The equivalent resistance of a circuit depends on whether the resistors are arranged in series or parallel. Here’s a detailed breakdown of the formulas for both configurations:
### 1. Resistors in Series
When resistors are connected in series, the total or equivalent resistance (\(R_{eq}\)) is simply the sum of the individual resistances. This is because the current flowing through each resistor is the same, and the total voltage across the series combination is the sum of the voltages across each resistor.
**Formula:**
\[
R_{eq} = R_1 + R_2 + R_3 + \ldots + R_n
\]
- **Example:** If you have three resistors in series: \(R_1 = 2 \, \Omega\), \(R_2 = 3 \, \Omega\), and \(R_3 = 5 \, \Omega\):
\[
R_{eq} = 2 + 3 + 5 = 10 \, \Omega
\]
### 2. Resistors in Parallel
When resistors are connected in parallel, the total or equivalent resistance (\(R_{eq}\)) is calculated using the reciprocal of the sum of the reciprocals of the individual resistances. In this configuration, the voltage across each resistor is the same, but the current can vary.
**Formula:**
\[
\frac{1}{R_{eq}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \ldots + \frac{1}{R_n}
\]
To find \(R_{eq}\), you can take the reciprocal of the total obtained from the right side:
\[
R_{eq} = \frac{1}{\left( \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \ldots + \frac{1}{R_n} \right)}
\]
- **Example:** If you have three resistors in parallel: \(R_1 = 2 \, \Omega\), \(R_2 = 3 \, \Omega\), and \(R_3 = 6 \, \Omega\):
\[
\frac{1}{R_{eq}} = \frac{1}{2} + \frac{1}{3} + \frac{1}{6}
\]
\[
\frac{1}{R_{eq}} = \frac{3}{6} + \frac{2}{6} + \frac{1}{6} = \frac{6}{6} = 1
\]
Therefore, \(R_{eq} = 1 \, \Omega\).
### Summary
- **Series:** \(R_{eq} = R_1 + R_2 + R_3 + \ldots\)
- **Parallel:** \(\frac{1}{R_{eq}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \ldots\)
These formulas help you calculate the equivalent resistance in various circuit configurations, which is essential for analyzing electrical circuits.