Elastic Collisions in One Dimension — Question 3

Section 9-9 · Physics pages 1316–1317

Question 3 Why matching masses maximizes single-collision transfer A mass m at speed u collides elastically with a stationary mass M. Define r = M/m > 0. r η 1 1 Energy-transfer fraction versus positive mass ratio. (a) Derive the fraction of incident kinetic energy transferred to the target. (b) Find its maximum and compare r with 1/r.
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Question 3 - Solution Why matching masses maximizes single-collision transfer r η 1 1 (a) Derivation and calculation With r = M/m and v2 = 2u/(1 + r), η = Mv2 2 mu2 = 4r (1 + r)2 . (1 + r)2 −4r = (r −1)2 ≥0 ⇒η ≤1. Equality occurs only at r = 1 . (b) Result and interpretation Under a reciprocal mass ratio, η(1/r) = 4/r (1 + 1/r)2 = 4r (1 + r)2 = η(r). Thus equally mismatched reciprocal ratios transfer the same energy fraction, while equal masses transfer all the incident energy. Physical check The transfer tends to zero as either r →0 or r →∞.

Question 3

Why matching masses maximizes single-collision transfer

A mass mm at speed uu collides elastically with a stationary mass MM. Define r=M/m>0r=M/m>0.

Diagram shown in the original SVG worksheet.

  1. Derive the fraction of incident kinetic energy transferred to the target.

  2. Find its maximum and compare rr with 1/r1/r.

Question 3 - Solution

Why matching masses maximizes single-collision transfer

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

With r=M/mr=M/m and v2=2u/(1+r)v_2=2u/(1+r), η=Mv22mu2=4r(1+r)2.\boxed{\eta=\frac{Mv_2^2}{mu^2}=\frac{4r}{(1+r)^2}}. (1+r)2−4r=(r−1)2≥0⇒η≤1.(1+r)^2-4r=(r-1)^2\geq0\Rightarrow\eta\leq1. Equality occurs only at r=1\boxed{r=1}.

(b) Result and interpretation

Under a reciprocal mass ratio, η(1/r)=4/r(1+1/r)2=4r(1+r)2=η(r).\eta(1/r)=\frac{4/r}{(1+1/r)^2}=\frac{4r}{(1+r)^2}=\eta(r). Thus equally mismatched reciprocal ratios transfer the same energy fraction, while equal masses transfer all the incident energy.

Physical check

The transfer tends to zero as either r→0r\to0 or r→∞r\to\infty.