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Physics 2211, Spring 2002

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... a ball, period of a pendulum, two objects colliding) in a boxcar ... velocity will have the same results as the same experiments in a boxcar at rest. ... – PowerPoint PPT presentation

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Title: Physics 2211, Spring 2002


1
Physics 2211 Lecture 6Todays Agenda
  • Reference frames and relative motion

2
Inertial Reference Frames
  • A Reference Frame is the place from which you
    measure.
  • -- its where you nail down your (x,y,z) axes!
  • An Inertial Reference Frame (IRF) is one that is
    not accelerating.
  • We will consider only IRFs in this course.
  • Valid IRFs can have fixed velocities with respect
    to each other.
  • More about this later when we discuss forces.
  • For now, just remember that we can make
    measurements from different vantage points.

3
Newtons Principle of Relativity
  • Principle of Relativity (from Newton in 1600s)
  • The motion of bodies included in a given space
    are the same among themselves whether that space
    is at rest or moves uniformly forward in a
    straight line.
  • Newtons Principle of Relativity Restated
  • The laws of mechanics (Newtons Laws) are
    invariant (the same) in all inertial
    (non-accelerating) reference frames(IRFs).
  • OR
  • Absolute uniform motion (or absolute rest)
    cannot be detected.
  • Impact Experiments (e.g., dropping a ball,
    period of a pendulum, two objects colliding) in a
    boxcar moving with constant velocity will have
    the same results as the same experiments in a
    boxcar at rest.

4
Example(relative motion)
  • Kim is sitting on a train moving at 20 m/s. She
    is throwing a ball straight up and is catching it
    at the same place she threw it. The ball is in
    the air 1.5 s. Joe is standing on the ground by
    the railroad tracks and watches Kim as she throws
    the ball.
  • What is the initial speed of the ball and how
    high does it go
  • as seen by Kim?
  • as seen by Joe?

5
Example
  • The ball moves vertically in the IRF attached to
    the train (Kims IRF)

6
Example
  • But suppose the train is moving to the right in
    the IRF attached to the ground (Joes IRF).
  • From the grounds IRF, the balls motion exhibits
    projectile motion.

Galilean velocity transformation
7
Example
  • The initial velocity as see my Joe is
  • Magnitude of initial velocity (initial speed)
  • Angle above the horizontal

8
Example
  • Recall x and y components of motion are
    independent
  • Therefore, vertical (y) motion is the same both
    in both IRFs

9
Example
  • You are swimming across a 50m wide river in which
    the current moves at 1 m/s with respect to the
    shore. Your swimming speed is 2 m/s with respect
    to the water. You swim across in such a way that
    your path is a straight perpendicular line across
    the river.
  • How many seconds does it take you to get across
    ?(a) (b)(c)

50 m
2 m/s
10
Example
  • The time taken to swim straight across is
    (distance across) / (vy )
  • Since you swim straight across, you must be
    tilted in the water so thatyour x component of
    velocity with respect to the water exactly
    cancels the velocity of the water in the x
    direction

11
Example
12
Example(relative motion)
  • What is the boats velocity with respect to the
    shore if
  • the boat travels from point A to point B directly
    across?
  • the boat crosses in the shortest possible time?

13
Example
  • Apply Galilean Transformation

14
Example
15
Example
  • What is the boats velocity with respect to the
    shore if the boat crosses in the shortest
    possible time?
  • Time to cross the river is given by the distance
    travel (as measured on the shore) divided by the
    speed of the boat (as measured on the shore)

16
Example
17
Example
18
Recap for today
  • Reference frames and relative motion
  • For next time Review Chapter 3 in Tipler.
    Begin Chapter 4.
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