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3. A uniformly charged sphere of radius a has a charge density po. Find D everywhere using Gausss law. Plot the magnitude

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Answer #1

D is electric displacement vector inside matter ( dielectrics , not conductors).

Gauss law for insulators is

\oint D .da = Q_{fenc}

D = \epsilon _oE + P , where P is polarisation the medium.

Qfenc - is the free charge enclosed inside the Gaussian surface.

charge density = \rho_o

Draw a Gaussian sphere of radius R < a , concentric with the center of the sphere.

charge enclosed in side the Gaussian sphere qen = \rho_o 4/3 \piR3

Like electric field E, D also uniform every where on the surface of the sphere and is normal to the surface.

D* 4\piR2 =  \rho_o 4/3 \piR3

D = \rho_oR/3 for R<a

for R >= a total charge enclosed inside the Gaussian surface Qenc = \rho_o 4/3 \pia3

D* 4\piR2 =  \rho_o 4/3 \pia3  

D =  \rho_o/3a3/R2  

D increases linearly for R<=a to max. \rho_oa/3 and then falls with inverse square of R.

- - - - - - + 10 rho*R 3

4. It is not clear how the two shells are placed.

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