To find the voltage \( V \) in a given electrical network using the Superposition Theorem, follow these steps. I'll illustrate the process with a general example to make the approach clear. For this example, assume we have a linear circuit with multiple independent sources (current or voltage sources).
### Example Circuit Description
Consider a circuit with:
- A voltage source \( V_1 \) in series with a resistor \( R_1 \).
- A second voltage source \( V_2 \) in series with a resistor \( R_2 \).
- Both voltage sources are connected in parallel across a common resistor \( R_3 \), and we want to find the voltage \( V \) across \( R_3 \).
### Steps to Apply Superposition Theorem
1. **Identify Independent Sources**: In this case, we have two independent sources, \( V_1 \) and \( V_2 \).
2. **Turn Off All Sources Except One**: To use the superposition theorem, we need to analyze the circuit multiple times, each time considering only one independent source while replacing the others with their internal resistances.
- **Turn off \( V_2 \)**: Replace \( V_2 \) with a short circuit (since an ideal voltage source when turned off becomes a short circuit).
- **Analyze the Circuit with \( V_1 \) Only**: Calculate the voltage \( V_{1} \) across \( R_3 \) with \( V_2 \) shorted.
- **Turn off \( V_1 \)**: Replace \( V_1 \) with a short circuit.
- **Analyze the Circuit with \( V_2 \) Only**: Calculate the voltage \( V_{2} \) across \( R_3 \) with \( V_1 \) shorted.
3. **Calculate the Voltage Due to Each Source**:
- **For \( V_1 \)**:
- **Circuit Analysis**: With \( V_2 \) shorted, the voltage \( V_{1} \) across \( R_3 \) can be found using voltage divider or other circuit analysis methods.
- **Example Calculation**: Assuming the resistors are in series, the voltage \( V_{1} \) across \( R_3 \) can be given by:
\[
V_{1} = V_1 \times \frac{R_3}{R_1 + R_2 + R_3}
\]
- **For \( V_2 \)**:
- **Circuit Analysis**: With \( V_1 \) shorted, calculate the voltage \( V_{2} \) across \( R_3 \) in a similar manner.
- **Example Calculation**: The voltage \( V_{2} \) across \( R_3 \) can be:
\[
V_{2} = V_2 \times \frac{R_3}{R_2 + R_3}
\]
4. **Superimpose the Results**: Add the voltages obtained from each source to get the total voltage \( V \) across \( R_3 \).
\[
V = V_{1} + V_{2}
\]
### Example
Let’s assume the following values for simplicity:
- \( V_1 = 10V \), \( R_1 = 1k\Omega \)
- \( V_2 = 5V \), \( R_2 = 2k\Omega \)
- \( R_3 = 3k\Omega \)
**1. With \( V_2 \) Shorted:**
\[
V_{1} = V_1 \times \frac{R_3}{R_1 + R_2 + R_3} = 10V \times \frac{3k\Omega}{1k\Omega + 2k\Omega + 3k\Omega} = 10V \times \frac{3k\Omega}{6k\Omega} = 5V
\]
**2. With \( V_1 \) Shorted:**
\[
V_{2} = V_2 \times \frac{R_3}{R_2 + R_3} = 5V \times \frac{3k\Omega}{2k\Omega + 3k\Omega} = 5V \times \frac{3k\Omega}{5k\Omega} = 3V
\]
**3. Total Voltage Across \( R_3 \):**
\[
V = V_{1} + V_{2} = 5V + 3V = 8V
\]
So, the voltage across \( R_3 \) is \( 8V \).
### Summary
The Superposition Theorem helps simplify complex circuits with multiple sources by breaking the problem into simpler parts, analyzing each part, and then combining the results. Always remember to turn off all sources except one at a time, and replace each turned-off source with its internal resistance (short circuit for voltage sources and open circuit for current sources).