Kinetics of Particles: Impulse and Momentum

Example: Braking Car (Impulse-Momentum Method)

Example

A 1500 kg1500 \text{ kg} car is traveling at 20 m/s20 \text{ m/s}. The driver applies the brakes, resulting in a constant braking force of 6000 N6000 \text{ N}. How long will it take for the car to stop?

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Example: Train Car Collision

Example

A 10,000 kg10,000 \text{ kg} train car A traveling at 5 m/s5 \text{ m/s} strikes a stationary 15,000 kg15,000 \text{ kg} train car B. The cars couple together (perfectly plastic impact). Determine their common velocity after the collision and the percentage of kinetic energy lost.

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Example: Two-Dimensional Elastic Collision

Example

Two identical hockey pucks, A and B (mass m=0.15 kgm = 0.15 \text{ kg} each), slide on a frictionless horizontal ice surface. Puck A is moving at 4 m/s4 \text{ m/s} along the x-axis and strikes puck B, which is initially at rest. The collision is perfectly elastic (e=1e = 1). After the collision, puck A moves off at an angle of 3030^\circ above the x-axis. Determine the final velocities of both pucks and the direction of puck B's motion.

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Example: Conceptual Case Study - Bouncing Balls and the Coefficient of Restitution

Example

A tennis ball and a seemingly identical "sad" ball (made of a highly inelastic rubber compound) are dropped simultaneously from the same height onto a hard floor. The tennis ball rebounds to a significant portion of its original height, while the sad ball barely bounces at all. Analyze the physical differences in these collisions in terms of impulse, deformation, and the coefficient of restitution (ee).

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Example: Conceptual Case Study - Recoil of a Cannon

Example

A stationary cannon fires a heavy projectile horizontally. The cannon immediately recoils backward. Analyze this event using the principle of conservation of momentum. Explain why the cannon recoils much slower than the projectile travels forward, and how a recoil mechanism (like a spring-damper system) utilizes impulse to safely stop the cannon.

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