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A parallel plate capacitor is charged to...

A parallel plate capacitor is charged to `60 muC`. Due to a radioactive source, the plate losses charge at the rate of `1.8 xx 10^(-8) Cs^(-1)`. The magnitued of displacement current is

A

`1.8 xx 10^(-8) Cs^(-1)`

B

`3.6 xx 10^(-8) Cs^(-1)`

C

`4.1 xx 10^(-11) Cs^(-1)`

D

`5.7 xx 10^(-12) Cs^(-1)`

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The correct Answer is:
To find the magnitude of the displacement current in a parallel plate capacitor that is losing charge, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Concept of Displacement Current**: Displacement current is a term introduced by James Clerk Maxwell to account for the changing electric field in situations where the electric field is changing with time, such as in a capacitor. The displacement current \( I_d \) can be expressed as: \[ I_d = \epsilon \frac{d\Phi}{dt} \] where \( \epsilon \) is the permittivity of the medium and \( \Phi \) is the electric flux. 2. **Identify the Rate of Charge Loss**: The problem states that the capacitor is losing charge at a rate of \( 1.8 \times 10^{-8} \, \text{C/s} \). This rate of charge loss can be represented as: \[ \frac{dQ}{dt} = -1.8 \times 10^{-8} \, \text{C/s} \] (The negative sign indicates a loss of charge.) 3. **Relate Displacement Current to Rate of Change of Charge**: In a capacitor, the displacement current \( I_d \) can also be defined as: \[ I_d = \frac{dQ}{dt} \] Since the displacement current is equal to the rate of change of charge, we can substitute the value we have: \[ I_d = 1.8 \times 10^{-8} \, \text{A} \] 4. **Conclusion**: Therefore, the magnitude of the displacement current is: \[ I_d = 1.8 \times 10^{-8} \, \text{A} \] ### Final Answer: The magnitude of the displacement current is \( 1.8 \times 10^{-8} \, \text{A} \).

To find the magnitude of the displacement current in a parallel plate capacitor that is losing charge, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Concept of Displacement Current**: Displacement current is a term introduced by James Clerk Maxwell to account for the changing electric field in situations where the electric field is changing with time, such as in a capacitor. The displacement current \( I_d \) can be expressed as: \[ I_d = \epsilon \frac{d\Phi}{dt} ...
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DC PANDEY ENGLISH-ELECTROMAGNETIC WAVES-Sec A
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