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Momentum, Impulse, and Collisions
Introduction to Momentum
Momentum is a fundamental concept in physics that quantifies the motion of an object. It is defined for any object with mass moving at a certain velocity and is a vector quantity, meaning it has both magnitude and direction.
Definition: The momentum p of an object is given by , where m is mass and \mathbf{v} is velocity.
Direction: Momentum points in the same direction as the velocity of the object.
Units: The SI unit of momentum is kilogram meter per second (kg·m/s).
Sign: If the object moves in the negative direction, both velocity and momentum are negative.
Example: A 4,000 kg truck moving right at 10 m/s has a momentum of kg·m/s to the right. An 800 kg racecar moving left at 50 m/s has kg·m/s to the left.
Impulse and Change in Momentum
Impulse is the effect of a force acting over a time interval, resulting in a change in momentum. It is closely related to Newton's Second Law.
Definition: Impulse J is given by .
Units: Impulse is measured in newton-seconds (N·s) or kg·m/s.
Relation to Work: While work changes kinetic energy, impulse changes momentum.
Example: Pushing a 50 kg crate with a 100 N force for 8 seconds delivers an impulse N·s, changing the crate's momentum by 800 kg·m/s.
Impulse from Force vs. Time Graphs
Impulse can be calculated as the area under a force vs. time graph. Positive areas (above the axis) add to impulse, while negative areas (below the axis) subtract from it.
Area Calculation: For rectangles, ; for triangles, .
Interpretation: The total area under the curve gives the net impulse delivered to the object.
Total Momentum of a System
The total momentum of a system is the vector sum of the momenta of all objects in the system. When objects interact, the system's total momentum is a key quantity.
System: A collection of interacting objects.
Formula:
Example: Two objects, A (4 kg, 12 m/s right) and B (5 kg, 9 m/s left), have total momentum kg·m/s to the right.
Conservation of Momentum
Conservation of momentum states that the total momentum of a system remains constant if no external forces act on it. This principle is fundamental in analyzing collisions and explosions.
Equation:
Application: Used for both collisions and push-away problems (e.g., recoil, explosions).
Example: A 4-kg rifle fires a 5-g bullet at 600 m/s. The recoil speed of the rifle is found by setting the total momentum before and after to zero (if initially at rest).
Types of Collisions
Collisions are classified based on whether kinetic energy is conserved:
Elastic Collision: Both momentum and kinetic energy are conserved.
Inelastic Collision: Only momentum is conserved; some kinetic energy is lost.
Completely Inelastic Collision: Objects stick together after collision, moving with the same final velocity.
Example: A 1 kg block at 20 m/s collides and sticks to a 9 kg block at rest. The final speed is found using conservation of momentum.
Identifying Collision Types
To determine the type of collision, follow a series of checks based on momentum and velocity conditions:
Check if momentum is conserved.
If objects stick together, it's completely inelastic.
If the sum of initial and final velocities matches for both objects, it's elastic.
Otherwise, it's inelastic.

Collisions with Energy Considerations
Some problems require using both conservation of momentum and conservation of energy, especially when motion after collision involves changes in height, springs, or friction.
Momentum Conservation: Used during the collision.
Energy Conservation: Used after the collision if no non-conservative work is done.
Equations:
(momentum)
(energy)
Example: A bullet embeds in a block, and the block slides up an incline. Use momentum conservation for the collision and energy conservation for the motion up the incline.
Elastic Collisions
In elastic collisions, both momentum and kinetic energy are conserved. For two objects, the following equations apply:
(for elastic collisions only)
For equal masses, the objects exchange velocities after a head-on elastic collision.
Center of Mass
The center of mass (C.O.M.) of a system is the weighted average position of all the mass in the system. It is useful for simplifying the analysis of motion for a group of objects.
Definition:
Properties: The C.O.M. is closer to the more massive objects in the system.
Application: Used to analyze the motion of systems as if all mass were concentrated at a single point.
Example: Two objects of 10 kg each at x = 0 and x = 4 m have a center of mass at m.
Summary Table: Types of Collisions
Type | Momentum Conserved? | Kinetic Energy Conserved? | Objects Stick Together? |
|---|---|---|---|
Elastic | Yes | Yes | No |
Inelastic | Yes | No | No |
Completely Inelastic | Yes | No | Yes |