Collisions in Two Dimensions — Question 5

Section 9-10 · Physics pages 1340–1341

Question 5 A smooth contact transfers only the normal velocity component Two identical smooth spheres collide elastically on a frictionless plane. At contact the unit vector from sphere 1 to sphere 2 is ˆn = (3/5, 4/5). Initial velocities are⃗u1 = (5, 0) and⃗u2 = 0 m/s. Ignore spin. ˆn⃗ u1 Contact normal joins the centers; the spheres touch. (a) Find both final velocity vectors by resolving along and perpendicular to ˆn. (b) Check momentum, kinetic energy and separation along the contact normal.
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Question 5 - Solution A smooth contact transfers only the normal velocity component ˆn⃗ u1 (a) Derivation and calculation Project the incident velocity onto the contact normal: u1n =⃗u1 · ˆn = (5, 0) · (3/5, 4/5) = 3 m/s. Equal masses exchange normal components while smooth contact leaves tangential components unchanged:⃗ v2 = 3ˆn = (9/5, 12/5) ,⃗ v1 = (5, 0) −3ˆn = (16/5, −12/5) m/s . (b) Result and interpretation Check all three requirements:⃗ v1 +⃗v2 = (5, 0) =⃗u1, v2 1 + v2 2 = 16 + 9 = 25 = u2 1. (⃗v2 −⃗v1) · ˆn = (−7/5, 24/5) · (3/5, 4/5) = 3 > 0. Thus momentum and energy are conserved, and the surfaces separate after contact. Physical check The contact impulse is parallel to the line joining the centers.

Question 5

A smooth contact transfers only the normal velocity component

Two identical smooth spheres collide elastically on a frictionless plane. At contact the unit vector from sphere 1 to sphere 2 is n̂=(3/5,4/5)\hat n=(3/5,4/5). Initial velocities are u→1=(5,0)\vec u_1=(5,0) and u→2=0m/s\vec u_2=0\,\mathrm{m/s}. Ignore spin.

Diagram shown in the original SVG worksheet.

  1. Find both final velocity vectors by resolving along and perpendicular to n̂\hat n.

  2. Check momentum, kinetic energy and separation along the contact normal.

Question 5 - Solution

A smooth contact transfers only the normal velocity component

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Project the incident velocity onto the contact normal: u1n=u→1⋅n̂=(5,0)⋅(3/5,4/5)=3m/s.u_{1n}=\vec u_1\cdot\hat n=(5,0)\cdot(3/5,4/5)=3\ \mathrm{m/s}. Equal masses exchange normal components while smooth contact leaves tangential components unchanged: v→2=3n̂=(9/5,12/5),v→1=(5,0)−3n̂=(16/5,−12/5)m/s.\boxed{\vec v_2=3\hat n=(9/5,12/5)},\qquad\boxed{\vec v_1=(5,0)-3\hat n=(16/5,-12/5)\ \mathrm{m/s}}.

(b) Result and interpretation

Check all three requirements: v→1+v→2=(5,0)=u→1,v12+v22=16+9=25=u12.\vec v_1+\vec v_2=(5,0)=\vec u_1,\qquad v_1^2+v_2^2=16+9=25=u_1^2. (v→2−v→1)⋅n̂=(−7/5,24/5)⋅(3/5,4/5)=3>0.(\vec v_2-\vec v_1)\cdot\hat n=(-7/5,24/5)\cdot(3/5,4/5)=3>0. Thus momentum and energy are conserved, and the surfaces separate after contact.

Physical check

The contact impulse is parallel to the line joining the centers.