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Question: Express the total charge \(Q\) on the rod in terms of \(\alpha \) and \(L\). ![](https://www.vedan...

Express the total charge QQ on the rod in terms of α\alpha and LL.

(A) αL2\dfrac{{\alpha L}}{2}
(B) αL22\dfrac{{\alpha {L^2}}}{2}
(C) αL32\dfrac{{\alpha {L^3}}}{2}
(D) αL23\dfrac{{\alpha {L^2}}}{3}

Explanation

Solution

Linear charge density varies continuously at a constant rate throughout the rod when the charge is kept in line with the axis of the rod. Which means that at every point on the rod, the linear charge density is different.

Complete step by step answer:
Linear charge density is the ratio of the total charge present on the rod to total length. Linear charge density on a small segment of rod can be given by,
λ=dqdx\lambda = \dfrac{{dq}}{{dx}}
Where, dq=dq = small charge present on small segment dxdx. So,
dq=λdxdq = \lambda dx
This can also be written as,
dq=αxdxdq = \alpha xdx
Now integrating the above equation,
0Qdq=0Lαxdx\Rightarrow \int\limits_0^Q {dq} = \int\limits_0^L {\alpha xdx}
Q=α[x22]0L\Rightarrow Q = \alpha \left[ {\dfrac{{{x^2}}}{2}} \right]_0^L
Q=αL22\Rightarrow Q = \dfrac{{\alpha {L^2}}}{2}

Hence option B is the correct answer.

Note: Surface Charge Density is the ratio of total charge on a plane sheet to total area of sheet. And volume charge density is the ratio of total charge present on a body to total volume of the body. All the charge densities are born from one theorem and Gauss' theorem.