The Stern-Gerlach Experiment — Question 1

Section 40-4 · Physics pages 6632–6633

Question 1 A Stern-Gerlach force depends on the field gradient A neutral atom has a fixed adiabatic magnetic-moment projection µz = ±µ. Across the beam in the vertical direction the field magnitude is B(z) = B0 + Gz, with G > 0. Use U = −µzB and neglect spin flips. G magnet and detector Schematic; labels, not drawing lengths, specify the data. (a) Derive the vertical force for each component. (b) Compare increasing B0 at fixed G with increasing G at fixed B0.
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Question 1 - Solution A Stern-Gerlach force depends on the field gradient G magnet and detector (a) Method and calculation Fz = −∂U/∂z = µz dB/dz. Fz,± = ±µG . (b) Interpretation and further calculation ∂Fz ∂B0 G = 0 , ∂Fz ∂G B0 = µz. G →2G ⇒Fz,± →2Fz,± . Physical check A uniform bias field can define the quantization direction without separating the beam. The model describes the local field magnitude; a real magnet also has transverse field components consistent with Maxwell equations.

Question 1

A Stern-Gerlach force depends on the field gradient

A neutral atom has a fixed adiabatic magnetic-moment projection μz=±μ\mu_z=\pm\mu. Across the beam in the vertical direction the field magnitude is B(z)=B0+GzB(z)=B_0+Gz, with G>0G>0. Use U=−μzBU=-\mu_zB and neglect spin flips.

Diagram shown in the original SVG worksheet.

  1. Derive the vertical force for each component.

  2. Compare increasing B0B_0 at fixed G with increasing G at fixed B0B_0.

Question 1 - Solution

A Stern-Gerlach force depends on the field gradient

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Fz=−∂U/∂z=μzdB/dz.F_z=-\partial U/\partial z=\mu_z\,dB/dz.Fz,±=±μG.\boxed{F_{z,\pm}=\pm\mu G}.

(b) Interpretation and further calculation

∂Fz∂B0|G=0,∂Fz∂G|B0=μz.\left.\frac{\partial F_z}{\partial B_0}\right|_G=\boxed{0},\quad\left.\frac{\partial F_z}{\partial G}\right|_{B_0}=\mu_z.G→2G⇒Fz,±→2Fz,±.G\to2G\Rightarrow\boxed{F_{z,\pm}\to2F_{z,\pm}}.

Physical check

A uniform bias field can define the quantization direction without separating the beam. The model describes the local field magnitude; a real magnet also has transverse field components consistent with Maxwell equations.