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The electrostatic potential inside a cha...

The electrostatic potential inside a charged spherical ball is given by `phi=ar^2+b` where r is the distance from the centre and a, b are constants. Then the charge density inside the ball is:

A

`-24 pi a epsi_(0) r`

B

`-6pi a epsi_(0) r`

C

`-24 pi a epsi_(0)`

D

`-6 a epsi_(0)`

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To find the charge density inside a charged spherical ball where the electrostatic potential is given by \( \phi = ar^2 + b \), we can follow these steps: ### Step 1: Find the Electric Field The electric field \( E \) is related to the electrostatic potential \( \phi \) by the relation: \[ E = -\frac{d\phi}{dr} \] Given \( \phi = ar^2 + b \), we differentiate it with respect to \( r \): \[ E = -\frac{d}{dr}(ar^2 + b) = -\frac{d}{dr}(ar^2) - \frac{d}{dr}(b) = -2ar \] Thus, the electric field inside the charged spherical ball is: \[ E = -2ar \] ### Step 2: Relate Electric Field to Charge Density Using Gauss's law, we know that the electric field \( E \) is also related to the charge density \( \rho \) by the equation: \[ E = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2} \] where \( Q \) is the charge enclosed within a radius \( r \). The charge density \( \rho \) can be expressed as: \[ \rho = \frac{dQ}{dV} \] For a spherical volume, the volume element \( dV \) is given by \( dV = 4\pi r^2 dr \). ### Step 3: Calculate Charge Enclosed From the electric field expression, we can find the total charge \( Q \) enclosed within radius \( r \): \[ E = -2ar \implies -2ar = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2} \] Rearranging gives: \[ Q = -8\pi\epsilon_0 ar^3 \] ### Step 4: Differentiate Charge to Find Charge Density Now, we differentiate \( Q \) with respect to \( r \) to find the charge density \( \rho \): \[ \frac{dQ}{dr} = \frac{d}{dr}(-8\pi\epsilon_0 ar^3) = -24\pi\epsilon_0 ar^2 \] Thus, the charge density \( \rho \) is: \[ \rho = \frac{dQ}{dV} = \frac{dQ}{dr} \cdot \frac{1}{dV/dr} = \frac{-24\pi\epsilon_0 ar^2}{4\pi r^2} = -6\epsilon_0 a \] ### Conclusion The charge density inside the ball is: \[ \rho = -6\epsilon_0 a \]
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