Simple Harmonic Motion — Question 10

Section 15-1 · Physics pages 2250–2251

Question 10 Average speed and root-mean-square speed answer different questions An SHM oscillator has amplitude A and period T. Define the rms speed as vrms = √ T −1 ∫T 0 v2dt. ψ x/A 2π 1 −1 Normalized displacement over one cycle; the horizontal coordinate is phase. (a) Find the mean velocity and mean speed over a complete cycle. (b) Find the rms speed and compare it with mean speed and maximum speed. Explain the strict ordering for nonzero amplitude.
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Question 10 - Solution Average speed and root-mean-square speed answer different questions ψ x/A 2π 1 −1 (a) Derivation and calculation For one closed cycle, the signed displacement vanishes but the distance traveled is 4A: v = x(T) −x(0) T = 0 , |v| = 4A T = 2Aω π . (b) Result and interpretation v2 rms = A2ω2 T ∫T 0 sin2(ωt + ϕ) dt = A2ω2 2 . vrms = Aω √ 2 , vmax = Aω. 2 π = 0.63662 < 1 √ 2 = 0.70711 < 1 ⇒ |v| < vrms < vmax. RMS averaging weights larger speeds more strongly; equality would require constant speed. Physical check The inequalities are strict for A > 0 and ω > 0. Mean velocity remains zero despite nonzero mean speed.

Question 10

Average speed and root-mean-square speed answer different questions

An SHM oscillator has amplitude AA and period TT. Define the rms speed as vrms=T−1∫0Tv2dtv_{\mathrm{rms}}=\sqrt{T^{-1}\int_0^T v^2dt}.

Diagram shown in the original SVG worksheet.

  1. Find the mean velocity and mean speed over a complete cycle.

  2. Find the rms speed and compare it with mean speed and maximum speed. Explain the strict ordering for nonzero amplitude.

Question 10 - Solution

Average speed and root-mean-square speed answer different questions

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For one closed cycle, the signed displacement vanishes but the distance traveled is 4A4A:v¯=x(T)−x(0)T=0,|v|¯=4AT=2Aωπ.\overline v=\frac{x(T)-x(0)}T=\boxed0,\qquad\overline{|v|}=\frac{4A}{T}=\boxed{\frac{2A\omega}{\pi}}.

(b) Result and interpretation

vrms2=A2ω2T∫0Tsin⁡2(ωt+ϕ)dt=A2ω22.v_{\mathrm{rms}}^2=\frac{A^2\omega^2}{T}\int_0^T\sin^2(\omega t+\phi)\,dt=\frac{A^2\omega^2}{2}.vrms=Aω2,vmax=Aω.\boxed{v_{\mathrm{rms}}=\frac{A\omega}{\sqrt2}},\qquad v_{\max}=A\omega.2π=0.63662<12=0.70711<1⇒|v|¯<vrms<vmax.\frac{2}{\pi}=0.63662<\frac1{\sqrt2}=0.70711<1\quad\Rightarrow\quad\overline{|v|}<v_{\mathrm{rms}}<v_{\max}.RMS averaging weights larger speeds more strongly; equality would require constant speed.

Physical check

The inequalities are strict for A>0A>0 and ω>0\omega>0. Mean velocity remains zero despite nonzero mean speed.