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Thread: phase speed & group velocity

  1. #11
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    Hi again,

    Evenif wave number is, by definition, number of waves in unit distance (space),
    we may account that direction of space when we want to specify the direction
    of wave propagation.

    The 'k' and 'l' are wave numbers in X and Y directions.
    For a 2D wave, if we measure the wave characterestics along two axes
    (i.e. X and Y) we get two wave speed. They may or may not be equal,
    according to the geometry of the axis.

    Phase line of a wave is a "line through constant wave
    proporties", for example a line through constant height. It is equivalent
    to the "wave front".

    A figure is attached. It is partially redrawn from Pedlosky book. In that
    pciture, three items are shown. (1) A set of waves radiating from a
    source at the center and its phase line (b) A measure of wave number
    in XY plane at one part of the wave (c) A Physical view of wave propagation
    and "lines of constant height" (called phase lines).

    The phase speed along X-direction of the reference frame is the
    speed at which the "intersection of phase lines" at X-axis
    advances in time. Similiarly for the phase speed along Y-axis also.
    Now try to project the mean Wave Vector "K" onto X-axis and
    try to find its speed. That will be different from the former calculation.

    Key parameters,

    k = 2.pi./lamda_x
    l = 2.pi./lamda_y
    K = sqrt (k^2+l^2)
    C = w/K
    Cx = w/k = C.K/k (where BIG K=mean wave vector, BIG C=mean phase speed)
    Cy = w/l = C.K/l






    Thanks

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  2. #12
    Join Date
    Aug 2005
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    INCOIS
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    Thanks!!!

    HI Vinu,
    Thank you very much for the nice explanation and clarifications. I will be getting a copy of Pedlovsky's book soon and then I can explore it further.
    Regards,
    Sandhya.

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