Energy in Simple Harmonic Motion — Question 8

Section 15-3 · Physics pages 2286–2287

Question 8 A weak quartic term changes turning-point energy before it changes the center A conservative oscillator has U(x) = kx2/2 + λx4/4, with k, λ > 0, and turns at x = ±A. Its mass is m. x U Quartic potential (solid) and its quadratic approximation (dashed). (a) Find total energy and speed at equilibrium. Compare the result with the harmonic prediction for the same amplitude. (b) Find the condition on A for the quartic contribution to turning-point energy to be at most 5% of the quadratic contribution. Does the potential describe exact SHM?
Show solutionHide solution
Question 8 - Solution A weak quartic term changes turning-point energy before it changes the center x U (a) Derivation and calculation E = U(A) = 1 2kA2 + 1 4λA4. 1 2mv2 max = E −U(0) ⇒vmax = √ kA2 m + λA4 2m . vmax A √ k/m = √ 1 + λA2 2k > 1. F = −dU dx = −kx −λx3. (b) Result and interpretation At amplitude A, the relative quartic contribution is U4 U2 = λA4/4 kA2/2 = λA2 2k . λA2 2k ≤.05 ⇒A ≤ √ .10k/λ . Finite excursions are not exact SHM because F/x = −(k + λx2) varies with position. Physical check As λA2/k →0, the usual vmax = A √ k/m is recovered.

Question 8

A weak quartic term changes turning-point energy before it changes the center

A conservative oscillator has U(x)=kx2/2+λx4/4U(x)=kx^2/2+\lambda x^4/4, with k,λ>0k,\lambda>0, and turns at x=±Ax=\pm A. Its mass is mm.

Diagram shown in the original SVG worksheet.

  1. Find total energy and speed at equilibrium. Compare the result with the harmonic prediction for the same amplitude.

  2. Find the condition on AA for the quartic contribution to turning-point energy to be at most 5%5\% of the quadratic contribution. Does the potential describe exact SHM?

Question 8 - Solution

A weak quartic term changes turning-point energy before it changes the center

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

E=U(A)=12kA2+14λA4.E=U(A)=\tfrac12kA^2+\tfrac14\lambda A^4.12mvmax⁡2=E−U(0)⇒vmax=kA2m+λA42m.\tfrac12mv_{\max}^2=E-U(0)\Rightarrow\boxed{v_{\max}=\sqrt{\frac{kA^2}{m}+\frac{\lambda A^4}{2m}}}.vmaxAk/m=1+λA22k>1.\frac{v_{\max}}{A\sqrt{k/m}}=\sqrt{1+\frac{\lambda A^2}{2k}}>1.F=−dUdx=−kx−λx3.F=-\frac{dU}{dx}=-kx-\lambda x^3.

(b) Result and interpretation

At amplitude AA, the relative quartic contribution isU4U2=λA4/4kA2/2=λA22k.\frac{U_4}{U_2}=\frac{\lambda A^4/4}{kA^2/2}=\frac{\lambda A^2}{2k}.λA22k≤.05⇒A≤.10k/λ.\frac{\lambda A^2}{2k}\le.05\Rightarrow\boxed{A\le\sqrt{.10k/\lambda}}.Finite excursions are not exact SHM because F/x=−(k+λx2)F/x=-(k+\lambda x^2) varies with position.

Physical check

As λA2/k→0\lambda A^2/k\to0, the usual vmax=Ak/mv_{\max}=A\sqrt{k/m} is recovered.