Calculating the Field from the Potential — Question 5

Section 24-9 · Physics pages 3960–3961

Question 5 A smooth field zero can be stable in one direction and unstable in another A vacuum-region potential is V = A(x2 + y2 −2z2) with A>0. A positive particle q of mass m is near the origin. x z Schematic; labels, not drawing lengths, specify the data. (a) Find E and the linear equations of motion. (b) Find transverse oscillation frequencies and the axial exponential growth rate; explain why this is not a stable three-dimensional trap.
Show solutionHide solution
Question 5 - Solution A smooth field zero can be stable in one direction and unstable in another x z (a) Method and calculation E = −2Axˆx −2Ayˆy + 4Azˆz. m¨x = −2qAx, m¨y = −2qAy, m¨z = 4qAz. (b) Interpretation and further calculation ωx = ωy = √ 2qA/m, z = C+eγt + C−e−γt, γ = √ 4qA/m. ∇2V = 2A + 2A −4A = 0. The axial instability accompanies transverse confinement. Physical check A field zero alone gives equilibrium, while curvature signs determine stability in each direction.

Question 5

A smooth field zero can be stable in one direction and unstable in another

A vacuum-region potential is V=A(x2+y2−2z2)V=A(x^2+y^2-2z^2) with A>0. A positive particle q of mass m is near the origin.

Diagram shown in the original SVG worksheet.

  1. Find E and the linear equations of motion.

  2. Find transverse oscillation frequencies and the axial exponential growth rate; explain why this is not a stable three-dimensional trap.

Question 5 - Solution

A smooth field zero can be stable in one direction and unstable in another

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑬=−2Ax𝒙̂−2Ay𝒚̂+4Az𝒛̂.\mathbf E=-2Ax\hat{\mathbf x}-2Ay\hat{\mathbf y}+4Az\hat{\mathbf z}.mẍ=−2qAx,mÿ=−2qAy,mz̈=4qAz.m\ddot x=-2qAx,\quad m\ddot y=-2qAy,\quad m\ddot z=4qAz.

(b) Interpretation and further calculation

ωx=ωy=2qA/m,z=C+eγt+C−e−γt,γ=4qA/m.\omega_x=\omega_y=\sqrt{2qA/m},\quad z=C_+e^{\gamma t}+C_-e^{-\gamma t},\quad\gamma=\sqrt{4qA/m}.∇2V=2A+2A−4A=0.\nabla^2V=2A+2A-4A=0.The axial instability accompanies transverse confinement.

Physical check

A field zero alone gives equilibrium, while curvature signs determine stability in each direction.