A Circulating Charged Particle — Question 10

Section 28-5 · Physics pages 4570–4571

Question 10 Linear drag shrinks the speed of a magnetic orbit while the magnetic force remains work-free A nonrelativistic particle moves perpendicular to uniform B and also experiences isotropic drag⃗ Fd = −b⃗v, with b positive. Initially its speed is v0. Ignore every other force and define ω = |q|B/m. shrinking trajectory uniform⃗B, drag −b⃗v Schematic; labels, not drawing lengths, specify the data. (a) Derive its speed and kinetic energy as functions of time. (b) Find its total path length before asymptotic rest and the heat transferred to the drag medium; explain which force supplies the energy loss.
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Question 10 - Solution Linear drag shrinks the speed of a magnetic orbit while the magnetic force remains work-free shrinking trajectory uniform⃗B, drag −b⃗v (a) Method and calculation dK dt =⃗v · (q⃗v ×⃗B −b⃗v) = −bv2 = −2b mK. K(t) = 1 2mv2 0e−2bt/m, v(t) = v0e−bt/m. (b) Interpretation and further calculation stotal = ∫∞ 0 v0e−bt/m dt = mv0/b. Qmedium = K(0) −K(∞) = 1 2mv2 0, WB = 0. Physical check A shrinking orbit does not imply magnetic work when an additional dissipative force is present.

Question 10

Linear drag shrinks the speed of a magnetic orbit while the magnetic force remains work-free

A nonrelativistic particle moves perpendicular to uniform B and also experiences isotropic drag F→d=−bv→\vec F_d=-b\vec v, with b positive. Initially its speed is v0. Ignore every other force and define ω=|q|B/m\omega=|q|B/m.

Diagram shown in the original SVG worksheet.

  1. Derive its speed and kinetic energy as functions of time.

  2. Find its total path length before asymptotic rest and the heat transferred to the drag medium; explain which force supplies the energy loss.

Question 10 - Solution

Linear drag shrinks the speed of a magnetic orbit while the magnetic force remains work-free

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dKdt=v→⋅(qv→×B→−bv→)=−bv2=−2bmK.\frac{dK}{dt}=\vec v\cdot(q\vec v\times\vec B-b\vec v)=-bv^2=-\frac{2b}{m}K.K(t)=12mv02e−2bt/m,v(t)=v0e−bt/m.K(t)=\tfrac12mv_0^2e^{-2bt/m},\quad v(t)=v_0e^{-bt/m}.

(b) Interpretation and further calculation

stotal=∫0∞v0e−bt/mdt=mv0/b.s_{\mathrm{total}}=\int_0^\infty v_0e^{-bt/m}\,dt=mv_0/b.Qmedium=K(0)−K(∞)=12mv02,WB=0.Q_{\mathrm{medium}}=K(0)-K(\infty)=\tfrac12mv_0^2,\quad W_B=0.

Physical check

A shrinking orbit does not imply magnetic work when an additional dissipative force is present.