The Magnetic Dipole Moment — Question 7

Section 28-9 · Physics pages 4644–4645

Question 7 A field gradient and a guide can provide stable axial dipole equilibrium against gravity A dipole of mass m and fixed upward moment mu moves on a frictionless vertical guide that also fixes its orientation. Along the guide, Bz(z) = B0 + Gz −Hz2/2, with H positive. Gravity is downward with acceleration g. The expression specifies only the on-axis field, not its off-axis components.⃗ µ mg z zeq Schematic; labels, not drawing lengths, specify the data. (a) Find the equilibrium height and small-oscillation angular frequency along the guide. (b) Evaluate them for m=.0200 kg, mu=.500 ampere square metre, G=2.00 T/m, H=10.0 T/m squared and g=9.81 m/s squared.
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Question 7 - Solution A field gradient and a guide can provide stable axial dipole equilibrium against gravity⃗ µ mg z zeq (a) Method and calculation U(z) = mgz −µBz(z), Fz = µ(G −Hz) −mg. zeq = G −mg/µ H , Fz = −µH(z −zeq), Ω= √ µH/m. (b) Interpretation and further calculation zeq = 2.00 −(.0200)(9.81)/.500 10.0 = .16076 m. Ω= √ (.500)(10.0)/.0200 = 15.8114 rad/s. Physical check This establishes stability only along the imposed guide; it is not a claim of unconstrained three-dimensional magnetic levitation.

Question 7

A field gradient and a guide can provide stable axial dipole equilibrium against gravity

A dipole of mass m and fixed upward moment mu moves on a frictionless vertical guide that also fixes its orientation. Along the guide, Bz(z)=B0+Gz−Hz2/2B_z(z)=B_0+Gz-Hz^2/2, with H positive. Gravity is downward with acceleration g. The expression specifies only the on-axis field, not its off-axis components.

Diagram shown in the original SVG worksheet.

  1. Find the equilibrium height and small-oscillation angular frequency along the guide.

  2. Evaluate them for m=.0200 kg, mu=.500 ampere square metre, G=2.00 T/m, H=10.0 T/m squared and g=9.81 m/s squared.

Question 7 - Solution

A field gradient and a guide can provide stable axial dipole equilibrium against gravity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U(z)=mgz−μBz(z),Fz=μ(G−Hz)−mg.U(z)=mgz-\mu B_z(z),\quad F_z=\mu(G-Hz)-mg.zeq=G−mg/μH,Fz=−μH(z−zeq),Ω=μH/m.z_{\mathrm{eq}}=\frac{G-mg/\mu}{H},\quad F_z=-\mu H(z-z_{\mathrm{eq}}),\quad\Omega=\sqrt{\mu H/m}.

(b) Interpretation and further calculation

zeq=2.00−(.0200)(9.81)/.50010.0=.16076m.z_{\mathrm{eq}}=\frac{2.00-(.0200)(9.81)/.500}{10.0}=.16076\,\mathrm m.Ω=(.500)(10.0)/.0200=15.8114rad/s.\Omega=\sqrt{(.500)(10.0)/.0200}=15.8114\,\mathrm{rad/s}.

Physical check

This establishes stability only along the imposed guide; it is not a claim of unconstrained three-dimensional magnetic levitation.