Collisions in Two Dimensions — Question 2

Section 9-10 · Physics pages 1334–1335

Question 2 Why equal-mass elastic departures are perpendicular A puck strikes an identical stationary puck elastically on a frictionless plane. Initially⃗ u = (10, 0) m/s. Both pucks move after collision, and the incident puck leaves at 30◦above +x.⃗ u1⃗ v1⃗ v2 Incident motion is horizontal; departure directions are 30 and -60 degrees. (a) Prove that their final velocities are perpendicular. (b) Find both final speeds and the target's direction.
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Question 2 - Solution Why equal-mass elastic departures are perpendicular⃗ u1⃗ v1⃗ v2 (a) Derivation and calculation For equal masses, momentum conservation gives⃗u =⃗v1 +⃗v2. Square this relation and compare with elastic energy conservation: u2 = v2 1 + v2 2 + 2⃗v1 ·⃗v2, u2 = v2 1 + v2 2.⃗ v1 ·⃗v2 = 0 . Both velocities are nonzero, so their departure directions are perpendicular. (b) Result and interpretation The velocity triangle has hypotenuse u = 10 m/s: v1 = u cos 30◦= 5 √ 3 m/s , v2 = u sin 30◦= 5 m/s . Vertical momentum cancellation selects the target direction below the axis: θ2 = 30◦−90◦= −60◦. Physical check The squared final speeds sum to 75 + 25 = 100 m2/s2.

Question 2

Why equal-mass elastic departures are perpendicular

A puck strikes an identical stationary puck elastically on a frictionless plane. Initially u→=(10,0)m/s\vec u=(10,0)\,\mathrm{m/s}. Both pucks move after collision, and the incident puck leaves at 30∘30^\circ above +x+x.

Diagram shown in the original SVG worksheet.

  1. Prove that their final velocities are perpendicular.

  2. Find both final speeds and the target's direction.

Question 2 - Solution

Why equal-mass elastic departures are perpendicular

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For equal masses, momentum conservation gives u→=v→1+v→2\vec u=\vec v_1+\vec v_2. Square this relation and compare with elastic energy conservation: u2=v12+v22+2v→1⋅v→2,u2=v12+v22.u^2=v_1^2+v_2^2+2\vec v_1\cdot\vec v_2,\qquad u^2=v_1^2+v_2^2. v→1⋅v→2=0.\boxed{\vec v_1\cdot\vec v_2=0}. Both velocities are nonzero, so their departure directions are perpendicular.

(b) Result and interpretation

The velocity triangle has hypotenuse u=10u=10 m/s: v1=ucos⁡30∘=53m/s,v2=usin⁡30∘=5m/s.\boxed{v_1=u\cos30^\circ=5\sqrt3\ \mathrm{m/s}},\qquad\boxed{v_2=u\sin30^\circ=5\ \mathrm{m/s}}. Vertical momentum cancellation selects the target direction below the axis: θ2=30∘−90∘=−60∘.\boxed{\theta_2=30^\circ-90^\circ=-60^\circ}.

Physical check

The squared final speeds sum to 75+25=10075+25=100 m2^2/s2^2.