Lecture 12 13m

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    Transverse waves

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    Transverse waves on a string

    T

    x

    y

    x = y = 0

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    Horizontal forces:

    Vertical forces:

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    Solution of the wave equation

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    Boundary conditions

    l

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    Missing modes by arbitrary plucking

    F

    X

    All those modes having a node at X would be missing.

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    F

    Arbitrary disturbance may be expressed by a Fourier series

    with appropriate strengths of different modes.

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    Reflection and transmission of waves

    Y

    X=0

    TT

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    Boundary conditions

    X=0

    Y

    XNot possible

    T

    T

    X=0

    Y

    XPossible

    TT

    X=0

    Y

    X

    Not possible

    TT

    X=0

    Y

    X

    Possible

    T T

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    1

    1 1

    i r

    x xY f t f t

    c c

    2

    2

    t

    xY f t

    c

    0 0( ) i r ti Y Y f t f t f t Boundary conditions at X=0 for all time:

    120 0

    ( )i r t

    cY Yi i f t f t f t

    x x c

    12

    ( )i r t

    cf t f t f t K t

    c

    12

    i r t

    cf t f t f t

    c As K=0,

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    Reflection coefficient

    At X = 0

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    Transmission coefficient

    At X = 0

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    Stokes relations

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    Note

    But

    At X=0 for all time

    with and

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    Setting

    We also have

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    Special cases

    Case 1:

    Change in sign of reflected pulse

    Abrupt phase change of on reflection

    1 2 1 2 12 0c c r

    Case 2:1 2 1 2 12

    0c c r

    No change in sign of reflected pulse

    No abrupt phase change on reflection

    At the knot or joint (X = 0)

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    Case 3: for both the cases

    No phase change on transmission

    Case 4: At a fixed knot/joint

    Total reflection with an inversion of shape

    Case 5: At a free end with

    Total reflection without inversion of shape

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    Case 6: Impedance matching at the joint

    Total transmission without reflection