Inelastic Collisions in One Dimension — Question 3

Section 9-8 · Physics pages 1296–1297

Question 3 A ballistic pendulum requires two different balances A 0.020 kg pellet embeds in a stationary 0.980 kg bob suspended by a light cord. The combined bob rises by 0.20 m. The short collision occurs at the bottom, and air drag is negligible. Use g = 9.8 m/s2. u h Schematic: short horizontal impact, then a rising swing. (a) Find the pellet speed immediately before impact. (b) Find the kinetic energy lost during embedding and explain why one energy equation from launch to peak would fail.
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Question 3 - Solution A ballistic pendulum requires two different balances u h (a) Derivation and calculation Use mechanical energy conservation during the swing, then momentum conservation during capture: 1 2(m + M)V 2 = (m + M)gh ⇒V = √ 2gh = √ 3.92 = 1.980 m/s. mu = (m + M)V ⇒u = 1.000 0.020 √ 3.92 = 99.0 m/s . (b) Result and interpretation Immediately before and after capture, Ki = 1 2(0.020)u2 = 98.0 J, K+ = 1 2(1.000)(3.92) = 1.96 J. Klost,impact = 96.04 J . Impact is inelastic; the subsequent ideal swing converts the retained kinetic energy into gravitational potential energy. Physical check The impact retains only the fraction m/(m + M) = 0.020 of the initial kinetic energy.

Question 3

A ballistic pendulum requires two different balances

A 0.020kg0.020\,\mathrm{kg} pellet embeds in a stationary 0.980kg0.980\,\mathrm{kg} bob suspended by a light cord. The combined bob rises by 0.20m0.20\,\mathrm m. The short collision occurs at the bottom, and air drag is negligible. Use g=9.8m/s2g=9.8\,\mathrm{m/s^2}.

Diagram shown in the original SVG worksheet.

  1. Find the pellet speed immediately before impact.

  2. Find the kinetic energy lost during embedding and explain why one energy equation from launch to peak would fail.

Question 3 - Solution

A ballistic pendulum requires two different balances

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Use mechanical energy conservation during the swing, then momentum conservation during capture: 12(m+M)V2=(m+M)gh⇒V=2gh=3.92=1.980m/s.\tfrac12(m+M)V^2=(m+M)gh\Rightarrow V=\sqrt{2gh}=\sqrt{3.92}=1.980\ \mathrm{m/s}. mu=(m+M)V⇒u=1.0000.0203.92=99.0m/s.mu=(m+M)V\Rightarrow\boxed{u=\frac{1.000}{0.020}\sqrt{3.92}=99.0\ \mathrm{m/s}}.

(b) Result and interpretation

Immediately before and after capture, Ki=12(0.020)u2=98.0J,K+=12(1.000)(3.92)=1.96J.K_i=\tfrac12(0.020)u^2=98.0\ \mathrm J,\qquad K_+=\tfrac12(1.000)(3.92)=1.96\ \mathrm J. Klost,impact=96.04J.\boxed{K_{\mathrm{lost,impact}}=96.04\ \mathrm J}. Impact is inelastic; the subsequent ideal swing converts the retained kinetic energy into gravitational potential energy.

Physical check

The impact retains only the fraction m/(m+M)=0.020m/(m+M)=0.020 of the initial kinetic energy.