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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Electric Field and Potential

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Electric Field and Potential

A circular ring of radius r is uniformly charged with a linear...

A circular ring of radius rr is uniformly charged with a linear charge density λ\lambda. Determine the electric potential at a point on the axis located at a distance xx from the centre of the ring. Subsequently, use this potential expression to determine the electric field at the same point.

Options

  1. Arλ2ε0(r2+x2)1/2\dfrac{r\lambda}{2\varepsilon_0 (r^2 + x^2)^{1/2}}, rλx2ε0(r2+x2)3/2\dfrac{r\lambda x}{2\varepsilon_0 (r^2 + x^2)^{3/2}}
  2. Brλε0(r2+x2)1/2\dfrac{r\lambda}{\varepsilon_0 (r^2 + x^2)^{1/2}}, rλxε0(r2+x2)3/2\dfrac{r\lambda x}{\varepsilon_0 (r^2 + x^2)^{3/2}}
  3. Crλ4ε0(r2+x2)1/2\dfrac{r\lambda}{4\varepsilon_0 (r^2 + x^2)^{1/2}}, rλx4ε0(r2+x2)3/2\dfrac{r\lambda x}{4\varepsilon_0 (r^2 + x^2)^{3/2}}
  4. Drλ2ε0(r2+x2)3/2\dfrac{r\lambda}{2\varepsilon_0 (r^2 + x^2)^{3/2}}, rλx2ε0(r2+x2)5/2\dfrac{r\lambda x}{2\varepsilon_0 (r^2 + x^2)^{5/2}}

Correct answer

A. rλ2ε0(r2+x2)1/2\dfrac{r\lambda}{2\varepsilon_0 (r^2 + x^2)^{1/2}}, rλx2ε0(r2+x2)3/2\dfrac{r\lambda x}{2\varepsilon_0 (r^2 + x^2)^{3/2}}

Step-by-step solution

Consider an elemental charge dqdq on the ring of radius rr. The linear charge density is λ\lambda, so dq=λdldq = \lambda dl.

The total charge on the ring is Q=∫λdl=λ(2πr)Q = \int \lambda dl = \lambda (2\pi r).

The electric potential VV at a point on the axis at a distance xx from the centre is given by integrating the potential due to each elemental charge:

V=∫14πε0dqr2+x2V = \int \dfrac{1}{4\pi\varepsilon_0} \dfrac{dq}{\sqrt{r^2 + x^2}}

Since the distance r2+x2\sqrt{r^2 + x^2} is constant for all points on the ring:

V=14πε0r2+x2∫dq=Q4πε0r2+x2V = \dfrac{1}{4\pi\varepsilon_0 \sqrt{r^2 + x^2}} \int dq = \dfrac{Q}{4\pi\varepsilon_0 \sqrt{r^2 + x^2}}

Substituting Q=2πrλQ = 2\pi r \lambda:

V=2πrλ4πε0r2+x2=rλ2ε0(r2+x2)1/2V = \dfrac{2\pi r \lambda}{4\pi\varepsilon_0 \sqrt{r^2 + x^2}} = \dfrac{r\lambda}{2\varepsilon_0 (r^2 + x^2)^{1/2}}

The electric field EE along the axis is the negative gradient of the potential:

E = -\dfrac{dV}{dx} = -\dfrac{d}{dx} \left(\dfrac{r\lambda}{2\varepsilon_0} (r^2 + x²)^{-1/2} \right)

E=E =-\dfrac{r\lambda}{2\varepsilon_0} \left( −12(-\dfrac{1}{2} (r^2 + x^2)^{-3/2} \times 2x \right)<br><br><br><br>E = rλx2ε0(r2+x2)3/2\dfrac{r\lambda x}{2\varepsilon_0 (r^2 + x^2)^{3/2}}
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