# Momentum Problems

On this page I put together a collection of momentum problems to help you understand momentum better. The required equations and background reading to solve these problems is given on the momentum pages on the

dynamics page.

**Problem # 1**
A particle has a mass of 10 kg and a velocity of 5 m/s. What is the momentum of the particle? (Answer: 50 kg.m/s)

**Problem # 2**
An impulse of 20 kg.m/s acts on the particle in problem # 1, in the same direction as the velocity. What is the final velocity of the particle? (Answer: 7 m/s)

**Problem # 3**
If the impulse in problem # 2 is delivered for a duration of 0.5 seconds, what is the average force acting on the particle? (Answer: 40 N)

**Problem # 4**
An elastic collision occurs in one dimension, in which a 10 kg block traveling at 5 m/s collides with a 5 kg block traveling at 3 m/s in the same direction. What are the velocities of the two blocks immediately after the collision? (Answer: 3.67 m/s, 5.67 m/s)

**Problem # 5**
An inelastic collision occurs in one dimension, in which a 10 kg block traveling at 5 m/s collides with a 5 kg block traveling at 3 m/s in the same direction, and they stick together. What are the velocities of the blocks immediately after the collision? (Answer: 4.33 m/s)

**Problem # 6**
A simple and practical understanding of conservation of momentum problems is given by the following: When a figure skater makes a jump, he increases his rotation speed by pulling together his arms and legs. This reduces his rotational inertia causing him to spin faster. If the initial spin rate of a figure skater is 1 RPM and he decreases his rotational inertia by half during the spin, what is his final spin rate? (Answer: 2 RPM)

**Problem # 7**
When two billiard balls collide the collision is assumed to be elastic. Show that for a general case, where the collision is not head on, the cue ball moves in a direction perpendicular to the direction of the object ball, after impact. Assume that the balls have the same mass and the object ball is initially at rest.

(For the answer see the

physics of billiards page)

**Problem # 8**
A solid ball of mass

*m* and radius

*r* is rolling without slipping on a flat horizontal surface, at an initial angular velocity

*w*_{1}. It hits a small bump of height

*h*. What is the angular velocity of the ball immediately after impact? Also, what is the minimum initial angular velocity

*w*_{1} so that the ball just makes it over the bump? What is the minimum initial speed of the ball?

Assume that the ball pivots about the tip of the bump during, and after impact.

(For the answer see the

impulse and momentum page)

**Problem # 9**
In the

angular momentum page we showed how the angular momentum equations for a rigid body are derived. The figure below shows the set up used for the derivation.

Where:

*r*_{iG} is the position vector from point

*G* (the center of mass of the rigid body) to the location of

*m*_{i}. This vector is measured relative to the local

*xyz* axes

*m*_{i} is the mass of a small, arbitrary mass element in the rigid body. This mass element is small enough to be considered a particle

*w* is the angular velocity vector of the rigid body with respect to ground

Introduce the following new variables:

*r*_{i} is the position vector from the origin

*o* of the global XYZ frame (ground) to particle

*i*. This vector is measured relative to the local

*xyz* axes

*r*_{G} is the position vector from point

*o* to point

*G*. This vector is measured relative to the local

*xyz* axes

*v*_{i} is the velocity vector of particle

*i* with respect to ground and with components resolved along the local

*xyz* axes

*v*_{G} is the velocity vector of point

*G* with respect to ground and with components resolved along the local

*xyz* axes

*v*_{iG} is the velocity vector of this mass element relative to point

*G*, and with components resolved along the local

*xyz* axes

The following vector equation defines the angular momentum (

*H*_{oi}) of an arbitrary particle

*i*, about an arbitrary ground reference point

*o*:

*H*_{oi} =

*r*_{i}x

*m*_{i}*v*_{i} (where 'x' represents the vector cross product)

If we set,

*r*_{i} =

*r*_{G}+

*r*_{iG}
and

*v*_{i} =

*v*_{G}+

*v*_{iG}
show that the angular momentum (

*H*_{o}) of a rigid body about an arbitrary ground reference point

*o* is given by:

*H*_{o} =

*Σ**H*_{oi} =

*m**r*_{G}x

*v*_{G}+

*H*_{G}
where

*m* is the mass of the rigid body,

*Σ* represents summation over all the particles in the rigid body, and

*H*_{G} is the angular momentum of the rigid body about point

*G*, as given by equation (6) on the

angular momentum page. The above equation can be very useful when solving certain momentum problems, as shown in the next problem.

**Problem # 10**
See the problem,

Cat righting reflex. This is an excellent real-world example to aid your understanding of conservation of momentum problems.

Return from **Momentum Problems** to **Physics Questions** page
Return from **Momentum Problems** to **Real World Physics Problems** home page