Coulomb's Law — Question 2

Section 21-3 · Physics pages 3414–3415

Question 2 A force-free point between like charges is stable only along the joining line Use k = 8.99 × 109 N m2/C2; treat the specified charges as points in vacuum. Fixed charges +4.0 nC and +9.0 nC lie at x = 0 and x = 1.00 m. A positive test charge q is placed between them. Its influence on the fixed sources is neglected. x +4 nC q +9 nC Schematic; labels, not drawing lengths, specify the data. (a) Find the position where the test charge force vanishes. (b) Differentiate the longitudinal force to determine stability for small displacements along the line. Explain the force direction for a small upward displacement from that point.
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Question 2 - Solution A force-free point between like charges is stable only along the joining line x +4 nC q +9 nC (a) Method and calculation Fx = kq ( 4.0 × 10−9 x2 −9.0 × 10−9 (1 −x)2 ) = 0. 2 x = 3 1 −x ⇒x = .400 m. (b) Interpretation and further calculation dFx dx = −2kq ( 4.0 × 10−9 x3 + 9.0 × 10−9 (1 −x)3 ) < 0. δx > 0 ⇒δFx < 0, δy > 0 ⇒Fy > 0. The longitudinal force is restoring, but both positive sources push an upward-displaced positive charge farther upward. This is not a stable unconstrained three-dimensional trap. Physical check For a negative test charge the force-free location is unchanged, but the local restoring and destabilizing directions reverse.

Question 2

A force-free point between like charges is stable only along the joining line

Use k=8.99×109Nm2/C2k=8.99\times10^9\,\mathrm{N\,m^2/C^2}; treat the specified charges as points in vacuum. Fixed charges +4.0+4.0 nC and +9.0+9.0 nC lie at x=0x=0 and x=1.00x=1.00 m. A positive test charge qq is placed between them. Its influence on the fixed sources is neglected.

Diagram shown in the original SVG worksheet.

  1. Find the position where the test charge force vanishes.

  2. Differentiate the longitudinal force to determine stability for small displacements along the line. Explain the force direction for a small upward displacement from that point.

Question 2 - Solution

A force-free point between like charges is stable only along the joining line

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Fx=kq(4.0×10−9x2−9.0×10−9(1−x)2)=0.F_x=kq\left(\frac{4.0\times10^{-9}}{x^2}-\frac{9.0\times10^{-9}}{(1-x)^2}\right)=0.2x=31−x⇒x=.400m.\frac2x=\frac3{1-x}\Rightarrow x=.400\,\mathrm m.

(b) Interpretation and further calculation

dFxdx=−2kq(4.0×10−9x3+9.0×10−9(1−x)3)<0.\frac{dF_x}{dx}=-2kq\left(\frac{4.0\times10^{-9}}{x^3}+\frac{9.0\times10^{-9}}{(1-x)^3}\right)<0.δx>0⇒δFx<0,δy>0⇒Fy>0.\delta x>0\Rightarrow\delta F_x<0,\qquad\delta y>0\Rightarrow F_y>0.The longitudinal force is restoring, but both positive sources push an upward-displaced positive charge farther upward. This is not a stable unconstrained three-dimensional trap.

Physical check

For a negative test charge the force-free location is unchanged, but the local restoring and destabilizing directions reverse.