The Force Law for Simple Harmonic Motion — Question 5

Section 15-2 · Physics pages 2260–2261

Question 5 Added masses can separate unknown stiffness from hidden inertia A spring oscillator has unknown spring constant k and unknown moving fixture mass M. With an added mass m1 = 0.20 kg its squared period is T 2 1 = 0.30 s2. With m2 = 0.50 kg it is T 2 2 = 0.60 s2. The spring mass is negligible. m T 2 (.20, .30) (.50, .60) Measured points; horizontal units are kg and vertical units are s2. (a) Infer k and M from the two measurements. (b) Predict the squared period with no added mass. Why would plotting T rather than T 2 against added mass conceal the simple linear relation?
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Question 5 - Solution Added masses can separate unknown stiffness from hidden inertia m T 2 (.20, .30) (.50, .60) (a) Derivation and calculation T 2 = 4π2 k (M + m) = s m + b. s = 0.60 −0.30 0.50 −0.20 = 1.00 s2/kg, k = 4π2 s = 39.4784 N/m . M = T 2 1 s −m1 = 0.30 −0.20 = 0.100 kg . (b) Result and interpretation T 2 0 = sM = 0.100 s2 , T0 = 0.31623 s. T(m) = √ s(M + m), dT dm = s 2T , d2T dm2 = −s2 4T 3 < 0. The T graph is curved; the T 2 graph separates stiffness (slope) from fixture mass (intercept). Physical check Back-substitution gives T 2 = 0.30 and 0.60 s2 for the two stated added masses.

Question 5

Added masses can separate unknown stiffness from hidden inertia

A spring oscillator has unknown spring constant kk and unknown moving fixture mass MM. With an added mass m1=0.20kgm_1=0.20\,\mathrm{kg} its squared period is T12=0.30s2T_1^2=0.30\,\mathrm{s^2}. With m2=0.50kgm_2=0.50\,\mathrm{kg} it is T22=0.60s2T_2^2=0.60\,\mathrm{s^2}. The spring mass is negligible.

Diagram shown in the original SVG worksheet.

  1. Infer kk and MM from the two measurements.

  2. Predict the squared period with no added mass. Why would plotting TT rather than T2T^2 against added mass conceal the simple linear relation?

Question 5 - Solution

Added masses can separate unknown stiffness from hidden inertia

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

T2=4π2k(M+m)=sm+b.T^2=\frac{4\pi^2}{k}(M+m)=s\,m+b.s=0.60−0.300.50−0.20=1.00s2/kg,k=4π2s=39.4784N/m.s=\frac{0.60-0.30}{0.50-0.20}=1.00\,\mathrm{s^2/kg},\quad\boxed{k=\frac{4\pi^2}{s}=39.4784\,\mathrm{N/m}}.M=T12s−m1=0.30−0.20=0.100kg.M=\frac{T_1^2}{s}-m_1=0.30-0.20=\boxed{0.100\,\mathrm{kg}}.

(b) Result and interpretation

T02=sM=0.100s2,T0=0.31623s.\boxed{T_0^2=sM=0.100\,\mathrm{s^2}},\qquad T_0=0.31623\,\mathrm s.T(m)=s(M+m),dTdm=s2T,d2Tdm2=−s24T3<0.T(m)=\sqrt{s(M+m)},\quad\frac{dT}{dm}=\frac{s}{2T},\quad\frac{d^2T}{dm^2}=-\frac{s^2}{4T^3}<0.The TT graph is curved; the T2T^2 graph separates stiffness (slope) from fixture mass (intercept).

Physical check

Back-substitution gives T2=0.30T^2=0.30 and 0.60s20.60\,\mathrm{s^2} for the two stated added masses.