Electrostatics: Numerical Problems Set (7)

easy 3 min read

Question

Two point charges q1=+4μCq_1 = +4 \mu\text{C} and q2=2μCq_2 = -2 \mu\text{C} are placed 30 cm30 \text{ cm} apart in vacuum. Find (a) the force between them, (b) the electric field at the midpoint of the line joining them, (c) the location of the point on the line where the net field is zero. Take k=9×109 N m2/C2k = 9 \times 10^9 \text{ N m}^2/\text{C}^2.

Solution — Step by Step

F=kq1q2r2=9×109×4×106×2×106(0.3)2F = \frac{k|q_1 q_2|}{r^2} = \frac{9 \times 10^9 \times 4 \times 10^{-6} \times 2 \times 10^{-6}}{(0.3)^2}

F=72×1030.09=0.8 NF = \frac{72 \times 10^{-3}}{0.09} = 0.8 \text{ N}, attractive (opposite signs).

At midpoint (r1=r2=0.15 mr_1 = r_2 = 0.15 \text{ m}), both fields point from +q1+q_1 toward q2-q_2 (positive test charge feels push from ++ and pull toward -, both in the same direction).

E1=kq1/r12=9×109×4×106/0.0225=1.6×106 N/CE_1 = kq_1/r_1^2 = 9 \times 10^9 \times 4 \times 10^{-6}/0.0225 = 1.6 \times 10^6 \text{ N/C}.

E2=kq2/r22=0.8×106 N/CE_2 = kq_2/r_2^2 = 0.8 \times 10^6 \text{ N/C}.

Enet=E1+E2=2.4×106 N/CE_{net} = E_1 + E_2 = 2.4 \times 10^6 \text{ N/C}, directed from q1q_1 toward q2q_2.

Net field is zero only outside the segment, on the side of the smaller charge (q2q_2). Let the point be at distance xx from q2q_2 on the side away from q1q_1.

Then distance from q1q_1 is x+0.3x + 0.3. Setting magnitudes equal (fields point opposite outside on this side):

kq1(x+0.3)2=kq2x2\frac{k|q_1|}{(x+0.3)^2} = \frac{k|q_2|}{x^2}

4(x+0.3)2=2x2    4x2=2(x+0.3)2\frac{4}{(x+0.3)^2} = \frac{2}{x^2} \implies 4x^2 = 2(x+0.3)^2.

2x=x+0.3\sqrt{2}\, x = x + 0.3 (taking positive root). x(21)=0.3x(\sqrt{2} - 1) = 0.3.

x=0.3/0.4140.724 mx = 0.3/0.414 \approx 0.724 \text{ m}.

Final answers: F=0.8 NF = \mathbf{0.8 \text{ N}} attractive, Emid=2.4×106 N/CE_{mid} = \mathbf{2.4 \times 10^6 \text{ N/C}}, zero point at 72.4 cm\mathbf{\approx 72.4 \text{ cm}} from q2q_2 on the far side.

Why This Works

The midpoint trick: when charges have opposite signs, their fields add at every point between them (both push/pull the test charge in the same direction). When charges have the same sign, fields subtract between them — and the zero-field point lies between them.

For zero net field with opposite signs, the point must be outside, on the side of the smaller-magnitude charge. (You’re farther from the bigger charge, so 1/r21/r^2 scaling can balance the bigger q|q|.)

Alternative Method

For part (c), use q1/d12=q2/d22|q_1|/d_1^2 = |q_2|/d_2^2 with d1/d2=q1/q2=2d_1/d_2 = \sqrt{|q_1|/|q_2|} = \sqrt{2}. With d1=d2+0.3d_1 = d_2 + 0.3, solve directly: d2=0.3/(21)0.724 md_2 = 0.3/(\sqrt{2}-1) \approx 0.724 \text{ m}.

Common Mistake

Students often look for the zero-field point between the two charges when they have opposite signs. That cannot work — between them, both fields point the same way. The zero must be outside, beyond the smaller charge. Sketch the field arrows before computing.

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