re-mains the
same, an INCREASED resistance will DECREASE the current. Compare the drawings in figure 13. In the water system
there are four factors, determining the resistance to the flow of water -
(1) Diameter of
(2) Length of the pipe.
(3) Kind of pipe.
Velocity of flow.
The smaller the pipe, the longer the pipe, the dirtier the inside of the pipe-the more
friction the pipe has. Friction is resistance, so the greater the friction, the smaller the flow of water through
the pipe. Electrical wires are the "pipes" of an electrical circuit. The resistance of these wires, which is like
the friction of the pipes, depends on four factors -
(2) Length of the wire.
(3) Kind of wire.
(4) Temperature of the wire.
Notice in figure 13 that if the wire is
longer or smaller, less current will flow. This is because the resistance has been increased. Likewise, if the
wire is made of higher resistance material (iron) the current is less. These three factors are similar to the
first three factors in the water - pipe system. Temperature - the fourth factor which affects the resistance of a
wire - may be compared to the velocity of flow in a water-pipe. For some reason, not entirely Clear to scientists,
the resistance of most conductors increases as the temperature increases. The effect of temperature change is so
small that it may be neglected for all ordinary cases.
If the RESISTANCE of a wire is INCREASED by any on
of these four factors - size, length, material, and temperature - the CURRENT is DECREASED. Thus, you have another
fundamental law of electricity-
CURRENT IS INVERSELY PROPORTIONAL TO RESISTANCE.
Figure 13. - Resistance and current.
Imagine again that you are running a power cable to the bridge searchlight. A wire long enough to reach from
the dynamo room to the bridge will have considerable resistance because of its LENGTH. You don't want too much
resistance, so you select a wire LARGE ENOUGH IN DIAMETER to carry the 150 amperes. Naturally, you use a wire of
low resistance material-probably copper-and insulate it.
In this chapter you have studied how a current flows
and how its strength is measured. YOU MUST understand these fundamentals - how resistance and potential difference
affect the strength of a current. Be sure you have these ideas straight.
Chapter 3 Quiz