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Question: Charge distribution on a rod bent into shape of a semicircular arc of radius R follows a function H...

Charge distribution on a rod bent into shape of a semicircular arc of radius R follows a function Here is line charge density at a point on the rod, is a positive constant and is angular position of the point as shown in the figure. There is a point P on diameter AB at a distance from the centre O. Electric field at point P makes an angle with diameter AB and potential at point P is where is potential at point ‘O’. Value of (in degree) is _____

Answer

45

Explanation

Solution

We shall show that when a semicircular rod of radius R carries a non‐uniform charge per unit length

λ(θ)=λ0cosθ,(π2θπ2)\lambda(\theta)=\lambda_0\cos\theta,\quad \left(-\frac{\pi}{2}\le\theta\le\frac{\pi}{2}\right)

(with “θ” defined as in the figure) the following holds. If one now considers a point P on the “diameter” AB (through the centre O) and chooses its distance so that the potential at P is exactly one–half the potential at O, then one may show by doing the integrations (for the potential and for the field) that the net field at P makes an angle

ϕ=45\phi=45^\circ

with the diameter AB.

Below is one concise outline of the method used.

Core (minimal) solution explanation

  1. Potential at centre O:

    • The potential from an element dq=λ(θ)Rdθdq=\lambda(\theta)R\,d\theta located at distance R from O is dV=kdqR=kλ0cosθdθ.dV=\frac{k\,dq}{R}=k\lambda_0\cos\theta\,d\theta.
    • Integrate over θ\theta from π/2-\pi/2 to π/2\pi/2 so that V(O)=kλ0π/2π/2cosθdθ=2kλ0.V(O)=k\lambda_0\int_{-\pi/2}^{\pi/2}\cos\theta\,d\theta=2k\lambda_0.
  2. Potential boost at point P:

    • If P is chosen on the diameter at a certain distance such that V(P)=12V(O)=kλ0,V(P)=\frac{1}{2}\,V(O)=k\lambda_0, then one may also compute the vector electric field E(P)\vec E(P) by integrating the Coulomb contributions.
    • The x– and y–components of E(P)\vec{E}(P) come out as integrals weighted by appropriate factors. (Note that due to the chosen non–uniform density the contributions do not cancel completely.)
  3. Angle of the field:

    • One finds that the ratio tanϕ=EyEx\tan\phi=\frac{E_y}{E_x} simplifies (after using the condition on V(P)) to 1 so that ϕ=tan1(1)=45.\phi=\tan^{-1}(1)=45^\circ.

A detailed integration (using standard techniques appropriate for JEE/NEET level) confirms this result.