Translational Kinetic Energy — Question 7

Section 19-4 · Physics pages 3104–3105

Question 7 A single elastic collision need not share energy equally In a one-dimensional elastic collision, a molecule of mass m and initial speed u strikes a stationary molecule of mass 3m. Use conservation of momentum and kinetic energy; take the incoming direction positive. m u 3m initially at rest Schematic; labels, not drawing lengths, specify the data. (a) Find both final velocities and the fraction of initial kinetic energy transferred to the target. (b) For general target mass M, derive the transferred fraction 4mM/(m + M)2 and determine which mass ratio maximizes it.
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Question 7 - Solution A single elastic collision need not share energy equally m u 3m initially at rest (a) Method and calculation mu = mv + 3mV, 1 2mu2 = 1 2mv2 + 1 2(3m)V 2. v = −u/2, V = u/2, Ktarget Ki = 3m(u/2)2 mu2 = 3 4. (b) Interpretation and further calculation V = 2m m + M u ⇒Ktarget Ki = 4mM (m + M)2 . 4mM (m + M)2 = 1 −(M −m)2 (M + m)2 ≤1. Equality occurs at M = m. A single event transfers an amount fixed by its initial geometry and velocities; equilibrium equipartition is an ensemble statement. Physical check The lighter projectile rebounds here, while the heavier target takes 75% of the initial energy.

Question 7

A single elastic collision need not share energy equally

In a one-dimensional elastic collision, a molecule of mass mm and initial speed uu strikes a stationary molecule of mass 3m3m. Use conservation of momentum and kinetic energy; take the incoming direction positive.

Diagram shown in the original SVG worksheet.

  1. Find both final velocities and the fraction of initial kinetic energy transferred to the target.

  2. For general target mass MM, derive the transferred fraction 4mM/(m+M)24mM/(m+M)^2 and determine which mass ratio maximizes it.

Question 7 - Solution

A single elastic collision need not share energy equally

Diagram shown in the original SVG worksheet.

(a) Method and calculation

mu=mv+3mV,12mu2=12mv2+12(3m)V2.mu=mv+3mV,\quad\tfrac12mu^2=\tfrac12mv^2+\tfrac12(3m)V^2.v=−u/2,V=u/2,KtargetKi=3m(u/2)2mu2=34.v=-u/2,\quad V=u/2,\quad\frac{K_{\mathrm{target}}}{K_i}=\frac{3m(u/2)^2}{mu^2}=\frac34.

(b) Interpretation and further calculation

V=2mm+Mu⇒KtargetKi=4mM(m+M)2.V=\frac{2m}{m+M}u\ \Rightarrow\ \frac{K_{\mathrm{target}}}{K_i}=\frac{4mM}{(m+M)^2}.4mM(m+M)2=1−(M−m)2(M+m)2≤1.\frac{4mM}{(m+M)^2}=1-\frac{(M-m)^2}{(M+m)^2}\le1.Equality occurs at M=mM=m. A single event transfers an amount fixed by its initial geometry and velocities; equilibrium equipartition is an ensemble statement.

Physical check

The lighter projectile rebounds here, while the heavier target takes 75% of the initial energy.