Electric Field Lines — Question 9

Section 22-2 · Physics pages 3508–3509

Question 9 An oblique counting surface must be projected perpendicular to the field The same narrow bundle of representative field lines crosses two small patches. The first has area A1 = 2.00 cm2 normal to the local field. The second has area A2 = 3.00 cm2 with its normal at 60◦to the field. The magnitude on a patch is proportional to the line count divided by its perpendicular projected area. 1 2 Schematic; labels, not drawing lengths, specify the data. (a) Find the ratio E2/E1. (b) Find the second patch area required for equal field strengths at that angle. Explain the limit as the patch becomes parallel to the field.
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Question 9 - Solution An oblique counting surface must be projected perpendicular to the field 1 2 (a) Method and calculation A2,⊥= A2 cos 60◦= 1.50 cm2. E2/E1 = A1,⊥/A2,⊥= 2.00/1.50 = 4/3. (b) Interpretation and further calculation E2 = E1 ⇒A2 cos 60◦= A1 ⇒A2 = 4.00 cm2. θ →90◦: A⊥→0. A finite field then sends vanishing line count through a fixed nearly parallel patch; keeping the count fixed would require growing patch area. Physical check This local density argument is not a count of how many decorative strokes happen to appear in the schematic.

Question 9

An oblique counting surface must be projected perpendicular to the field

The same narrow bundle of representative field lines crosses two small patches. The first has area A1=2.00A_1=2.00 cm2^2 normal to the local field. The second has area A2=3.00A_2=3.00 cm2^2 with its normal at 60∘60^\circ to the field. The magnitude on a patch is proportional to the line count divided by its perpendicular projected area.

Diagram shown in the original SVG worksheet.

  1. Find the ratio E2/E1E_2/E_1.

  2. Find the second patch area required for equal field strengths at that angle. Explain the limit as the patch becomes parallel to the field.

Question 9 - Solution

An oblique counting surface must be projected perpendicular to the field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

A2,⟂=A2cos⁡60∘=1.50cm2.A_{2,\perp}=A_2\cos60^\circ=1.50\,\mathrm{cm^2}.E2/E1=A1,⟂/A2,⟂=2.00/1.50=4/3.E_2/E_1=A_{1,\perp}/A_{2,\perp}=2.00/1.50=4/3.

(b) Interpretation and further calculation

E2=E1⇒A2cos⁡60∘=A1⇒A2=4.00cm2.E_2=E_1\Rightarrow A_2\cos60^\circ=A_1\Rightarrow A_2=4.00\,\mathrm{cm^2}.θ→90∘:A⟂→0.\theta\to90^\circ:\quad A_\perp\to0.A finite field then sends vanishing line count through a fixed nearly parallel patch; keeping the count fixed would require growing patch area.

Physical check

This local density argument is not a count of how many decorative strokes happen to appear in the schematic.