The Definition of B — Question 10

Section 28-2 · Physics pages 4510–4511

Question 10 Two orthogonal near-null force tests place a finite upper bound on the entire field A charge of magnitude q is tested with velocities vˆx and vˆy. In each trial the magnetic-force magnitude is no greater than Fmax. Assume q and v are nonzero and no other forces act. Set b = Fmax/(qv). x y⃗ v1⃗ v2 Schematic; labels, not drawing lengths, specify the data. (a) Derive inequalities for the field components and the sharp upper bound on B. (b) Give a field that attains the bound and explain the exact-null limit.
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Question 10 - Solution Two orthogonal near-null force tests place a finite upper bound on the entire field x y⃗ v1⃗ v2 (a) Method and calculation B2 y + B2 z ≤b2, B2 x + B2 z ≤b2. B2 + B2 z ≤2b2 ⇒B ≤ √ 2 b. (b) Interpretation and further calculation⃗ B = bˆx + bˆy : |⃗Fx| = |⃗Fy| = qvb = Fmax. Fmax = 0 ⇒B = 0. Physical check One null direction permits a parallel field; two nonparallel exact-null directions exclude every nonzero field.

Question 10

Two orthogonal near-null force tests place a finite upper bound on the entire field

A charge of magnitude q is tested with velocities vx̂v\hat x and vŷv\hat y. In each trial the magnetic-force magnitude is no greater than Fmax. Assume q and v are nonzero and no other forces act. Set b=Fmax/(qv)b=F_{\max}/(qv).

Diagram shown in the original SVG worksheet.

  1. Derive inequalities for the field components and the sharp upper bound on B.

  2. Give a field that attains the bound and explain the exact-null limit.

Question 10 - Solution

Two orthogonal near-null force tests place a finite upper bound on the entire field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

By2+Bz2≤b2,Bx2+Bz2≤b2.B_y^2+B_z^2\le b^2,\quad B_x^2+B_z^2\le b^2.B2+Bz2≤2b2⇒B≤2b.B^2+B_z^2\le2b^2\Rightarrow B\le\sqrt2\,b.

(b) Interpretation and further calculation

B→=bx̂+bŷ:|F→x|=|F→y|=qvb=Fmax.\vec B=b\hat x+b\hat y:\quad|\vec F_x|=|\vec F_y|=qvb=F_{\max}.Fmax=0⇒B=0.F_{\max}=0\Rightarrow B=0.

Physical check

One null direction permits a parallel field; two nonparallel exact-null directions exclude every nonzero field.