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Physics 319 Classical Mechanics
G. A. Krafft Old Dominion University Jefferson Lab Lecture 5 G. A. Krafft Jefferson Lab
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Mechanical Momentum System of N particles: (vector) momentum is
As shown in Lecture 2, if there is no net external force acting on the system, momentum is conserved
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Inelastic Two Body Collision
Momentum before Momentum after Collision with stationary object
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Rockets and Jets Momentum Equation
Thrust vector (force acting on rocket or jet)
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Rocket Payload Relation
Integrated Limited velocity (independent how quickly burned!) In gravity (need results from later in course!) Therefore important to burn quickly!
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Center of Mass Definition of Center of Mass for system of N particles
Individual components Two bodies
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On Vector Joining 1 and 2 Closest to larger mass object
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Motion of the Center of Mass
Center of mass of a system of particle moves as if it were a particle with the total mass Mtot concentrated at the center of mass location For a continuous distribution
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Example: Center of Mass of a Cone
Center of mass on symmetry axis of cone Why? Calculation of Zcm
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