Forced Oscillations and Resonance — Question 9

Section 15-8 · Physics pages 2388–2389

Question 9 Energy supplied per cycle is determined by the force-displacement loop In steady driven motion, x = X cos(Ωt −δ) and the applied force is F = F0 cos Ωt. Let Ω> 0 and 0 < δ < π. x F The oriented force-displacement loop encloses the positive input work per steady cycle. (a) Evaluate the work supplied in one cycle and relate it to the oriented force-displacement loop. (b) For F0 = 3.0 N, X = .020 m, δ = π/6 and Ω= 10 rad/s, find the work per cycle, mean power and compatible viscous coefficient b.
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Question 9 - Solution Energy supplied per cycle is determined by the force-displacement loop x F (a) Derivation and calculation Put ψ = Ωt −δ; then F = F0 cos(ψ + δ) and dx = −X sin ψ dψ. W = −F0X Z 2π 0 (cos ψ cos δ −sin ψ sin δ) sin ψ dψ. W = I F dx = πF0X sin δ = πbΩX2 . (b) Result and interpretation W = π(3.00)(.0200) sin(π/6) = .094248 J . P = WΩ 2π = .150 W . b = F0 sin δ ΩX = 3.00(.500) 10(.0200) = 7.50 kg/s . The loop integral is positive and replaces the energy dissipated during a cycle. Physical check Stored mechanical energy returns to its original value each steady cycle, so net input equals damping loss.

Question 9

Energy supplied per cycle is determined by the force-displacement loop

In steady driven motion, x=Xcos⁡(Ωt−δ)x=X\cos(\Omega t-\delta) and the applied force is F=F0cos⁡ΩtF=F_0\cos\Omega t. Let Ω>0\Omega>0 and 0<δ<π0<\delta<\pi.

Diagram shown in the original SVG worksheet.

  1. Evaluate the work supplied in one cycle and relate it to the oriented force-displacement loop.

  2. For F0=3.0NF_0=3.0\,\mathrm{N}, X=.020mX=.020\,\mathrm{m}, δ=π/6\delta=\pi/6 and Ω=10rad/s\Omega=10\,\mathrm{rad/s}, find the work per cycle, mean power and compatible viscous coefficient bb.

Question 9 - Solution

Energy supplied per cycle is determined by the force-displacement loop

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Put ψ=Ωt−δ\psi=\Omega t-\delta; then F=F0cos⁡(ψ+δ)F=F_0\cos(\psi+\delta) and dx=−Xsin⁡ψdψdx=-X\sin\psi\,d\psi.W=−F0X∫02π(cos⁡ψcos⁡δ−sin⁡ψsin⁡δ)sin⁡ψdψ.W=-F_0X\int_0^{2\pi}(\cos\psi\cos\delta-\sin\psi\sin\delta)\sin\psi\,d\psi.W=∮Fdx=πF0Xsin⁡δ=πbΩX2.\boxed{W=\oint F\,dx=\pi F_0X\sin\delta=\pi b\Omega X^2}.

(b) Result and interpretation

W=π(3.00)(.0200)sin⁡(π/6)=.094248J.\boxed{W=\pi(3.00)(.0200)\sin(\pi/6)=.094248\,\mathrm J}.P¯=WΩ2π=.150W.\boxed{\overline P=\frac{W\Omega}{2\pi}=.150\,\mathrm W}.b=F0sin⁡δΩX=3.00(.500)10(.0200)=7.50kg/s.\boxed{b=\frac{F_0\sin\delta}{\Omega X}=\frac{3.00(.500)}{10(.0200)}=7.50\,\mathrm{kg/s}}.The loop integral is positive and replaces the energy dissipated during a cycle.

Physical check

Stored mechanical energy returns to its original value each steady cycle, so net input equals damping loss.