Collision and Impulse — Question 9

Section 9-5 · Physics pages 1248–1249

Question 9 Equal impulses delivered at different times A 1 kg cart starts at rest. In experiment A a 4 N force acts over 0 < t < 1 s; in B it acts over 1 < t < 2 s. Otherwise horizontal force is zero. t Fx A B 1 2 4 Equal-height, equal-duration pulses occur at different times; the dashed trace is offset slightly for visibility. (a) Compare final velocities at t = 2 s. (b) Compare displacements by t = 2 s and explain why the impulse theorem alone cannot determine them.
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Question 9 - Solution Equal impulses delivered at different times t Fx A B 1 2 4 (a) Derivation and calculation Both experiments apply the same total impulse by two seconds: JA = 4(1) = 4 N s, JB = 4(1) = 4 N s. vA(2) = vB(2) = 0 + J/m = 4 m/s . (b) Result and interpretation The earlier pulse gives an extra second of coasting: xA(2) = 1 2(4)(1)2 + 4(1) = 6 m , xB(2) = 0 + 1 2(4)(1)2 = 2 m . Generally, from rest, x(T) = m−1 ∫T 0 (T −t)F(t) dt; displacement retains the timing that total impulse discards. Physical check The final velocities agree while the earlier acceleration produces 4 m more travel.

Question 9

Equal impulses delivered at different times

A 1kg1\,\mathrm{kg} cart starts at rest. In experiment A a 4N4\,\mathrm N force acts over 0<t<1s0<t<1\,\mathrm s; in B it acts over 1<t<2s1<t<2\,\mathrm s. Otherwise horizontal force is zero.

Diagram shown in the original SVG worksheet.

  1. Compare final velocities at t=2st=2\,\mathrm s.

  2. Compare displacements by t=2st=2\,\mathrm s and explain why the impulse theorem alone cannot determine them.

Question 9 - Solution

Equal impulses delivered at different times

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Both experiments apply the same total impulse by two seconds: JA=4(1)=4Ns,JB=4(1)=4Ns.J_A=4(1)=4\ \mathrm{N\,s},\qquad J_B=4(1)=4\ \mathrm{N\,s}. vA(2)=vB(2)=0+J/m=4m/s.\boxed{v_A(2)=v_B(2)=0+J/m=4\ \mathrm{m/s}}.

(b) Result and interpretation

The earlier pulse gives an extra second of coasting: xA(2)=12(4)(1)2+4(1)=6m,xB(2)=0+12(4)(1)2=2m.\boxed{x_A(2)=\tfrac12(4)(1)^2+4(1)=6\ \mathrm m},\qquad \boxed{x_B(2)=0+\tfrac12(4)(1)^2=2\ \mathrm m}. Generally, from rest, x(T)=m−1∫0T(T−t)F(t)dtx(T)=m^{-1}\int_0^T(T-t)F(t)\,dt; displacement retains the timing that total impulse discards.

Physical check

The final velocities agree while the earlier acceleration produces 4 m more travel.