1.

A sphere of radius R has a volume density of charge rho=kr, were r is the distance from the centre of the sphere and k is constant . The magnitude of the electric field which exists at the surface of the sphere is given by (epsilon_(0)= permittivity of free space)

Answer»

`(4pikR^(4))/(3epsilon_(0))`
`(kR)/(3epsilon_(0))`
`(4pikR)/(epsilon_(0))`
`(kR^(2))/(4pi_(0))`

Solution :Consider a thin spherical shell of radius x and thickness dx as shown in the figure.

Volume of the shell , `dV=4pix^(2)dx`
LET us draw a GAUSSIAN SURFACE od radius `r(rltR)`as shown in the figure above.
Total charge enclosed by the Gaussian surface is
`Q_("in")=int_(0)^(r)rhodV=int_(0)(r)kx4pix^(2)dx=4pikint_(0)^(r)x^(3)dx`
`=4pik[(x^(4))/(4)]_(0)^(r)=pikr^(4)`
According to Gaussa.s law
`E4pir^(2)=(Q_("in"))/(epsilon_(0))orE4pir^(2)=(pikr^(4))/(epsilon_(0))`
At the surface of the sphere , r=R
`thereforeE=(kR^(2))/(4piepsilon_(0))`


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