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Question: Three points charges are placed at the corners of an equilateral triangle of side L as shown in the ...

Three points charges are placed at the corners of an equilateral triangle of side L as shown in the figure.

  • The potential at the centroid of the triangle is zero.
  • The electric field at the centroid of the triangle is zero.
  • The dipole moment of the system is 2qL\sqrt{2}qL.
  • The dipole moment of the system is 3qL\sqrt{3}qL.
A

The potential at the centroid of the triangle is zero.

B

The electric field at the centroid of the triangle is zero.

C

The dipole moment of the system is 2qL\sqrt{2}qL.

D

The dipole moment of the system is 3qL\sqrt{3}qL.

Answer

The potential at the centroid of the triangle is zero. The dipole moment of the system is 3qL\sqrt{3}qL.

Explanation

Solution

Let the vertices of the equilateral triangle be A, B, and C. Assume charges +q are at A and B, and -2q is at C.

Statement 1: Potential at the centroid is zero.

The distance from each vertex to the centroid is r=L3r = \frac{L}{\sqrt{3}}. The potential at the centroid O is:

VO=14πϵ0(qArA+qBrB+qCrC)V_O = \frac{1}{4\pi\epsilon_0} \left( \frac{q_A}{r_A} + \frac{q_B}{r_B} + \frac{q_C}{r_C} \right)

VO=14πϵ0(+qL/3++qL/3+2qL/3)=0V_O = \frac{1}{4\pi\epsilon_0} \left( \frac{+q}{L/\sqrt{3}} + \frac{+q}{L/\sqrt{3}} + \frac{-2q}{L/\sqrt{3}} \right) = 0

Statement 2: Electric field at the centroid is zero.

The electric field at the centroid is the vector sum of the electric fields due to each charge.

EA=14πϵ03qL2E_A = \frac{1}{4\pi\epsilon_0} \frac{3q}{L^2}, directed away from A.

EB=14πϵ03qL2E_B = \frac{1}{4\pi\epsilon_0} \frac{3q}{L^2}, directed away from B.

EC=14πϵ06qL2E_C = \frac{1}{4\pi\epsilon_0} \frac{6q}{L^2}, directed towards C.

The resultant electric field is non-zero.

Statement 3 & 4: Dipole moment of the system.

The total charge of the system is 0. Place the origin at vertex C.

P=qArA+qBrB+qCrC\vec{P} = q_A \vec{r}_A + q_B \vec{r}_B + q_C \vec{r}_C

P=q(L/2,L3/2)+q(L/2,L3/2)+(2q)(0,0)\vec{P} = q (-L/2, L\sqrt{3}/2) + q (L/2, L\sqrt{3}/2) + (-2q) (0,0)

P=(0,qL3)\vec{P} = (0, qL\sqrt{3})

The magnitude of the dipole moment is P=3qL|\vec{P}| = \sqrt{3} qL.

Therefore, statements 1 and 4 are correct.