Difference between revisions of "Forest UCM MnAM InElasticCol"
Line 27: | Line 27: | ||
or | or | ||
− | : v = \frac{}{} | + | : <math>v = \frac{2m}{M+2m}u</math> |
+ | |||
+ | b.) Now consider the case where they jump separately. The second hobo starts running AFTER the first hobo has jumped off. | ||
+ | |||
+ | Break the problem up into the two parts | ||
+ | |||
+ | PART A: The first hobo jumps off | ||
+ | |||
+ | ;Conservation of momentum | ||
+ | :<math>0 = m(u-v_1) - (m+M) v_1</math> | ||
+ | :<math>v_1 = \frac{2m}{M+2m}u</math>: same as before | ||
+ | |||
+ | But now the second hobo jumps off | ||
+ | |||
+ | :<math>m(u-v_1) - (m+M) v_1 = m(u-v_1) + m(u-v_2) - (M) v_2</math> | ||
+ | : -(m+M)\frac{2m}{M+2m}u= mu- (M+m) v_2</math> | ||
+ | : (M+m) v_2= mu + (m+M)\frac{2m}{M+2m}u</math> | ||
+ | : (M+m) v_2= \frac{m(M+2m)+2m(m+M)}{M+2m}u</math> |
Revision as of 11:47, 12 September 2014
An Inelastic collision conservers Momentum But Not energy
Consider a collision between two bodies of mass
and initially moving at speeds and respectively. They stick together after they collide so that each is moving at the same velocity after the collision.
If there are no external force then
- Conservation of momentum
Given that the amsses and initially velocities are known we can solve for v such that
Forest_UCM_MnAM#Inelastic_Collision_of_2_bodies
problem 3.4 two hobos
Two hobos are standing at one end of a stationary railroad flatcar of mass
. Each hobo has a mass and the flatcar has frictionless wheels. A hobo can run to the other end of the car and jump off with a speed with respect to the car.a.) Find the final speed of the car if both men run and jump off simultaneously.
At the instant the hobo jumps off with speed the railcar will move in the opposite direction at some speed . Since the hobo's speed is relative to the car, the hobos speed relative to the ground is .
- conservationof momentum
or
b.) Now consider the case where they jump separately. The second hobo starts running AFTER the first hobo has jumped off.
Break the problem up into the two parts
PART A: The first hobo jumps off
- Conservation of momentum
- : same as before
But now the second hobo jumps off
- -(m+M)\frac{2m}{M+2m}u= mu- (M+m) v_2</math>
- (M+m) v_2= mu + (m+M)\frac{2m}{M+2m}u</math>
- (M+m) v_2= \frac{m(M+2m)+2m(m+M)}{M+2m}u</math>