JEE Challenger
More from Electric Charges and Fields

Electric Field Lines and Charge Magnitude Relationship

A few electric field lines for a system of two charges Q1Q_1 and Q2Q_2 fixed at two different points on the x-axis are shown in the figure. These lines suggest that

Diagram 0

Options

A

∣Q1∣>∣Q2∣|Q_1| > |Q_2|

Correct
B

∣Q1∣<∣Q2∣|Q_1| < |Q_2|

C

at a finite distance to the left of Q1Q_1 the electric field is zero

D

at a finite distance to the right of Q2Q_2 the electric field is zero

Correct

Step-by-Step Solution

Based on the provided electric field lines diagram:

  1. Sign and Magnitude of Charges:

    • The electric field lines originate from charge Q1Q_1 and terminate on charge Q2Q_2. This implies that Q1Q_1 is a positive charge and Q2Q_2 is a negative charge.
    • The number of electric field lines originating from or terminating on a charge is directly proportional to the magnitude of that charge (N∝∣Q∣N \propto |Q|).
    • In the figure, a larger number of field lines originate from Q1Q_1 than the number of lines terminating on Q2Q_2 (several lines from Q1Q_1 extend out to infinity). Therefore:
      ∣Q1∣>∣Q2∣|Q_1| > |Q_2|
    • Hence, Option (A) is correct and Option (B) is incorrect.
  2. Location of the Neutral Point (E=0E = 0):

    • The charges have opposite signs, so their electric fields between them point in the same direction (from the positive charge Q1Q_1 towards the negative charge Q2Q_2). Consequently, the electric field cannot be zero between the two charges.
    • Outside the charges along the line joining them, the fields due to Q1Q_1 and Q2Q_2 point in opposite directions. The net electric field can be zero where the magnitudes of the two fields are equal:
      E=14πε0∣Q1∣r12=14πε0∣Q2∣r22  ⟹  r1r2=∣Q1∣∣Q2∣E = \frac{1}{4\pi\varepsilon_0}\frac{|Q_1|}{r_1^2} = \frac{1}{4\pi\varepsilon_0}\frac{|Q_2|}{r_2^2} \implies \frac{r_1}{r_2} = \sqrt{\frac{|Q_1|}{|Q_2|}}
    • Since ∣Q1∣>∣Q2∣|Q_1| > |Q_2|, we must have r1>r2r_1 > r_2 for the fields to cancel each other out.
    • For points to the left of Q1Q_1, any point is closer to Q1Q_1 than to Q2Q_2 (r1<r2r_1 < r_2). Because ∣Q1∣>∣Q2∣|Q_1| > |Q_2| and r1<r2r_1 < r_2, the field due to Q1Q_1 is strictly greater than that due to Q2Q_2 at all points to the left of Q1Q_1, meaning the field can never be zero there. Thus, Option (C) is incorrect.
    • For points to the right of Q2Q_2, any point is closer to Q2Q_2 than to Q1Q_1 (r2<r1r_2 < r_1). Thus, the condition r1>r2r_1 > r_2 is satisfied, and there exists a finite distance to the right of Q2Q_2 where the two opposing electric fields cancel each other completely. Hence, Option (D) is correct.

Correct Options: A and D