Example 21.1 from College Physics, 21.1 Resistors in Series and Parallel
Suppose the voltage output of the battery in Figure 21.3 is , and the resistances are , , and . (a) What is the total resistance? (b) Find the current. (c) Calculate the voltage drop in each resistor, and show these add to equal the voltage output of the source. (d) Calculate the power dissipated by each resistor. (e) Find the power output of the source, and show that it equals the total power dissipated by the resistors.
Work it out on paper first. Then open the solution one step at a time, and stop as soon as you can finish on your own.
The total resistance is simply the sum of the individual resistances, as given by this equation:
The current is found using Ohm’s law, . Entering the value of the applied voltage and the total resistance yields the current for the circuit:
The voltage—or drop—in a resistor is given by Ohm’s law. Entering the current and the value of the first resistance yields
Similarly,
and
The three drops add to , as predicted:
The easiest way to calculate power in watts (W) dissipated by a resistor in a DC circuit is to use Joule’s law, , where is electric power. In this case, each resistor has the same full current flowing through it. By substituting Ohm’s law into Joule’s law, we get the power dissipated by the first resistor as
Similarly,
and
Power can also be calculated using either or , where is the voltage drop across the resistor (not the full voltage of the source). The same values will be obtained.
The easiest way to calculate power output of the source is to use , where is the source voltage. This gives
Note, coincidentally, that the total power dissipated by the resistors is also 7.20 W, the same as the power put out by the source. That is,
Power is energy per unit time (watts), and so conservation of energy requires the power output of the source to be equal to the total power dissipated by the resistors.
How did it go?