Solveeit Logo

Question

Question: Uniformly charged long cylinder has volume charge density\(\rho \). Find an electric field at a dist...

Uniformly charged long cylinder has volume charge densityρ\rho . Find an electric field at a distancex<Rx < Rfrom the axis of the cylinder.
(A) ρxε0\dfrac{{\rho x}}{{{\varepsilon _0}}}
(B) ρx2ε0\dfrac{{\rho x}}{{2{\varepsilon _0}}}
(C) ρx3ε0\dfrac{{\rho x}}{{3{\varepsilon _0}}}
(D) ρx4ε0\dfrac{{\rho x}}{{4{\varepsilon _0}}}

Explanation

Solution

For symmetric objects like a cylinder, it is very easy to apply Gauss’s law. In this specific problem, we have given that volume charge density ρ\rho is uniform throughout the cylinder. For calculation, take a cylinder of radius xx and then compute the required volume and surface area.

Formula used:
Gauss’s law is given as
E.ds=qenε0\oint {\overrightarrow E .\overrightarrow {ds} = \dfrac{{{q_e}_n}}{{{\varepsilon _0}}}}
Where qen{q_e}_n is the charge enclosed within the Gaussian surface.
E\overrightarrow E is the electric field.
ds\overrightarrow {ds} is the surface area element

Complete step by step solution:
Consider a cylinder of radius xx and length ll.

Here, the long cylinder with radius RR is shown in a solid line and the Gaussian surface that we have taken with radius xxand length llis shown in the dotted line.
We know that,
E.ds=qenε0\oint {\overrightarrow E .\overrightarrow {ds} = \dfrac{{{q_e}_n}}{{{\varepsilon _0}}}} (1) - - - - (1)
Here, we have volume charge density ρ\rho and a cylinder (Gaussian surface) of radiusxxand lengthll.
So, the charge enclosed within this cylinder can be calculated as
qen=ρ×V{q_e}_n = \rho \times V
Here,VVis the volume of the cylinder.
qen=ρ×πx2l\Rightarrow {q_e}_n = \rho \times \pi {x^2}l
Using this in the equation(1)(1), we get
E.ds=ρ×πx2lε0\oint {\overrightarrow E .\overrightarrow {ds} = \dfrac{{\rho \times \pi {x^2}l}}{{{\varepsilon _0}}}}
Here, the surface area element is
ds=2πxl\overrightarrow {ds} = 2\pi xl
Using this in the above equation, we get
E2πxl=ρ×πx2lε0E2\pi xl = \dfrac{{\rho \times \pi {x^2}l}}{{{\varepsilon _0}}}
E=ρπx2l2πxlε0\Rightarrow E = \dfrac{{\rho \pi {x^2}l}}{{2\pi xl{\varepsilon _0}}}
Solving this, we get
E=ρx2ε0E = \dfrac{{\rho x}}{{2{\varepsilon _0}}}

Thus, option (B) is correct.

Additional information: While choosing the Gaussian surface, theoretically we can take any shape or size. But while calculating it would be difficult to calculate the surface area or volume of any arbitrary shape. Moreover, if the given charge density is cylindrical, it is suggested to take a cylindrical Gaussian surface. If you have any doubts, you can try to solve this simple question by taking a spherical Gaussian surface.

Note: In this problem, we have been given a constant volume charge density. But if the volume charge density is given likeρ=ρ0x\rho = {\rho _0}x, then you simply can’t calculate the enclosed charge like this problem. You have to integrate over the whole volume of your Gaussian surface.