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Physics 2211: Lecture 38 Todays Agenda

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one period T so its speed is v = / T = f. ... Consider a pulse propagating along a string: v 'Snap' a rope to see such a pulse ... – PowerPoint PPT presentation

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Title: Physics 2211: Lecture 38 Todays Agenda


1
Physics 2211 Lecture 38Todays Agenda
  • Conceptual discussion of wave motion
  • Wave properties
  • Mathematical description
  • Waves on a string

2
What is a wave ?
  • A wave is a traveling disturbance that transports
    energy but not matter.
  • Examples
  • Sound waves (air moves back forth)
  • Stadium waves (people move up down)
  • Water waves (water moves up down)
  • String waves (string moves up down)
  • Light waves (what moves??)

3
Types of Waves
  • Transverse The medium oscillates perpendicular
    to the direction the wave is moving.
  • Water waves
  • Wave on a string
  • Light waves
  • Slinky
  • Longitudinal The medium oscillates in the same
    direction as the wave is moving
  • Sound waves
  • Slinky
  • We will deal only with transverse waves in this
    course!

4
Wave Properties
  • Wave Number k 2p/l

y
x
5
Wave Properties...
  • Period The time T for a point on the wave to
    undergo one complete oscillation.
  • Frequency The number of complete oscillations
    per second, f 1/T.
  • Speed A traveling harmonic wave moves one
    wavelength ? in one period T so its
    speed is v ??/ T ? f.

6
t 0
t T/4
t T/2
t 3T/4
t T
7
Wave Properties...
  • We will show that the speed of a wave is a
    constant that depends only on the medium, not on
    amplitude, wavelength, or frequency.
    ? and f are related by v
  • For a given frequency and medium, wavelength is
    determined ? v / f
  • Note that v ??/k since ?? 2? f ?and k
    2? / ? ?????????????
  • Units f cycles/sec or hertz (Hz)
  • ? rad/sec
  • k m-1

8
Wave Forms
  • So far we have examined continuous waves that
    go on forever in each direction!
  • We can also have pulses caused by a brief
    disturbanceof the medium

9
Mathematical Description
  • Suppose we have some function y f(x)

0
  • Let a v t Then
  • f(x - v t) will describe the same shape
    moving to the right with speed v.

v
10
Math...
y
?
  • Consider a wave that is harmonic in x and has a
    wavelength of ?.

A
x
In general, this wave has the function form
v
y
  • Now, if this is moving tothe right with speed v
    it will be described by

x
11
Math...
  • So we see that a simple harmonic wave moving with
    speed v in the x direction is described by the
    equation
  • By using

and
we can write this as
(what about moving in the -x direction?)
12
Traveling Wave Summary
?
y
  • describes a
    harmonic wave ofamplitude A moving in the x
    direction.

A
x
  • Each point on the wave oscillates in the y
    direction withsimple harmonic motion of angular
    frequency ? 2pf.
  • The quantity k is called the wave number.
  • The speed of the wave is .

13
Wave Particle Kinematics
?
y
  • Vertical speed of a point on the wave

A
x
  • Maximum vertical speed of a point on the wave
  • Vertical acceleration of a point on the wave
  • Maximum vertical acceleration of a point on the
    wave

14
Waves on a string
  • What determines the speed of a wave?
  • Consider a pulse propagating along a string
  • Snap a rope to see such a pulse
  • How can you make it go faster?

15
Waves on a string...
Suppose
  • The tension in the string is F
  • The mass per unit length of the string is ?
    (kg/m)
  • The shape of the string at the pulses maximum is
    circular and has radius R

F
?
R
16
Waves on a string...
  • Consider moving along with the pulse
  • Apply F ma to the small bit of string at the
    top of the pulse

v
17
Waves on a string...
  • The total force FNET is the sum of the tension F
    at each end of the string segment.
  • The total force is in the -y direction.

?
?
F
F
FNET 2F ? ?
(since ? is small, sin ? ?)
18
Waves on a string...
  • The mass m of the segment is its length (R x 2?)
    timesits mass per unit length ?.

m R 2???
?
?
??
R
19
Waves on a string...
  • The acceleration a of the segment is v 2/ R
    (centripetal)in the -y direction.

v
a
R
20
Waves on a string...
  • So FNET ma becomes

a
FTOT
m

21
Waves on a string...
  • So we find

v
tension F
mass per unit length ?
  • Making the tension bigger increases the speed.
  • Making the string heavier decreases the speed.
  • As we asserted earlier, this depends only on the
    nature of the medium, not on amplitude,
    frequency, etc. of the wave.

22
Recap of todays lecture
  • Conceptual discussion of wave motion
  • Wave properties
  • Mathematical description
  • Waves on a string
  • Review Chapter 15 in Tipler Read
    Chapter 16.
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