Introduction
This is a classic two-dimensional collision problem involving conservation of momentum. Since the truck and car stick together after collision, it’s an example of a perfectly inelastic collision. We will use vector components to solve for the unknown initial speed of the truck and the final velocity after the collision.
Given Data
- Mass of car = m
- Mass of truck = 2m
- Initial speed of car (eastward) = 20 m/s
- Final direction of combined mass = 30º east of north
Step 1: Use Conservation of Momentum
Let vt be the speed of the truck before collision (to be calculated).
Let V be the speed of the combined object after collision (to be calculated).
We write x- and y-components of momentum:
Initial x-momentum: m × 20 (car only)
Initial y-momentum: 2m × vt (truck only)
Final momentum (combined mass 3m): 3m × V, at angle 30° east of north
Step 2: Break Final Momentum into Components
x-direction: 3mV sin(30º) = m × 20 → 3V × 0.5 = 20 → 1.5V = 20 → V = 13.33 m/s
Step 3: Now Solve for Truck’s Speed
y-direction: 3mV cos(30º) = 2m × vt
cos(30º) ≈ 0.866
3 × 13.33 × 0.866 = 2 × vt
34.63 = 2 × vt → vt = 17.31 m/s
Final Answers
- Speed of truck before collision: 17.31 m/s
- Speed after collision: 13.33 m/s at 30° east of north
Conclusion
This problem demonstrates how the principle of conservation of linear momentum applies in two-dimensional collisions. By breaking the momentum into components and equating them before and after the collision, we determine the unknown velocities of both the truck and the combined object.