Electric Field Lines — Question 10

Section 22-2 · Physics pages 3510–3511

Question 10 A curved line supplies a local tangent, not a force toward its center of curvature At P an oriented field line has tangent direction proportional to (−1, 2) and field magnitude 90.0 N/C. A particle with charge −3.00 nC is placed at P. The drawn curve bends, but its curvature radius is not specified. P Schematic; labels, not drawing lengths, specify the data. (a) Find the field and force vectors. (b) Find the force component along a unit normal (2, 1)/ √ 5 to the field line. Explain why curvature alone does not create a normal electric force.
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Question 10 - Solution A curved line supplies a local tangent, not a force toward its center of curvature P (a) Method and calculation ˆt = (−1, 2)/ √ 5, E = 90 √ 5(−1, 2) N/C. F = 270 √ 5 (1, −2) nN ≈(120.748, −241.495) nN. (b) Interpretation and further calculation Fn = F · (2, 1) √ 5 = 270 5 (2 −2) = 0. |F| = 270 nN. A field line is a directional construction, not a wire constraining motion; its curvature does not imply centripetal acceleration of a freely moving particle. Physical check The actual acceleration is parallel or antiparallel to the local tangent, according to the charge sign.

Question 10

A curved line supplies a local tangent, not a force toward its center of curvature

At P an oriented field line has tangent direction proportional to (−1,2)(-1,2) and field magnitude 90.0 N/C. A particle with charge −3.00-3.00 nC is placed at P. The drawn curve bends, but its curvature radius is not specified.

Diagram shown in the original SVG worksheet.

  1. Find the field and force vectors.

  2. Find the force component along a unit normal (2,1)/5(2,1)/\sqrt5 to the field line. Explain why curvature alone does not create a normal electric force.

Question 10 - Solution

A curved line supplies a local tangent, not a force toward its center of curvature

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝒕̂=(−1,2)/5,𝑬=905(−1,2)N/C.\hat{\mathbf t}=(-1,2)/\sqrt5,\quad\mathbf E=\frac{90}{\sqrt5}(-1,2)\,\mathrm{N/C}.𝑭=2705(1,−2)nN≈(120.748,−241.495)nN.\mathbf F=\frac{270}{\sqrt5}(1,-2)\,\mathrm{nN}\approx(120.748,-241.495)\,\mathrm{nN}.

(b) Interpretation and further calculation

Fn=𝑭⋅(2,1)5=2705(2−2)=0.F_n=\mathbf F\cdot\frac{(2,1)}{\sqrt5}=\frac{270}{5}(2-2)=0.|𝑭|=270nN.|\mathbf F|=270\,\mathrm{nN}.A field line is a directional construction, not a wire constraining motion; its curvature does not imply centripetal acceleration of a freely moving particle.

Physical check

The actual acceleration is parallel or antiparallel to the local tangent, according to the charge sign.