A Point Charge in an Electric Field — Question 1

Section 22-7 · Physics pages 3592–3593

Question 1 A deflector followed by free drift measures charge-to-mass ratio A nonrelativistic particle enters a uniform field Eˆy with velocity vˆx. The field occupies horizontal length L and is followed by a field-free drift distance D. Ignore gravity, edge fields and source disturbance. A screen measures signed displacement Y from the undeflected path. L D Geometry of deflection and drift; the illustrated upward branch corresponds to positive q. (a) Derive Y including both the in-field deflection and drift contribution. (b) Infer q/m for E = 200 N/C, v = 2.00 × 105 m/s, L = .100 m, D = .200 m and Y = −.00500 m.
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Question 1 - Solution A deflector followed by free drift measures charge-to-mass ratio L D (a) Method and calculation tL = L/v, ay = qE/m, yL = 1 2ay(L/v)2, vy,L = ayL/v. Y = yL + vy,LD/v = qE mv2 L(D + L/2). (b) Interpretation and further calculation q m = Y v2 EL(D + L/2) = −4.00 × 107 C/kg. Y < 0, E > 0 ⇒q < 0. Ignoring drift would overestimate the magnitude inferred for q/m, because the particle keeps its acquired transverse velocity after leaving the field. Physical check Horizontal speed remains constant because the prescribed field has no x component.

Question 1

A deflector followed by free drift measures charge-to-mass ratio

A nonrelativistic particle enters a uniform field E𝒚̂E\hat{\mathbf y} with velocity v𝒙̂v\hat{\mathbf x}. The field occupies horizontal length L and is followed by a field-free drift distance D. Ignore gravity, edge fields and source disturbance. A screen measures signed displacement Y from the undeflected path.

Diagram shown in the original SVG worksheet.

  1. Derive Y including both the in-field deflection and drift contribution.

  2. Infer q/mq/m for E=200E=200 N/C, v=2.00×105v=2.00\times10^5 m/s, L=.100L=.100 m, D=.200D=.200 m and Y=−.00500Y=-.00500 m.

Question 1 - Solution

A deflector followed by free drift measures charge-to-mass ratio

Diagram shown in the original SVG worksheet.

(a) Method and calculation

tL=L/v,ay=qE/m,yL=12ay(L/v)2,vy,L=ayL/v.t_L=L/v,\quad a_y=qE/m,\quad y_L=\tfrac12a_y(L/v)^2,\quad v_{y,L}=a_yL/v.Y=yL+vy,LD/v=qEmv2L(D+L/2).Y=y_L+v_{y,L}D/v=\frac{qE}{mv^2}L(D+L/2).

(b) Interpretation and further calculation

qm=Yv2EL(D+L/2)=−4.00×107C/kg.\frac qm=\frac{Yv^2}{EL(D+L/2)}=-4.00\times10^7\,\mathrm{C/kg}.Y<0,E>0⇒q<0.Y<0,E>0\Rightarrow q<0.Ignoring drift would overestimate the magnitude inferred for q/mq/m, because the particle keeps its acquired transverse velocity after leaving the field.

Physical check

Horizontal speed remains constant because the prescribed field has no x component.