The Study of Elementary Electricity and Magnetism by Experiment: Containing Two Hundred Experiments Performed with Simple, Home-made ApparatusSt. John, Thomas M. (Thomas Matthew)
Science
The Study of Elementary Electricity and Magnetism by Experiment: Containing Two Hundred Experiments Performed with Simple, Home-made Apparatus
_=305. Resistance.=_ It is harder for a horse to draw a wagon through
deep sand than over a smooth pavement. We may say that the sand holds
the horse back--that is, it offers a resistance. The electric current
does not pass through all sorts of substances with the same ease, and
when it succeeds in pushing its way through a circuit of considerable
resistance, we cannot expect it to arrive at the end of its journey
without being weaker than when it started. Do we expect this of a man
or horse? We shall soon see that there is a definite relation between
resistance and the strength of the current at the end of its journey.
=EXPERIMENT 118. To study the general effect of "resistance"
upon a current.=
_Apparatus._ Galvanoscope, G V (No. 58); resistance coil, R
C (No. 79) (§ 310); two-fluid cell, 2-F C (§ 281); 4 wires
with connectors (§ 226). _Arrange_ as in Fig. 92. The current
passes as shown by the arrow, and the circuit may be opened and
closed at the metal plate, M P, or by using a key in its place.
Properly place G V.
=306. Directions.= (A) Take the reading of G V in degrees, the
current passing through the entire length of R C. (See § 310.)
(B) Change the end of wire 4 from binding-post R to M, on R C,
so that the current will pass through one-half only of R C.
Note the reading of G V.
(C) Remove R C entirely and connect wires 3 and 4 by means of a
metal plate. Compare the readings of (A), (B) and (C). What do
they show?
[Illustration: Fig. 92.]
_=307. External Resistance; Internal Resistance.=_ When we consider
a circuit like that shown in Fig. 92 we see that it is composed of
two parts, and that we have two kinds of resistances. The wires,
instruments, etc., make up what is called the _external resistance_
of the circuit; that is, the part that is external to the cell. The
liquids in the cell offer a resistance to the current; this is called
_internal resistance_. (See § 314.) The strength of the current depends
upon the relation between these two resistances, as will be seen by
future experiments, as well as upon the E. M. F. of the cell. As
liquids are not as good conductors as metals, the internal resistance
of cells may be quite high.
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