FIG. 55.--CURVES OF RISE OF CURRENT WITH DIFFERENT GROUPINGS OF BATTERY.

When they are all put in series, so that the battery has a much

greater resistance than the rest of the circuit, the current rises

much more rapidly, because of the smallness of the time constant,

although it never attains the same ultimate maximum as when grouped in

the other way. That is to say, if there is self-induction as well as

resistance in the circuit, the amateur rule does not tell you the best

way of arranging the battery. There is another mode of regarding the

matter which is helpful. Self-induction, while the current is growing,

acts as if there were a sort of spurious addition to the resistance of

the circuit; and while the current is dying away it acts of course in

the other way, as if there were a subtraction from the resistance.

Therefore you ought to arrange the battery so that the internal

resistance is equal to the real resistance of the circuit, plus the

spurious resistance during that time. But how much is the spurious

resistance during that time? It is a resistance proportional to the

time that has elapsed since the current was turned on. So then it

comes to a question of the length of time for which you want to work

it. What fraction of a second do you require your signal to be given

in? What is the rate of the vibrator of your electric bell? Suppose

you have settled that point, and that the short time during which the

current is required to rise is called t; then the apparent resistance

at time t after the current is turned on is given by the formula:

Scientific American Supplement, No. 787, January 31, 1891 · 第 35 / 71 题