Center of Mass when sets act like single particles § 8.5.

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Presentation transcript:

Center of Mass when sets act like single particles § 8.5

Center of Mass Location of center of mass: weighted average of particle positions r cm =  m i r i /  m i

Center of Mass Velocity of center of mass: Time-derivative of position v cm = d/dt (  m i r i /  m i ) =  m i v i /  m i = p tot /m tot

Systems of Particles A net external impulse changes total momentum v cm changes accordingly

Isolated System Zero net external force v cm is constant

Group Work What determines which team wins a tug- of-war in space? (no external forces) System = (Team 1) + (Team 2) + (rope)

Group Poll Question Two joined cars of mass M and 2M are at rest with a compressed spring between them. After the spring fires, one car moves off to the right and the other to the left. The speed of the car on the left is A.Zero. B.equal to the one on the right. C.one half the speed on the right. D.twice the one on the right. E.warp nine.

Group Poll Question A fireworks shell is launched vertically into the air and at the top of its trajectory an explosive charge breaks the shell into two pieces. In which directions is it possible for the two pieces to move? The pieces do not necessarily have equal mass and the arrows indicate only the direction of the velocity, not the speed. A.A only B.A or B C.A, B, or C D.A,B,C, or D E.All of the above are possible F.None of the above are possible

Example Problem 8.97 A fireworks rocket is fired vertically upward. At its maximum height of 80 m it explodes and breaks into two pieces of mass 1.4 kg and 0.28 kg. In the explosion 860 J of chemical energy is released and converted into kinetic energy of the fragments. a)What is the speed of each fragment? b)If they hit the ground at the same time, what is the distance between them?

CM Reference Frame It is often convenient to analyze interactions in the reference frame with its origin at the center of mass. Total momentum is zero Particle momentums equal and opposite Speeds inversely proportional to masses Speeds same before and after elastic collisions