Magnetism and Electrons — Question 5

Section 32-6 · Physics pages 5280–5281

Question 5 A neutral atomic beam separates according to moment projection Neutral atoms of mass M travel at speed v through a magnet of length ell, then drift distance D. Each atom has moment projection µz = ±µB. On the beam axis ∂Bz/∂z = G is constant. Assume small deflections and fixed projections. screen v ℓ D Schematic; labels, not drawing lengths, specify the data. (a) Find the vertical displacement acquired inside the magnet. (b) Include the field-free drift and find the separation of the two spots on the screen.
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Question 5 - Solution A neutral atomic beam separates according to moment projection screen v ℓ D (a) Method and calculation Fz = µzG, az = ±µBG/M, tm = ℓ/v. zm = ±µBGℓ2 2Mv2 . (b) Interpretation and further calculation vz,exit = ±µBGℓ Mv , zscreen = ±µBGℓ Mv2 (D + ℓ/2). ∆z = 2µB|G|ℓ Mv2 (D + ℓ/2) . Physical check Neutral atoms avoid the charge-force complication of a free electron beam; the gradient model applies locally on the beam axis.

Question 5

A neutral atomic beam separates according to moment projection

Neutral atoms of mass M travel at speed v through a magnet of length ell, then drift distance D. Each atom has moment projection μz=±μB\mu_z=\pm\mu_B. On the beam axis ∂Bz/∂z=G\partial B_z/\partial z=G is constant. Assume small deflections and fixed projections.

Diagram shown in the original SVG worksheet.

  1. Find the vertical displacement acquired inside the magnet.

  2. Include the field-free drift and find the separation of the two spots on the screen.

Question 5 - Solution

A neutral atomic beam separates according to moment projection

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Fz=μzG,az=±μBG/M,tm=ℓ/v.F_z=\mu_zG,\quad a_z=\pm\mu_BG/M,\quad t_m=\ell/v.zm=±μBGℓ22Mv2.\boxed{z_m=\pm\frac{\mu_BG\ell^2}{2Mv^2}}.

(b) Interpretation and further calculation

vz,exit=±μBGℓMv,zscreen=±μBGℓMv2(D+ℓ/2).v_{z,\mathrm{exit}}=\pm\frac{\mu_BG\ell}{Mv},\quad z_{\mathrm{screen}}=\pm\frac{\mu_BG\ell}{Mv^2}(D+\ell/2).Δz=2μB|G|ℓMv2(D+ℓ/2).\boxed{\Delta z=\frac{2\mu_B|G|\ell}{Mv^2}(D+\ell/2)}.

Physical check

Neutral atoms avoid the charge-force complication of a free electron beam; the gradient model applies locally on the beam axis.