Forced Oscillations and Resonance — Question 4

Section 15-8 · Physics pages 2378–2379

Question 4 The exact half-power bandwidth has a geometric center For fixed-amplitude force driving, P/P max = b2/[(k/Ω−mΩ)2 + b2]. Let Ω−and Ω+ be the positive frequencies at half the maximum power. Ω P Pmax/2 Ω− Ω+ The two half-power crossings define a bandwidth; their geometric mean is the natural frequency. (a) Derive both half-power frequencies, their difference and their product. (b) For m = 1 kg, k = 25 N/m and b = 2 kg/s, find the frequencies. Is the natural frequency exactly their arithmetic midpoint?
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Question 4 - Solution The exact half-power bandwidth has a geometric center Ω P Pmax/2 Ω− Ω+ (a) Derivation and calculation P/P max = 1 2 ⇐⇒(k/Ω−mΩ)2 = b2. mΩ2 −+ bΩ−−k = 0, mΩ2 + −bΩ+ −k = 0. Ω± = √ b2 + 4mk ± b 2m . (b) Result and interpretation Ω+ −Ω−= b/m , Ω+Ω−= k/m = ω2 0 . m = 1, k = 25, b = 2 : Ω−= √ 26 −1 = 4.09902, Ω+ = √ 26 + 1 = 6.09902. √ Ω−Ω+ = 5.00, (Ω−+ Ω+)/2 = √ 26 = 5.09902 rad/s. The natural frequency is exactly the geometric mean, not the arithmetic midpoint. Physical check The half-power width is exact; symmetry about ω0 is only a narrow-band approximation.

Question 4

The exact half-power bandwidth has a geometric center

For fixed-amplitude force driving, P¯/P¯max=b2/[(k/Ω−mΩ)2+b2]\overline P/\overline P_{\max}=b^2/[(k/\Omega-m\Omega)^2+b^2]. Let Ω−\Omega_- and Ω+\Omega_+ be the positive frequencies at half the maximum power.

Diagram shown in the original SVG worksheet.

  1. Derive both half-power frequencies, their difference and their product.

  2. For m=1kgm=1\,\mathrm{kg}, k=25N/mk=25\,\mathrm{N/m} and b=2kg/sb=2\,\mathrm{kg/s}, find the frequencies. Is the natural frequency exactly their arithmetic midpoint?

Question 4 - Solution

The exact half-power bandwidth has a geometric center

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

P¯/P¯max=12⇔(k/Ω−mΩ)2=b2.\overline P/\overline P_{\max}=\tfrac12\iff(k/\Omega-m\Omega)^2=b^2.mΩ−2+bΩ−−k=0,mΩ+2−bΩ+−k=0.m\Omega_-^2+b\Omega_--k=0,\quad m\Omega_+^2-b\Omega_+-k=0.Ω±=b2+4mk±b2m.\boxed{\Omega_{\pm}=\frac{\sqrt{b^2+4mk}\pm b}{2m}}.

(b) Result and interpretation

Ω+−Ω−=b/m,Ω+Ω−=k/m=ω02.\boxed{\Omega_+-\Omega_-=b/m},\qquad\boxed{\Omega_+\Omega_-=k/m=\omega_0^2}.m=1,k=25,b=2:Ω−=26−1=4.09902,Ω+=26+1=6.09902.m=1,\ k=25,\ b=2:\quad\Omega_-=\sqrt{26}-1=4.09902,\quad\Omega_+=\sqrt{26}+1=6.09902.Ω−Ω+=5.00,(Ω−+Ω+)/2=26=5.09902rad/s.\sqrt{\Omega_-\Omega_+}=5.00,\qquad(\Omega_-+\Omega_+)/2=\sqrt{26}=5.09902\,\mathrm{rad/s}.The natural frequency is exactly the geometric mean, not the arithmetic midpoint.

Physical check

The half-power width is exact; symmetry about ω0\omega_0 is only a narrow-band approximation.