Elastic Collisions in One Dimension — Question 2

Section 9-9 · Physics pages 1314–1315

Question 2 Measuring a target mass from rebound A cart of known mass m strikes a stationary target elastically and rebounds with speed u/3, where u was its incident speed. Motion is one dimensional. m M u/3 v2 The incident mass rebounds from an initially stationary target. (a) Infer the target mass M and its final speed. (b) What fraction of initial kinetic energy reaches the target?
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Question 2 - Solution Measuring a target mass from rebound m M u/3 v2 (a) Derivation and calculation For a stationary target in an elastic collision, v1 u = m −M m + M = −1 3. 3m −3M = −m −M ⇒M = 2m . v2 = 2m m + M u = 2 3u . (b) Result and interpretation The target energy fraction is η = 1 2(2m)(2u/3)2 1 2mu2 = 8 9 . The incident object retains K1f/Ki = (v1/u)2 = 1/9, so the fractions sum to unity. Physical check The final momentum is −mu/3 + 4mu/3 = mu.

Question 2

Measuring a target mass from rebound

A cart of known mass mm strikes a stationary target elastically and rebounds with speed u/3u/3, where uu was its incident speed. Motion is one dimensional.

Diagram shown in the original SVG worksheet.

  1. Infer the target mass MM and its final speed.

  2. What fraction of initial kinetic energy reaches the target?

Question 2 - Solution

Measuring a target mass from rebound

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For a stationary target in an elastic collision, v1u=m−Mm+M=−13.\frac{v_1}{u}=\frac{m-M}{m+M}=-\frac13. 3m−3M=−m−M⇒M=2m.3m-3M=-m-M\Rightarrow\boxed{M=2m}. v2=2mm+Mu=23u.\boxed{v_2=\frac{2m}{m+M}u=\frac23u}.

(b) Result and interpretation

The target energy fraction is η=12(2m)(2u/3)212mu2=89.\boxed{\eta=\frac{\tfrac12(2m)(2u/3)^2}{\tfrac12mu^2}=\frac89}. The incident object retains K1f/Ki=(v1/u)2=1/9K_{1f}/K_i=(v_1/u)^2=1/9, so the fractions sum to unity.

Physical check

The final momentum is −mu/3+4mu/3=mu-mu/3+4mu/3=mu.