An LC circuit consists of a 20 mH inductor and a 0.500 uf capacitor. If the maximum instantaneous current is 0.100 A, what is the greatest potential difference across the capacitor?

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**Problem 4: LC Circuit Analysis**

An LC circuit consists of a 20 mH inductor and a 0.500 μF capacitor. If the maximum instantaneous current is 0.100 A, what is the greatest potential difference across the capacitor?

**Solution Explanation**

To solve this problem, we use the principle of energy conservation in the LC circuit. The sum of the magnetic energy in the inductor and the electric energy in the capacitor is constant. 

1. **Magnetic Energy in the Inductor:**
   \[
   U_L = \frac{1}{2} L I^2
   \]
   Where:
   - \( L = 20 \, \text{mH} = 20 \times 10^{-3} \, \text{H} \)
   - \( I = 0.100 \, \text{A} \)
   
2. **Electric Energy in the Capacitor:**
   \[
   U_C = \frac{1}{2} C V^2
   \]
   Where:
   - \( C = 0.500 \, \mu\text{F} = 0.500 \times 10^{-6} \, \text{F} \)
   - \( V \) is the potential difference we need to find.

3. **Applying Energy Conservation:**
   \[
   \frac{1}{2} L I^2 = \frac{1}{2} C V^2
   \]

   Substituting values into the equation:
   \[
   \frac{1}{2} (20 \times 10^{-3}) (0.100)^2 = \frac{1}{2} (0.500 \times 10^{-6}) V^2
   \]

4. **Solving for V:**
   \[
   V^2 = \frac{(20 \times 10^{-3}) \times (0.100)^2}{0.500 \times 10^{-6}}
   \]
   \[
   V = \sqrt{\frac{(20 \times 10^{-3}) \times (0.100)^2}{0.500 \times 10^{-6}}}
   \]

Calculate the potential difference \( V \) from the equation above.

This approach provides the greatest potential difference across the capacitor in the LC circuit.
Transcribed Image Text:**Problem 4: LC Circuit Analysis** An LC circuit consists of a 20 mH inductor and a 0.500 μF capacitor. If the maximum instantaneous current is 0.100 A, what is the greatest potential difference across the capacitor? **Solution Explanation** To solve this problem, we use the principle of energy conservation in the LC circuit. The sum of the magnetic energy in the inductor and the electric energy in the capacitor is constant. 1. **Magnetic Energy in the Inductor:** \[ U_L = \frac{1}{2} L I^2 \] Where: - \( L = 20 \, \text{mH} = 20 \times 10^{-3} \, \text{H} \) - \( I = 0.100 \, \text{A} \) 2. **Electric Energy in the Capacitor:** \[ U_C = \frac{1}{2} C V^2 \] Where: - \( C = 0.500 \, \mu\text{F} = 0.500 \times 10^{-6} \, \text{F} \) - \( V \) is the potential difference we need to find. 3. **Applying Energy Conservation:** \[ \frac{1}{2} L I^2 = \frac{1}{2} C V^2 \] Substituting values into the equation: \[ \frac{1}{2} (20 \times 10^{-3}) (0.100)^2 = \frac{1}{2} (0.500 \times 10^{-6}) V^2 \] 4. **Solving for V:** \[ V^2 = \frac{(20 \times 10^{-3}) \times (0.100)^2}{0.500 \times 10^{-6}} \] \[ V = \sqrt{\frac{(20 \times 10^{-3}) \times (0.100)^2}{0.500 \times 10^{-6}}} \] Calculate the potential difference \( V \) from the equation above. This approach provides the greatest potential difference across the capacitor in the LC circuit.
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