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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

Determine the magnitude of the electric field at point P in the...

Determine the magnitude of the electric field at point PP in the configurations illustrated in the figure for d≫ad \gg a. Assume 2qa=p2qa = p.
Determine the magnitude of the electric field at point P in the configurations illustrated in the figure for d a .

Options

  1. A(a) q2πε0d2\dfrac{q}{2\pi\varepsilon_0 d^2}
    (b) p2πε0d3\dfrac{p}{2\pi\varepsilon_0 d^3}
    (c) 12πε0d3q2d2+p2\dfrac{1}{2\pi\varepsilon_0 d^3}\sqrt{q^2 d^2 + p^2}
  2. B(a) q4πε0d2\dfrac{q}{4\pi\varepsilon_0 d^2}
    (b) p4πε0d3\dfrac{p}{4\pi\varepsilon_0 d^3}
    (c) 14πε0d3q2d2+p2\dfrac{1}{4\pi\varepsilon_0 d^3}\sqrt{q^2 d^2 + p^2}
  3. C(a) q4πε0d2\dfrac{q}{4\pi\varepsilon_0 d^2}
    (b) 2p4πε0d3\dfrac{2p}{4\pi\varepsilon_0 d^3}
    (c) 14πε0d3q2d2+4p2\dfrac{1}{4\pi\varepsilon_0 d^3}\sqrt{q^2 d^2 + 4p^2}
  4. D(a) q4πε0d2\dfrac{q}{4\pi\varepsilon_0 d^2}
    (b) p4πε0d3\dfrac{p}{4\pi\varepsilon_0 d^3}
    (c) 14πε0d3(qd+p)\dfrac{1}{4\pi\varepsilon_0 d^3}(qd + p)

Correct answer

B. (a) q4πε0d2\dfrac{q}{4\pi\varepsilon_0 d^2}
(b) p4πε0d3\dfrac{p}{4\pi\varepsilon_0 d^3}
(c) 14πε0d3q2d2+p2\dfrac{1}{4\pi\varepsilon_0 d^3}\sqrt{q^2 d^2 + p^2}

Step-by-step solution

For configuration (a):

The electric field at point P due to a point charge qq at distance dd is:

Ea=14πε0qd2E_a = \dfrac{1}{4\pi\varepsilon_0} \dfrac{q}{d^2}

For configuration (b):

The system is an electric dipole with charges −q-q and +q+q separated by 2a2a. Point P is on the equatorial line at distance dd.

The electric field for d≫ad \gg a is:

Eb=14πε0pd3E_b = \dfrac{1}{4\pi\varepsilon_0} \dfrac{p}{d^3}

where p=2qap = 2qa is the dipole moment.

For configuration (c):

The system has three charges: −q-q at x=−ax = -a, +q+q at x=0x = 0, and +q+q at x=ax = a. Point P is at (0,d)(0, d).

The field due to the central charge +q+q is:

E⃗1=14πε0qd2j^\vec{E}_1 = \dfrac{1}{4\pi\varepsilon_0} \dfrac{q}{d^2} \hat{j}

The field due to the charge −q-q at (−a,0)(-a, 0) is:

E⃗2=14πε0−q(a2+d2)3/2(ai^+dj^)\vec{E}_2 = \dfrac{1}{4\pi\varepsilon_0} \dfrac{-q}{(a^2 + d^2)^{3/2}} (a\hat{i} + d\hat{j})

The field due to the charge +q+q at (a,0)(a, 0) is:

E⃗3=14πε0q(a2+d2)3/2(−ai^+dj^)\vec{E}_3 = \dfrac{1}{4\pi\varepsilon_0} \dfrac{q}{(a^2 + d^2)^{3/2}} (-a\hat{i} + d\hat{j})

The sum of the fields from the outer charges is:

E⃗2+E⃗3=14πε0q(a2+d2)3/2(−2ai^)=−14πε0p(a2+d2)3/2i^\vec{E}_2 + \vec{E}_3 = \dfrac{1}{4\pi\varepsilon_0} \dfrac{q}{(a^2 + d^2)^{3/2}} (-2a\hat{i}) = -\dfrac{1}{4\pi\varepsilon_0} \dfrac{p}{(a^2 + d^2)^{3/2}} \hat{i}

For d≫ad \gg a, this approximates to:

E⃗23≈−14πε0pd3i^\vec{E}_{23} \approx -\dfrac{1}{4\pi\varepsilon_0} \dfrac{p}{d^3} \hat{i}

The total electric field at P is:

E⃗c=E⃗1+E⃗23≈−14πε0pd3i^+14πε0qd2j^\vec{E}_c = \vec{E}_1 + \vec{E}_{23} \approx -\dfrac{1}{4\pi\varepsilon_0} \dfrac{p}{d^3} \hat{i} + \dfrac{1}{4\pi\varepsilon_0} \dfrac{q}{d^2} \hat{j}

The magnitude of the total electric field is:

Ec=(p4πε0d3)2+(q4πε0d2)2=14πε0d3p2+q2d2E_c = \sqrt{\left( \dfrac{p}{4\pi\varepsilon_0 d^3} \right)^2 + \left( \dfrac{q}{4\pi\varepsilon_0 d^2} \right)^2} = \dfrac{1}{4\pi\varepsilon_0 d^3} \sqrt{p^2 + q^2 d^2}

Answer: (a) q4πε0d2\dfrac{q}{4\pi\varepsilon_0 d^2}
(b) p4πε0d3\dfrac{p}{4\pi\varepsilon_0 d^3}
(c) 14πε0d3q2d2+p2\dfrac{1}{4\pi\varepsilon_0 d^3}\sqrt{q^2 d^2 + p^2}
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