Collisions in Two Dimensions — Question 4

Section 9-10 · Physics pages 1338–1339

Question 4 Perpendicular departures do not prove elasticity for unequal masses A 2 kg projectile moving at 6 m/s along +x hits a stationary 1 kg target. The projectile leaves at 30◦and the target at −60◦. External impulse is negligible.⃗ u1⃗ v1⃗ v2 The departure angle difference is 90 degrees, but the masses differ. (a) Use the two momentum components to find both final speeds. (b) Test whether the claimed event can be elastic or passive inelastic.
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Question 4 - Solution Perpendicular departures do not prove elasticity for unequal masses⃗ u1⃗ v1⃗ v2 (a) Derivation and calculation The two momentum equations are 12 = 2v1 cos 30◦+ v2 cos 60◦, 0 = 2v1 sin 30◦−v2 sin 60◦. The second gives v2 = 2v1/ √ 3. Substitution into the first gives 12 = 4 √ 3v1 ⇒v1 = 3 √ 3, v2 = 6 m/s . (b) Result and interpretation Test the energy rather than assuming the right-angle rule: Ki = 1 2(2)(6)2 = 36 J, Kf = 1 2(2)(27) + 1 2(1)(36) = 45 J. ∆K = +9 J . The event requires internal energy release. It is neither elastic nor passive inelastic; the usual perpendicular-departure result assumes equal masses. Physical check The momentum constraints permit the directions, but energy identifies the required active release.

Question 4

Perpendicular departures do not prove elasticity for unequal masses

A 2kg2\,\mathrm{kg} projectile moving at 6m/s6\,\mathrm{m/s} along +x+x hits a stationary 1kg1\,\mathrm{kg} target. The projectile leaves at 30∘30^\circ and the target at −60∘-60^\circ. External impulse is negligible.

Diagram shown in the original SVG worksheet.

  1. Use the two momentum components to find both final speeds.

  2. Test whether the claimed event can be elastic or passive inelastic.

Question 4 - Solution

Perpendicular departures do not prove elasticity for unequal masses

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The two momentum equations are 12=2v1cos⁡30∘+v2cos⁡60∘,0=2v1sin⁡30∘−v2sin⁡60∘.12=2v_1\cos30^\circ+v_2\cos60^\circ,\qquad0=2v_1\sin30^\circ-v_2\sin60^\circ. The second gives v2=2v1/3v_2=2v_1/\sqrt3. Substitution into the first gives 12=43v1⇒v1=33,v2=6m/s.12=\frac4{\sqrt3}v_1\Rightarrow\boxed{v_1=3\sqrt3,\quad v_2=6\ \mathrm{m/s}}.

(b) Result and interpretation

Test the energy rather than assuming the right-angle rule: Ki=12(2)(6)2=36J,Kf=12(2)(27)+12(1)(36)=45J.K_i=\tfrac12(2)(6)^2=36\ \mathrm J,\qquad K_f=\tfrac12(2)(27)+\tfrac12(1)(36)=45\ \mathrm J. ΔK=+9J.\boxed{\Delta K=+9\ \mathrm J}. The event requires internal energy release. It is neither elastic nor passive inelastic; the usual perpendicular-departure result assumes equal masses.

Physical check

The momentum constraints permit the directions, but energy identifies the required active release.