(a) Gauss’ law states that the electric flux of the resultant electric field through a closed surface is
1ε0 times of net charge enclosed by the surface
∫→E.→ds=qnetε0
where,
q = net charge enclosed by surface
ε0 = permittivity of free space
Electric field due to a long straight wire
Consider an infinitely long thin wire with uniform linear charge density
λ. To calculate the field imagine a cylindrical Gaussian surface as shown in the figure. Since the field is radial everywhere, therefore, flux through the two flat ends of the cylindrical Gaussian surface is zero.
Hence,
Flux through the Gaussian surface = Flux through the curved cylindrical part of the surface
=E.2πrl
The surface includes a charge equal to
λl, Gauss’s law then gives
E×2πrl=λlε0
E=λ2πε0r
Vectorially→E=λ2πε0r^n
^n is the radial unit vector, in the plane normal to the wire passing through the point.
(
b)
E=10r+5
The potential difference between the two points
VB−VA=−∫BA→E.d→r
=−∫r=10r=1(10r+5).dr
=−(10r22+5r)101
=−{[10×1002+5×10]−[102+5]}
=−(550−10)
=−540 volt
Hence potential increases by
–540 V in moving from point
r=1 m to
r=10 m.