The Library of Work and Play: Electricity and Its Everyday UsesWoodhull, John F. (John Francis)
Science
The Library of Work and Play: Electricity and Its Everyday Uses
Woodhull, John F. (John Francis)
Electricity -- Juvenile literature
We found out how much wire was wound upon the armature and put exactly
the same amount in the outside resistance, _R_ (Fig. 59). The needle
now showed that one volt is able to push through twice the resistance
of the armature only half as much current, and the needle stopped
at .008 ampere. If this were to be the resistance in the volt meter
circuit one volt should stand under .008 ampere and two under .016 and
three under .024. It is evident then, that, if we know the internal
resistance of a volt meter, we may make it capable of measuring greater
electrical pressures by adding the proper amount of resistance. By
putting at _R_, (Fig. 59) nine times the internal resistance of the
instrument, thus multiplying the total resistance tenfold, the figures
upon the scale of volts may be read as whole numbers from one to
fifteen. In this case it will require fifteen cells to push the needle
clear across the scale and ten cells to push it two thirds of the
way across. If now we add enough external resistance to multiply the
resistance of the armature a hundred fold it will require 150 volts to
push .024 of an ampere through the armature and pull its needle clear
across the scale. In this case the figures upon the scale of volts are
multiplied by one hundred and read from ten to one hundred and fifty.
Such a scale would adapt this volt meter for use with our 110-volt
lighting circuit. Volt meters are made with a series of such external
resistances, called "multipliers," attached so that they may be easily
thrown into the circuit.
It is evident that we need some term so that we may speak of quantities
of resistance. This need has given rise to a unit of resistance called
an ohm, after George Simon Ohm (1789-1854) born at Erlanger in Bavaria.
Two inches of No. 36 German silver wire, such as is wound upon the
armature of this volt meter, gives one ohm of resistance. There are 125
inches of this wire upon the armature. Its resistance is, therefore,
62.5 ohms, and we may, therefore, say that one volt of electric
pressure can push through 62.5 ohms of resistance .016 of an ampere of
current. Ohm discovered this relationship in 1827, and formulated it
as follows:
volts/ohms = amperes (not, however, using these words).
(1 volt)/(62.5 ohms) = .016 ampere.
62.5) 1.0000 (.016
625
----
3750
3750
----
This is called Ohm's law, as every candidate for college admission will
hear and hear again.
[Illustration: Fig. 60]
Public-domain text, read in full here on John Shaqi.
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