When resistors are connected in series, a simplification of the circuit is possible. Consider the resistive circuit shown in Fig. 1(a). Since the resistors are in series, they both carry the same current. Ohm's law gives:
(1)
\[{v_1} = {R_1}i\] \[{v_2} = {R_2}i\]Applying KVL around the loop:
(2)
\[ - v + {v_1} + {v_2} = 0 \Rightarrow v = {v_1} + {v_2}\]Substituting equations (1) into equation (2) and solving for the current i results in:
(3)
\[i = \frac{v}{{{R_1} + {R_2}}}\](4)
\[i = \frac{v}{{{R_{eq}}}}\](5)
\[{R_{eq}} = {R_1} + {R_2}\]Figures 1(a) and 1(b) are called equivalent circuits if the equivalent resistance of Fig. 1(b) is chosen as shown in equation (5). Req of equation (5) is called the equivalent resistance of the series combination of resistors R1 and R2.
This result can be generalized to a series combination of N resistances as follows:
Replace any series resistors in the circuit below with their equivalent resistance.
All four resistors in the circuit are in series. We can add all four resistances to obtain the equivalent resistance, so the equivalent resistance is:
And the equivalent circuit is:
Replace any series resistors in the circuit below with their equivalent resistance.
The two resistors to the far right—the 1.5 kΩ and 2.2 kΩ resistors—are not in series. However, recall that KCL can be applied over any enclosed surface. If we define a surface which encloses the 1.5 kΩ and 2.2 kΩ resistors, as shown below, we see that the 4.7k and 6.8k resistors are in series and can be combined into a ingle 11.5 kΩ resistor.
The 1k and 1.5k resistors to the left of the source are more obviously in series, and can be combined into a single 2.5k resistor. The final circuit is shown below.