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There are four concentric shells A,B, C and D of radii `a,2a,3a` and `4a` respectively. Shells B and D are given charges `+q` and `-q` respectively. Shell C is now earthed. The potential difference `V_A-V_C` is `k=(1/(4piepsilon_0))`

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To solve the problem, we need to calculate the potential difference \( V_A - V_C \) between the shells A and C, given the conditions of the concentric shells and their charges. ### Step-by-Step Solution: 1. **Identify the Shells and Their Charges**: - Shell A has radius \( a \). - Shell B has radius \( 2a \) and charge \( +q \). - Shell C has radius \( 3a \) and is earthed (potential is set to zero). - Shell D has radius \( 4a \) and charge \( -q \). 2. **Understand the Effect of Earthing Shell C**: - When shell C is earthed, its potential \( V_C \) becomes zero. 3. **Use Gauss's Law to Determine Electric Fields**: - For the region between shells A and B (from \( r = a \) to \( r = 2a \)), the electric field \( E \) is zero because the charge enclosed is zero. - From shell B to shell C (from \( r = 2a \) to \( r = 3a \)), the electric field can be calculated using Gauss's Law: \[ E = \frac{kq}{r^2} \] where \( k = \frac{1}{4\pi\epsilon_0} \). 4. **Calculate the Potential Difference \( V_A - V_C \)**: - The potential difference can be expressed as: \[ V_A - V_C = -\int_{r_A}^{r_C} E \, dr \] - Here, \( r_A = a \) and \( r_C = 3a \). The potential difference can be split into two parts: \[ V_A - V_C = -\int_{a}^{2a} 0 \, dr - \int_{2a}^{3a} \frac{kq}{r^2} \, dr \] - The first integral evaluates to zero since the electric field is zero between shells A and B. 5. **Evaluate the Second Integral**: - The second integral becomes: \[ -\int_{2a}^{3a} \frac{kq}{r^2} \, dr = -kq \left[-\frac{1}{r}\right]_{2a}^{3a} \] - Evaluating this gives: \[ -kq \left(-\frac{1}{3a} + \frac{1}{2a}\right) = kq \left(\frac{1}{2a} - \frac{1}{3a}\right) \] - Finding a common denominator (6a): \[ = kq \left(\frac{3}{6a} - \frac{2}{6a}\right) = \frac{kq}{6a} \] 6. **Final Result**: - Therefore, the potential difference \( V_A - V_C \) is: \[ V_A - V_C = \frac{kq}{6a} \] ### Conclusion: The potential difference \( V_A - V_C \) is \( \frac{kq}{6a} \).
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