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Review from Last Lecture

Review from Last Lecture. Impulse Momentum “What force changes” Center of Mass “The average position” Conservation of Momentum Constant momentum in isolated systems Collisions. Elastic and Inelastic Collisions. In an inelastic collision the total kinetic energy is not conserved

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Review from Last Lecture

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  1. Review from Last Lecture • Impulse • Momentum • “What force changes” • Center of Mass • “The average position” • Conservation of Momentum • Constant momentum in isolated systems • Collisions

  2. Elastic and Inelastic Collisions • In an inelastic collision the total kinetic energy is not conserved • Momentum is conserved in any collision • Example: case where particles stick together (“perfectly inelastic”)

  3. Elastic and Inelastic Collisions • Example: Ballistic Pendulum

  4. Elastic and Inelastic Collisions • In an elastic collision the total kinetic energy is conserved • Now have two constraints (momentum and energy) • First consider 1D (sign of v meaningful) • Separate by masses

  5. Elastic and Inelastic Collisions • Separate by masses • Divide equations • Now solve

  6. Collisions in 2D • Momentum conserved in each direction • Consider one particle at rest in elastic collision • Need one more constraint!

  7. Rocket Propulsion • “Rockets can’t fly in vacuum. What do they have to push against?” • Nonsense. Rockets don’t push; they conserve momentum, and send parts (fuel) away from the body as fast as possible

  8. Rocket Propulsion • How fast do rockets accelerate? • Start with v, with mass M+Dm • Some time Dt later, have expelled Dm with velocity ve. To conserve momentum, rest of rocket (M) must have additional velocity (in the other direction) of Dv = -ve Dm/M

  9. Rocket Propulsion • How fast do rockets accelerate? • Thrust: (instantaneous) force on rocket

  10. Rotation of Rigid Object • A rigid object is one in which the relative positions of all the parts is fixed • What happens when we rotate this object? • All points move in a circle about the axis • How far do they move? • Note that q is unitless (ratio of distances) but “measured” in radians

  11. Rotation of Rigid Object • What if the object is “spinning” • It turns thru a given angle every second • Define the “angular velocity” • Angular velocity measured in radians per second (rad/s or s-1) • What if it’s “spinning up” • Angular acceleration

  12. Rotation of Rigid Object • While q is a scalar, w and a are really vectors • Use “right hand rule” to determine w • For a, it’s in the same direction if the magnitude of w is increasing

  13. Linear to Angular and Back • For each linear quantity (x,v,a) there is a corresponding angular quantity connected by r • Note that centripetal acceleration is now:

  14. Linear to Angular and Back • This angular-linear correlation extends to the kinematic equations as well

  15. Rotational Kinetic Energy • What is the kinetic energy of a spinning object? • Just the sum of it’s parts! • Call I the Moment of Inertia

  16. Rotational Kinetic Energy • What is the kinetic energy of a rolling object? • Note that for a given energy, a larger I gives a smaller v. • Hoops on a ramp go slower than disks

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