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An overview of the concept of momentum, its calculation, and its conservation in various scenarios such as collisions, shooting a gun, rocket propulsion, and explosions. It also introduces the concept of rotational momentum and its relationship with rotational inertia.
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momentum is equal to the product of an object’s mass and its velocity.
p = m v
150 kg offensive lineman runs 5 m/s
p = (150 kg)(5 m/s) = 750 kg m/s
90 kg running back runs 9 m/s
p = (90 kg)(9 m/s) = 810 kg m/s
The running back has more momentum.
When two cars crash and stick together the momentum is conserved. The two cars will move together with the same final velocity.
m 1 v 1 + m 2 v 2 = (m 1 + m 2 )vf
Two cars of the same weight crash into each other. One of the cars was initially sitting still.
mv 0 + m(0) = (m+m)vf
vf = ½ v 0
The cars move together with half the velocity of the first car.
We can use the equation on the previous slide to determine how fast a gun shoots.
By firing a bullet into a block and knowing the masses and the speed the block obtains after being shot, we can calculate how fast the bullet was shot.
This is easy to do as long as the block is a lot more massive than the bullet.
Works the same as shooting a gun, except you
are continuously firing ‘bullets’ (expelling gas).
Gas gets momentum in one direction.
The rocket gets momentum in the opposite
direction.
An explosion can be treated as a collision in
reverse.
First an object has a momentum.
After the explosion, all the momentums of the
individual fragments add up to the original
momentum.
If you want to change the momentum of an object, an outside force is required.
F = p/ t
F t = p
F t is called an impulse.
Impulse equals the change in momentum
Rotational inertia – an objects tendency to resist changes in how fast it spins. This is the rotational analogy to mass. This is determined by how far the mass is from the rotation point.
angular velocity – the rate that an object spins.
Race a hoop against a disk. (each of radius r)
All of the hoop’s mass is r away from the center.
Some of the disk’s mass is closer than r from center.
The hoop has more rotational inertia. Harder for the hoop to start rolling. Angular velocity of the hoop speeds up slower.