Magnets — Question 5

Section 32-5 · Physics pages 5260–5261

Question 5 A field gradient translates a magnet even at zero torque A small permanent dipole is held parallel to +x on the symmetry axis of an external field whose on-axis magnitude is B(x) = B0 + ax + bx2, positive in the region of interest. Its fixed moment is mˆx. x m on-axis B(x) Schematic; labels, not drawing lengths, specify the data. (a) Find its potential energy, axial force, and torque on the axis. (b) Find the axial equilibrium and its stability; obtain the frequency for mass M when stable.
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Question 5 - Solution A field gradient translates a magnet even at zero torque x m on-axis B(x) (a) Method and calculation U(x) = −m(B0 + ax + bx2), Fx = m(a + 2bx) . τ = m × B = 0 . (b) Interpretation and further calculation x∗= −a/(2b), U′′ = −2mb > 0 ⇐⇒b < 0. ωx = √ −2mb/M (b < 0). Physical check This is constrained one-dimensional stability; it does not establish stability against rotation or transverse motion.

Question 5

A field gradient translates a magnet even at zero torque

A small permanent dipole is held parallel to +x on the symmetry axis of an external field whose on-axis magnitude is B(x)=B0+ax+bx2B(x)=B_0+ax+bx^2, positive in the region of interest. Its fixed moment is mx̂m\hat x.

Diagram shown in the original SVG worksheet.

  1. Find its potential energy, axial force, and torque on the axis.

  2. Find the axial equilibrium and its stability; obtain the frequency for mass M when stable.

Question 5 - Solution

A field gradient translates a magnet even at zero torque

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U(x)=−m(B0+ax+bx2),Fx=m(a+2bx).U(x)=-m(B_0+ax+bx^2),\qquad\boxed{F_x=m(a+2bx)}.𝝉=𝒎×𝑩=0.\boxed{\boldsymbol\tau=\mathbf m\times\mathbf B=0}.

(b) Interpretation and further calculation

x*=−a/(2b),U′′=−2mb>0⇔b<0.x_*=-a/(2b),\qquad U^{\prime\prime}=-2mb>0\iff b<0.ωx=−2mb/M(b<0).\boxed{\omega_x=\sqrt{-2mb/M}}\quad(b<0).

Physical check

This is constrained one-dimensional stability; it does not establish stability against rotation or transverse motion.