In series combination, resistors are connected end-to-end such that the same current flows through each.
\[ R_s = R_1 + R_2 + R_3 + \cdots \]
Derivation
\[
V = V_1 + V_2 + V_3
\]
\[
\begin{aligned}
V &= IR,\\ V_1 &= IR_1,\\ V_2 &= IR_2,\\ V_3 &= IR_3
\end{aligned}
\]
\[
\begin{aligned}
IR &= IR_1 + IR_2 + IR_3\\
\Rightarrow R_s &= R_1 + R_2 + R_3
\end{aligned}
\]
Key Characteristics
- Current remains same in all resistors
- Voltage divides across resistors
- Equivalent resistance increases
In parallel combination, resistors are connected across the same two points,
providing multiple paths for current.
\[
\frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3}
\]
Derivation
\[
I = I_1 + I_2 + I_3
\]
\[
\begin{aligned}
I &= \frac{V}{R_p},\\\\ I_1 &= \frac{V}{R_1},\\\\ I_2 &= \frac{V}{R_2},\\\\ I_3 &= \frac{V}{R_3}
\end{aligned}
\]
\[
\begin{aligned}
\frac{V}{R_p} &= \frac{V}{R_1} + \frac{V}{R_2} + \frac{V}{R_3}\\\\
\Rightarrow \frac{1}{R_p} &= \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3}
\end{aligned}
\]
Key Characteristics
- Voltage remains same across all resistors
- Current divides among branches
- Equivalent resistance decreases