JEE Challenger
More from Electric Charges and Fields

Electric Field and Potential of Three Charges on Circle

Consider a system of three charges q3,q3\frac{q}{3}, \frac{q}{3} and −2q3-\frac{2q}{3} placed at points A, B and C, respectively, as shown in the figure. Take O to be the centre of the circle of radius RR and angle CAB=60∘\text{CAB} = 60^\circ

Diagram 0

Options

A

The electric field at point O is q8πε0R2\frac{q}{8\pi\varepsilon_0 R^2} directed along the negative x-axis

B

The potential energy of the system is zero

C

The magnitude of the force between the charges at C and B is q254πε0R2\frac{q^2}{54\pi\varepsilon_0 R^2}

Correct
D

The potential at point O is q12πε0R\frac{q}{12\pi\varepsilon_0 R}

Step-by-Step Solution

To determine the correct option, we analyze the given system of charges using geometric and electrostatic principles.

1. Distance Between Charges at CC and BB

The three points AA, BB, and CC lie on a circle of radius RR centered at OO.
The angle subtended by the chord CBCB at the point AA on the circumference is given as:
∠CAB=60∘\angle \text{CAB} = 60^\circ

By the inscribed angle theorem, the angle subtended by the arc CBCB at the center OO is twice the angle subtended at the circumference:
∠COB=2×∠CAB=2×60∘=120∘\angle \text{COB} = 2 \times \angle \text{CAB} = 2 \times 60^\circ = 120^\circ

Now, considering triangle △COB\triangle COB, where OC=OB=ROC = OB = R and ∠COB=120∘\angle \text{COB} = 120^\circ, we apply the Law of Cosines to find the distance CBCB:
CB2=OC2+OB2−2(OC)(OB)cos⁡(∠COB)CB^2 = OC^2 + OB^2 - 2(OC)(OB)\cos(\angle \text{COB})
CB2=R2+R2−2R2cos⁡(120∘)CB^2 = R^2 + R^2 - 2R^2 \cos(120^\circ)
CB2=2R2−2R2(−12)=3R2CB^2 = 2R^2 - 2R^2 \left(-\frac{1}{2}\right) = 3R^2
CB=3RCB = \sqrt{3}R


2. Force Between Charges at CC and BB

The charges placed at points BB and CC are:
qB=q3,qC=−2q3q_B = \frac{q}{3}, \quad q_C = -\frac{2q}{3}

Using Coulomb's Law, the magnitude of the electrostatic force FCBF_{CB} between the charges at CC and BB is:
FCB=14πε0∣qC⋅qB∣CB2F_{CB} = \frac{1}{4\pi\varepsilon_0} \frac{|q_C \cdot q_B|}{CB^2}

Substitute the values of qBq_B, qCq_C, and CB2CB^2:
FCB=14πε0∣−2q3∣⋅∣q3∣3R2F_{CB} = \frac{1}{4\pi\varepsilon_0} \frac{\left|-\frac{2q}{3}\right| \cdot \left|\frac{q}{3}\right|}{3R^2}
FCB=14πε02q293R2F_{CB} = \frac{1}{4\pi\varepsilon_0} \frac{\frac{2q^2}{9}}{3R^2}
FCB=2q2108πε0R2=q254πε0R2F_{CB} = \frac{2q^2}{108\pi\varepsilon_0 R^2} = \frac{q^2}{54\pi\varepsilon_0 R^2}

This matches statement (C).


3. Verification of Other Options

  • Electric Potential at Point OO (Option D):
    VO=14πε0R(qA+qB+qC)=14πε0R(q3+q3−2q3)=0V_O = \frac{1}{4\pi\varepsilon_0 R} (q_A + q_B + q_C) = \frac{1}{4\pi\varepsilon_0 R} \left(\frac{q}{3} + \frac{q}{3} - \frac{2q}{3}\right) = 0
    Hence, Option D is incorrect.

  • Potential Energy of the System (Option B):
    The potential energy depends on the pairwise distances rAB,rBC,rCAr_{AB}, r_{BC}, r_{CA}. Since the net potential energy is generally non-zero, Option B is incorrect.

  • Electric Field at Point OO (Option A):
    The vector sum of electric fields depends on the explicit position vectors of A,B,CA, B, C, which are not given to yield a net magnitude of q8πε0R2\frac{q}{8\pi\varepsilon_0 R^2} along the negative x-axis in general.

Thus, the correct statement is C.