Electric Charge — Question 7

Section 21-1 · Physics pages 3384–3385

Question 7 A global reversal of charge signs leaves pair forces unchanged Four fixed point charges have arbitrary nonzero signed values qi. At fixed geometry, assume the force from pair i, j is a geometric vector factor times qiqj. Compare two operations: reverse all four charges, or reverse only q1. q1 q2 q3 q4 Schematic; labels, not drawing lengths, specify the data. (a) Derive the effect of global reversal on every pair force and on the net force of each particle. (b) If the original force on particle 1 is (2ˆi −5ˆj) mN, find it after reversal of q1 alone. Determine whether net forces on particles 2 through 4 must also reverse.
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Question 7 - Solution A global reversal of charge signs leaves pair forces unchanged q1 q2 q3 q4 (a) Method and calculation Fij = Gijqiqj, (−qi)(−qj) = qiqj. Fij′ = Fij, Fi′ = ∑ j̸=i Fij = Fi. (b) Interpretation and further calculation F1′ = −F1 = (−2ˆi + 5ˆj) mN. i̸ = 1 : Fi′ = Fi −2Fi1. For each other particle only the contribution from particle 1 reverses. Its whole resultant generally does not. Physical check The symmetry statement applies to electrostatic forces; an external force not reversed with the charges would not necessarily share it.

Question 7

A global reversal of charge signs leaves pair forces unchanged

Four fixed point charges have arbitrary nonzero signed values qiq_i. At fixed geometry, assume the force from pair i,ji,j is a geometric vector factor times qiqjq_iq_j. Compare two operations: reverse all four charges, or reverse only q1q_1.

Diagram shown in the original SVG worksheet.

  1. Derive the effect of global reversal on every pair force and on the net force of each particle.

  2. If the original force on particle 1 is (2𝒊̂−5𝒋̂)(2\hat{\mathbf i}-5\hat{\mathbf j}) mN, find it after reversal of q1q_1 alone. Determine whether net forces on particles 2 through 4 must also reverse.

Question 7 - Solution

A global reversal of charge signs leaves pair forces unchanged

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑭ij=𝑮ijqiqj,(−qi)(−qj)=qiqj.\mathbf F_{ij}=\mathbf G_{ij}q_iq_j,\quad(-q_i)(-q_j)=q_iq_j.𝑭ij′=𝑭ij,𝑭i′=∑j≠i𝑭ij=𝑭i.\mathbf F_{ij}\prime=\mathbf F_{ij},\quad\mathbf F_i\prime=\sum_{j\ne i}\mathbf F_{ij}=\mathbf F_i.

(b) Interpretation and further calculation

𝑭1′=−𝑭1=(−2𝒊̂+5𝒋̂)mN.\mathbf F_1\prime=-\mathbf F_1=(-2\hat{\mathbf i}+5\hat{\mathbf j})\,\mathrm{mN}.i≠1:𝑭i′=𝑭i−2𝑭i1.i\ne1:\quad\mathbf F_i\prime=\mathbf F_i-2\mathbf F_{i1}.For each other particle only the contribution from particle 1 reverses. Its whole resultant generally does not.

Physical check

The symmetry statement applies to electrostatic forces; an external force not reversed with the charges would not necessarily share it.