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Physics 2111 Unit 23 Today’s Concept: Waves Wave Equation Resonance Energy Mechanics Lecture 23, Slide 1

Physics 2111 Unit 23 - College of DuPageTypes of Waves Longitudinal: The medium oscillates in the same direction as the wave is moving. Mechanics Lecture 23, Slide 3 Transverse: The

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  • Physics 2111

    Unit 23

    Today’s Concept:

    Waves

    Wave Equation

    Resonance

    Energy

    Mechanics Lecture 23, Slide 1

  • 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) Light waves (what moves?)

    Mechanics Lecture 23, Slide 2

  • Types of Waves

    Longitudinal: The medium oscillates in the same direction as the wave is moving.

    Mechanics Lecture 23, Slide 3

    Transverse: The medium oscillates perpendicular to the direction the wave is moving.

    • Waves on a string

    • Water waves

    • Light Waves

    • Sound Waves

  • How to make a Function Move

    Suppose we have some function y = f (x):

    x

    y

    0

    Mechanics Lecture 23, Slide 4

    f (x - a) is just the same shape moveda distance a to the right:

    x = ax

    y

    0

    Let a = vt Then

    f (x - vt) will describe the same shape moving to the right with speed v.

    x = vt

    v

    x

    y

    0

  • If a function moving to the right with speed v is described by f (x - vt) then what describes the same function moving to the left with speed v?

    v

    x

    y

    0

    y = f (x - vt)

    v A) y = - f (x - vt)

    B) y = f (x + vt)

    C) y = f (-x + vt)

    Question

    Mechanics Lecture 23, Slide 5

    x

    y

    0x

    y

    0x

    y

  • Harmonic Wave

    Consider a wave that is harmonic in xand has a wavelength of .

    Mechanics Lecture 23, Slide 6

    Has the functional form:

    xAxy

    2cos)(

  • Harmonic Wave

    Mechanics Lecture 23, Slide 7

    2

    ( ) cosy x A x vt

    -

    cos( )A kx t -

    Give it speed v

    =Acos(2𝜋

    𝜆𝑥 −

    2𝜋

    𝜆𝑣𝑡)

    v=/P

  • Amplitude:

    The maximum displacement A of a point on the wave.

    A

    Wavelength: The distance between identical points on the wave.

    Period: The time P it takes for an element of the medium to make one complete oscillation.

    cos( )y A kx t -

    Pv

    k

    2k

    f2

    P

    2

    Wave Properties

    Mechanics Lecture 23, Slide 8

    Wavelength

    Not the spring constant!

    position(x)

  • NOTE:

    Wave Properties

    Mechanics Lecture 23, Slide 9

    PeriodP

    Same plot but vs time

    time(t)

  • Question

    Mechanics Lecture 23, Slide 10

    A boat is moored in a fixed location and waves make it move up

    and down. If the spacing between wave crests is L and the

    speed of the waves is v, how much time Δt does it take the boat

    to go from the top of one wave to the top of the next?

    A. Δt = L/v

    B. Δt = Lv

    C. Δt = v/L

  • You shake a rope up and down a distance of 40cm with a frequency of 10Hz. The wave formed has a velocity of 5m/sec. What is the equation for this wave?

    Example 23.1 (Traveling Wave)

    Mechanics Lecture 23, Slide 11

  • Example 23.2: Wave Graph

    Mechanics Lecture 11, Slide 12

    The figure to the left shows

    height vs. displacement plot for a

    string which has a wave traveling

    in the positive x direction at time

    t=5.0 sec with a velocity of 12.0

    m/sec.

    a) What is the amplitude of this wave?

    b) What is the wavelength of this wave?

    c) What is the frequency of this wave?

    d) What is the equation of motion of this string? (i.e. y(x,t)=?)

    e) What is the vertical (y) velocity of a piece of string at the

    point labeled 1?

    f) What is the vertical (y) acceleration of a piece of string at

    the point labeled 1?

  • Mechanics Lecture 23, Slide 13

  • You have a 2m long piece of string that has a mass of 0.6 grams. If you loop it over a pulley and hang a 200gram mass from one end, what is the velocity of wave in the string?

    Example 23.2 (Wave Speed)

    Mechanics Lecture 23, Slide 14

  • Linear Superposition

    What happens when two waves “collide”?

    x

    Mechanics Lecture 23, Slide 15

    x

    Constructive Interference

  • Or……

    Destructive Interference

    x

    Mechanics Lecture 23, Slide 16

    x

    Demo

    http://phet.colorado.edu/sims/wave-on-a-string/wave-on-a-string_en.html

  • Y(x,t) = 2*cos(kx)*cos(t)

    In the equation we just derived, when is the value of Y always equal to zero?

    A. When kx = 0

    B. When kx = /2

    C. When kx =

    D. (A) and (C)

    E. Y varies with time and isn’t always zero anywhere

    Question

    Mechanics Lecture 23, Slide 17

  • Resonance

    Mechanics Lecture 23, Slide 18

    Fundamental

    1st harmonic

    1st Overtone

    2nd harmonic

    2nd Overtone

    3rd harmonic

    L

    L = n* /2Resonant frequencies for strings always node at both ends

  • CheckPoint

    Mechanics Lecture 23, Slide 19

    L

    The wave length of the above wave is:

    A. 2 L

    B. 1.5 L

    C.1 L

    D.2/3 L

    E. 0.5 L

  • L = n* /2

    Resonant frequencies

    Mechanics Lecture 23, Slide 20

    L = n* (v/f)/2

    f= v*n/(L 2)

    Velocity -

    determined

    by tension

    and density

    of string

    (v2 = T/m

    Length of

    string

    But what is n?

  • Resonance

    Mechanics Lecture 23, Slide 21

    Fundamental

    1st harmonic

    1st Overtone

    2nd harmonic

    2nd Overtone

    3rd harmonic

    L

    f= v*n/(L 2)

    n = 1

    n = 2

    n = 3

  • When you tune a guitar, you are adjusting what resonant frequency at which each string will vibrate. You do this by:

    A. Adjusting the length of the string

    B. Adjusting the density of the string

    C. Adjusting the tension in the string

    D. Adjusting the speed of sound near the string

    Question

    Mechanics Lecture 23, Slide 22

  • When you play a guitar, you are also adjusting what resonant frequency at which each string will vibrate. You do this by:

    A. Adjusting the length of the string

    B. Adjusting the density of the string

    C. Adjusting the tension in the string

    D. Adjusting the speed of sound near the string

    Question

    Mechanics Lecture 23, Slide 23

  • In our previous example problem, we had a 2m long piece of string that has a mass of 0.6 grams. We looped it over a pulley and hung a 200gram mass from one end. What is fundamental frequency of the string?

    Example 23.3 (fundamental frequency)

    Mechanics Lecture 23, Slide 24

    5m

  • The velocity we find using the formula

    is the velocity of the wave.

    Velocity

    Mechanics Lecture 23, Slide 25

    2 Tvm

    The velocity of any little piece of the string varies with time. We get it by taking the derivative of y(x,t) = A*cos(kx-t)

  • Energy

    Mechanics Lecture 23, Slide 26