Energy in Simple Harmonic Motion — Question 5

Section 15-3 · Physics pages 2280–2281

Question 5 Catching extra mass changes inertia and can dissipate energy A horizontal spring oscillator has moving mass m, stiffness k and amplitude A. An equal mass drops vertically onto it and sticks, bringing zero horizontal momentum. The event is instantaneous; ignore any horizontal impulse from the spring and any change of equilibrium. m x m An equal mass drops onto and sticks to the oscillator; horizontal momentum is conserved during capture. (a) Find the new amplitude and energy if capture occurs at equilibrium. (b) Compare with capture at a turning point. Why does the same added mass not produce the same energy loss in both cases?
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Question 5 - Solution Catching extra mass changes inertia and can dissipate energy m x m (a) Derivation and calculation For capture by an initially stationary equal mass, mv = (2m)v+ ⇒v+ = v/2, ω+ = √ k/(2m) = ω/ √ 2. ∆K = 1 2(2m)(v/2)2 −1 2mv2 = −1 4mv2. (b) Result and interpretation At equilibrium, v = ωA and U = 0: E+ = E/2, A+ = √ 2E+/k = A/ √ 2 . At a turning point, v = 0: E+ = E, v+ = 0, A+ = A . The post-capture frequency is ω/ √ 2 in both cases. Physical check The horizontal kinetic energy lost in the inelastic capture is zero at a turning point and largest at equilibrium.

Question 5

Catching extra mass changes inertia and can dissipate energy

A horizontal spring oscillator has moving mass mm, stiffness kk and amplitude AA. An equal mass drops vertically onto it and sticks, bringing zero horizontal momentum. The event is instantaneous; ignore any horizontal impulse from the spring and any change of equilibrium.

Diagram shown in the original SVG worksheet.

  1. Find the new amplitude and energy if capture occurs at equilibrium.

  2. Compare with capture at a turning point. Why does the same added mass not produce the same energy loss in both cases?

Question 5 - Solution

Catching extra mass changes inertia and can dissipate energy

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For capture by an initially stationary equal mass,mv=(2m)v+⇒v+=v/2,ω+=k/(2m)=ω/2.mv=(2m)v_+\Rightarrow v_+=v/2,\qquad\omega_+=\sqrt{k/(2m)}=\omega/\sqrt2.ΔK=12(2m)(v/2)2−12mv2=−14mv2.\Delta K=\tfrac12(2m)(v/2)^2-\tfrac12mv^2=-\tfrac14mv^2.

(b) Result and interpretation

At equilibrium, v=ωAv=\omega A and U=0U=0:E+=E/2,A+=2E+/k=A/2.E_+=E/2,\qquad\boxed{A_+=\sqrt{2E_+/k}=A/\sqrt2}.At a turning point, v=0v=0:E+=E,v+=0,A+=A.E_+=E,\quad v_+=0,\qquad\boxed{A_+=A}.The post-capture frequency is ω/2\omega/\sqrt2 in both cases.

Physical check

The horizontal kinetic energy lost in the inelastic capture is zero at a turning point and largest at equilibrium.