Two point charges q1=+4μC and q2=−2μC are placed 30 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/C2.
Solution — Step by Step
F=r2k∣q1q2∣=(0.3)29×109×4×10−6×2×10−6
F=0.0972×10−3=0.8 N, attractive (opposite signs).
At midpoint (r1=r2=0.15 m), both fields point from +q1 toward −q2 (positive test charge feels push from + and pull toward −, both in the same direction).
E1=kq1/r12=9×109×4×10−6/0.0225=1.6×106 N/C.
E2=kq2/r22=0.8×106 N/C.
Enet=E1+E2=2.4×106 N/C, directed from q1 toward q2.
Net field is zero only outside the segment, on the side of the smaller charge (q2). Let the point be at distance x from q2 on the side away from q1.
Then distance from q1 is x+0.3. Setting magnitudes equal (fields point opposite outside on this side):
(x+0.3)2k∣q1∣=x2k∣q2∣
(x+0.3)24=x22⟹4x2=2(x+0.3)2.
2x=x+0.3 (taking positive root). x(2−1)=0.3.
x=0.3/0.414≈0.724 m.
Final answers:F=0.8 N attractive, Emid=2.4×106 N/C, zero point at ≈72.4 cm from q2 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/r2 scaling can balance the bigger ∣q∣.)
Alternative Method
For part (c), use ∣q1∣/d12=∣q2∣/d22 with d1/d2=∣q1∣/∣q2∣=2. With d1=d2+0.3, solve directly: d2=0.3/(2−1)≈0.724 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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