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A sphere of radius R and charge Q is pla...

A sphere of radius R and charge Q is placed inside an imaginary sphere of radius `2R` whose centre coincides with the given sphere. The flux related to imaginary sphere is:

A

`Q/in_(0)`

B

`Q/(2in_(0))`

C

`(4Q)/in_(0)`

D

`(2Q)/in_(0)`

Text Solution

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The correct Answer is:
To solve the problem of finding the electric flux through an imaginary sphere of radius `2R` that encloses a sphere of radius `R` with charge `Q`, we can use Gauss's Law. Here’s the step-by-step solution: ### Step 1: Understand Gauss's Law Gauss's Law states that the electric flux (Φ) through a closed surface is equal to the charge (Q_enc) enclosed by that surface divided by the permittivity of free space (ε₀). Mathematically, it is expressed as: \[ \Phi = \frac{Q_{\text{enc}}}{\epsilon_0} \] ### Step 2: Identify the Charge Enclosed In this scenario, we have a sphere of radius `R` with charge `Q` placed inside an imaginary sphere of radius `2R`. Since the charge `Q` is fully enclosed by the imaginary sphere, we can say that: \[ Q_{\text{enc}} = Q \] ### Step 3: Apply Gauss's Law Now, we can apply Gauss's Law to find the electric flux through the imaginary sphere of radius `2R`: \[ \Phi = \frac{Q}{\epsilon_0} \] ### Step 4: Conclusion Thus, the electric flux related to the imaginary sphere is: \[ \Phi = \frac{Q}{\epsilon_0} \] Now, we can check the options provided in the question to find the correct answer. ### Final Answer The flux related to the imaginary sphere is: \[ \Phi = \frac{Q}{\epsilon_0} \]

To solve the problem of finding the electric flux through an imaginary sphere of radius `2R` that encloses a sphere of radius `R` with charge `Q`, we can use Gauss's Law. Here’s the step-by-step solution: ### Step 1: Understand Gauss's Law Gauss's Law states that the electric flux (Φ) through a closed surface is equal to the charge (Q_enc) enclosed by that surface divided by the permittivity of free space (ε₀). Mathematically, it is expressed as: \[ \Phi = \frac{Q_{\text{enc}}}{\epsilon_0} \] ...
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