Energy in Simple Harmonic Motion — Question 3

Section 15-3 · Physics pages 2276–2277

Question 3 The same impulse can add or remove oscillator energy A horizontal oscillator has mass m, instantaneous velocity v and position x. A very short impulse J acts in the positive direction, leaving position unchanged. Spring force contributes negligible impulse during the event. m x J Instantaneous force directions and displacement are shown schematically. (a) Derive the energy change caused by the impulse and the new amplitude. (b) For m = .50 kg, k = 50 N/m, initial amplitude .10 m and J = .20 N s, compare applying the impulse at equilibrium while moving right versus while moving left.
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Question 3 - Solution The same impulse can add or remove oscillator energy m x J (a) Derivation and calculation An impulse leaves position continuous and changes momentum: x+ = x, m(v+ −v) = J ⇒v+ = v + J/m. ∆E = 1 2m(v + J/m)2 −1 2mv2 = Jv + J2 2m . A+ = √ x2 + m k (v + J/m)2 . (b) Result and interpretation ω = √ 50/.50 = 10 rad/s, v = ±ωA = ±1.00 m/s, J/m = .400 m/s. v = +1 : v+ = 1.40, A+ = .140 m , ∆E = .240 J. v = −1 : v+ = −.600, A+ = .0600 m , ∆E = −.160 J. Physical check The same positive impulse can add or remove energy; the term Jv retains the initial direction.

Question 3

The same impulse can add or remove oscillator energy

A horizontal oscillator has mass mm, instantaneous velocity vv and position xx. A very short impulse JJ acts in the positive direction, leaving position unchanged. Spring force contributes negligible impulse during the event.

Diagram shown in the original SVG worksheet.

  1. Derive the energy change caused by the impulse and the new amplitude.

  2. For m=.50kgm=.50\,\mathrm{kg}, k=50N/mk=50\,\mathrm{N/m}, initial amplitude .10m.10\,\mathrm{m} and J=.20NsJ=.20\,\mathrm{N\,s}, compare applying the impulse at equilibrium while moving right versus while moving left.

Question 3 - Solution

The same impulse can add or remove oscillator energy

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

An impulse leaves position continuous and changes momentum:x+=x,m(v+−v)=J⇒v+=v+J/m.x_+=x,\qquad m(v_+-v)=J\Rightarrow v_+=v+J/m.ΔE=12m(v+J/m)2−12mv2=Jv+J22m.\boxed{\Delta E=\tfrac12m(v+J/m)^2-\tfrac12mv^2=Jv+\frac{J^2}{2m}}.A+=x2+mk(v+J/m)2.\boxed{A_+=\sqrt{x^2+\frac m k(v+J/m)^2}}.

(b) Result and interpretation

ω=50/.50=10rad/s,v=±ωA=±1.00m/s,J/m=.400m/s.\omega=\sqrt{50/.50}=10\,\mathrm{rad/s},\quad v=\pm\omega A=\pm1.00\,\mathrm{m/s},\quad J/m=.400\,\mathrm{m/s}.v=+1:v+=1.40,A+=.140m,ΔE=.240J.v=+1:\ v_+=1.40,\quad\boxed{A_+=.140\,\mathrm m},\quad\Delta E=.240\,\mathrm J.v=−1:v+=−.600,A+=.0600m,ΔE=−.160J.v=-1:\ v_+=-.600,\quad\boxed{A_+=.0600\,\mathrm m},\quad\Delta E=-.160\,\mathrm J.

Physical check

The same positive impulse can add or remove energy; the term JvJv retains the initial direction.