Induced Magnetic Fields — Question 7

Section 32-2 · Physics pages 5204–5205

Question 7 A quasistatic capacitor field has a small magnetic-to-electric energy scale A uniform axial vacuum field oscillates with amplitude E0 and angular frequency omega in radius a. Its induced magnetic peak at the edge is Bp = aωE0/(2c2). Compare separately maximized energy densities, not simultaneous values. a r ⊙Ez(t) Schematic; labels, not drawing lengths, specify the data. (a) Find uB,max/uE,max using c−2 = µ0ϵ0. (b) Evaluate the ratio for aω/c = .0200 and interpret the quasistatic scale.
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Question 7 - Solution A quasistatic capacitor field has a small magnetic-to-electric energy scale a r ⊙Ez(t) (a) Method and calculation uB,max = B2 p/(2µ0), uE,max = ϵ0E2 0/2. uB,max/uE,max = (cBp/E0)2 = (aω/(2c))2 . (b) Interpretation and further calculation aω/c = .0200 ⇒(aω/(2c))2 = .000100. uB,max/uE,max = 10−4 . Physical check Small size compared with the electromagnetic variation length supports the leading quasistatic approximation.

Question 7

A quasistatic capacitor field has a small magnetic-to-electric energy scale

A uniform axial vacuum field oscillates with amplitude E0 and angular frequency omega in radius a. Its induced magnetic peak at the edge is Bp=aωE0/(2c2)B_p=a\omega E_0/(2c^2). Compare separately maximized energy densities, not simultaneous values.

Diagram shown in the original SVG worksheet.

  1. Find uB,max/uE,maxu_{B,\max}/u_{E,\max} using c−2=μ0ϵ0c^{-2}=\mu_0\epsilon_0.

  2. Evaluate the ratio for aω/c=.0200a\omega/c=.0200 and interpret the quasistatic scale.

Question 7 - Solution

A quasistatic capacitor field has a small magnetic-to-electric energy scale

Diagram shown in the original SVG worksheet.

(a) Method and calculation

uB,max=Bp2/(2μ0),uE,max=ϵ0E02/2.u_{B,\max}=B_p^2/(2\mu_0),\quad u_{E,\max}=\epsilon_0E_0^2/2.uB,max/uE,max=(cBp/E0)2=(aω/(2c))2.\boxed{u_{B,\max}/u_{E,\max}=(cB_p/E_0)^2=(a\omega/(2c))^2}.

(b) Interpretation and further calculation

aω/c=.0200⇒(aω/(2c))2=.000100.a\omega/c=.0200\Rightarrow(a\omega/(2c))^2=.000100.uB,max/uE,max=10−4.\boxed{u_{B,\max}/u_{E,\max}=10^{-4}}.

Physical check

Small size compared with the electromagnetic variation length supports the leading quasistatic approximation.