Crossed Fields: Discovery of the Electron — Question 4

Section 28-3 · Physics pages 4518–4519

Question 4 A short velocity selector has a calculable finite acceptance band In a selector with downward E and into-page B, positive particles enter with speed v0 + δv, where v0 = E/B and |δv| ≪v0. The field length is L and an exit slit admits transverse displacement |y| ≤a. Assume |q|BL/(mv0) ≪1, so transverse acceleration is nearly constant during transit. positive plate negative plate⃗ v⃗ E Schematic; labels, not drawing lengths, specify the data. (a) Derive the leading exit displacement in terms of delta v. (b) Find the approximate allowed fractional speed error and state how it changes when L doubles.
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Question 4 - Solution A short velocity selector has a calculable finite acceptance band positive plate negative plate⃗ v⃗ E (a) Method and calculation Fy = q[B(v0 + δv) −E] = qBδv, t ≃L/v0. y ≃qBδv 2m L2 v2 0 . (b) Interpretation and further calculation |δv| v0 ≲2mav0 |q|BL2 . L′ = 2L ⇒fractional acceptance′ = 1 4(original), within the short-transit regime. Physical check This is a controlled short-transit approximation, not the exact trajectory through a long crossed-field region.

Question 4

A short velocity selector has a calculable finite acceptance band

In a selector with downward E and into-page B, positive particles enter with speed v0+δvv_0+\delta v, where v0=E/Bv_0=E/B and |δv|≪v0|\delta v|\ll v_0. The field length is L and an exit slit admits transverse displacement |y|≤a|y|\le a. Assume |q|BL/(mv0)≪1|q|BL/(mv_0)\ll1, so transverse acceleration is nearly constant during transit.

Diagram shown in the original SVG worksheet.

  1. Derive the leading exit displacement in terms of delta v.

  2. Find the approximate allowed fractional speed error and state how it changes when L doubles.

Question 4 - Solution

A short velocity selector has a calculable finite acceptance band

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Fy=q[B(v0+δv)−E]=qBδv,t≃L/v0.F_y=q[B(v_0+\delta v)-E]=qB\delta v,\quad t\simeq L/v_0.y≃qBδv2mL2v02.y\simeq\frac{qB\delta v}{2m}\frac{L^2}{v_0^2}.

(b) Interpretation and further calculation

|δv|v0≲2mav0|q|BL2.\frac{|\delta v|}{v_0}\lesssim\frac{2mav_0}{|q|BL^2}.L′=2L⇒fractional acceptance′=14(original),within the short-transit regime.L\prime=2L\Rightarrow\text{fractional acceptance}\prime=\tfrac14\text{(original)},\quad\text{within the short-transit regime}.

Physical check

This is a controlled short-transit approximation, not the exact trajectory through a long crossed-field region.