Energy in Simple Harmonic Motion — Question 7

Section 15-3 · Physics pages 2284–2285

Question 7 Peak power occurs between equilibrium and the turning point For an ideal spring oscillator, the instantaneous power delivered by the spring is P = Fv = −kxv. Let x = A cos ωt and ω2 = k/m. ψ x/A 2π 1 −1 Normalized displacement over one cycle; the horizontal coordinate is phase. (a) Find the maximum magnitude of spring power and the positions where it occurs. (b) Find the net spring work over a full cycle and the work from x = A to x = 0. Explain how zero net work can coexist with large instantaneous power.
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Question 7 - Solution Peak power occurs between equilibrium and the turning point ψ x/A 2π 1 −1 (a) Derivation and calculation x = A cos ψ, v = −Aω sin ψ, F = −kA cos ψ. P = Fv = kA2ω sin ψ cos ψ = Eω sin 2ψ . |P|max = Eω , | sin 2ψ| = 1 ⇒|x| = A/ √ 2. (b) Result and interpretation Wcycle = I (−kx) dx = 0. WA→0 = Z 0 A (−kx) dx = 1 2kA2 = E . P = dK dt = −dU dt . Power is positive while moving toward equilibrium and negative while moving away. Physical check Power vanishes at both equilibrium (F = 0) and a turning point (v = 0).

Question 7

Peak power occurs between equilibrium and the turning point

For an ideal spring oscillator, the instantaneous power delivered by the spring is P=Fv=−kxvP=Fv=-kxv. Let x=Acos⁡ωtx=A\cos\omega t and ω2=k/m\omega^2=k/m.

Diagram shown in the original SVG worksheet.

  1. Find the maximum magnitude of spring power and the positions where it occurs.

  2. Find the net spring work over a full cycle and the work from x=Ax=A to x=0x=0. Explain how zero net work can coexist with large instantaneous power.

Question 7 - Solution

Peak power occurs between equilibrium and the turning point

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

x=Acos⁡ψ,v=−Aωsin⁡ψ,F=−kAcos⁡ψ.x=A\cos\psi,\quad v=-A\omega\sin\psi,\quad F=-kA\cos\psi.P=Fv=kA2ωsin⁡ψcos⁡ψ=Eωsin⁡2ψ.\boxed{P=Fv=kA^2\omega\sin\psi\cos\psi=E\omega\sin2\psi}.|P|max=Eω,|sin⁡2ψ|=1⇒|x|=A/2.\boxed{|P|_{\max}=E\omega},\qquad|\sin2\psi|=1\Rightarrow |x|=A/\sqrt2.

(b) Result and interpretation

Wcycle=∮(−kx)dx=0.W_{\mathrm{cycle}}=\oint(-kx)\,dx=0.WA→0=∫A0(−kx)dx=12kA2=E.W_{A\to0}=\int_A^0(-kx)\,dx=\tfrac12kA^2=\boxed E.P=dKdt=−dUdt.P=\frac{dK}{dt}=-\frac{dU}{dt}.Power is positive while moving toward equilibrium and negative while moving away.

Physical check

Power vanishes at both equilibrium (F=0F=0) and a turning point (v=0v=0).