The Force Law for Simple Harmonic Motion — Question 9

Section 15-2 · Physics pages 2268–2269

Question 9 A free spring pair oscillates with the reduced mass Two masses m1 and m2 slide on a frictionless line and are joined by a massless spring of constant k and natural length ℓ0. There is no external horizontal force. Let q = x2 −x1 −ℓ0 be the extension. m1 m2 Two free masses linked by a spring; forces are opposite when the spring is stretched. (a) Derive the equation for q and its angular frequency. (b) For m1 = m and m2 = 3m, find the ratio of their oscillation amplitudes about the center of mass. What separate motion can the center of mass have?
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Question 9 - Solution A free spring pair oscillates with the reduced mass m1 m2 (a) Derivation and calculation m1¨x1 = kq, m2¨x2 = −kq, q = x2 −x1 −ℓ0. ¨q = ¨x2 −¨x1 = −k ( 1 m1 + 1 m2 ) q. µ = m1m2 m1 + m2 , ω = √ k/µ . (b) Result and interpretation With X = (m1x1 + m2x2)/(m1 + m2), (m1 + m2) ¨X = 0 ⇒X = X0 + V0t. δx1 = − m2 m1 + m2 q, δx2 = m1 m1 + m2 q. m1 = m, m2 = 3m : A1/A2 = 3 , µ = 3m/4. Relative oscillation and uniform center-of-mass translation are independent. Physical check As one mass tends to infinity, µ tends to the finite mass and the fixed-support frequency is recovered.

Question 9

A free spring pair oscillates with the reduced mass

Two masses m1m_1 and m2m_2 slide on a frictionless line and are joined by a massless spring of constant kk and natural length ℓ0\ell_0. There is no external horizontal force. Let q=x2−x1−ℓ0q=x_2-x_1-\ell_0 be the extension.

Diagram shown in the original SVG worksheet.

  1. Derive the equation for qq and its angular frequency.

  2. For m1=mm_1=m and m2=3mm_2=3m, find the ratio of their oscillation amplitudes about the center of mass. What separate motion can the center of mass have?

Question 9 - Solution

A free spring pair oscillates with the reduced mass

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

m1ẍ1=kq,m2ẍ2=−kq,q=x2−x1−ℓ0.m_1\ddot x_1=kq,\qquad m_2\ddot x_2=-kq,\qquad q=x_2-x_1-\ell_0.q̈=ẍ2−ẍ1=−k(1m1+1m2)q.\ddot q=\ddot x_2-\ddot x_1=-k\left(\frac1{m_1}+\frac1{m_2}\right)q.μ=m1m2m1+m2,ω=k/μ.\boxed{\mu=\frac{m_1m_2}{m_1+m_2}},\qquad\boxed{\omega=\sqrt{k/\mu}}.

(b) Result and interpretation

With X=(m1x1+m2x2)/(m1+m2)X=(m_1x_1+m_2x_2)/(m_1+m_2),(m1+m2)Ẍ=0⇒X=X0+V0t.(m_1+m_2)\ddot X=0\Rightarrow X=X_0+V_0t.δx1=−m2m1+m2q,δx2=m1m1+m2q.\delta x_1=-\frac{m_2}{m_1+m_2}q,\qquad\delta x_2=\frac{m_1}{m_1+m_2}q.m1=m,m2=3m:A1/A2=3,μ=3m/4.m_1=m,\ m_2=3m:\quad\boxed{A_1/A_2=3},\quad\mu=3m/4.Relative oscillation and uniform center-of-mass translation are independent.

Physical check

As one mass tends to infinity, μ\mu tends to the finite mass and the fixed-support frequency is recovered.