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    1.138J/2.062J/18.376J, WAVE PROPAGATION

    Fall, 2004 MIT

    Homework set no 3, Due Oct 21,2004

    1 Dispersion of waves in a beam

    Read notes Section 1.9, Chapter 1, Notes on beams. Start from equation (9.5) and

    assume that k ,E,I , are constants andp(x, t) = 0 .

    Examine a simple progressive wave

    V= Aeikxit (H.1.1)

    and find the dispersion relation between and k. Sketch the dependence of, the phase

    and group velocities, on k.

    Solve the inital-value problem by using exponential Fourier transform subject to

    V(x, 0) = f(x), Vt(x, 0) = 0, (H.1.2)

    where f(x) is a given even function ofx and vanishing for large x.

    Get the inverse transform formally, and then use the method of stationary phase to

    find the asymptotic behavior for fixed x/t but large t. Describ e the physics by sketching

    several snapshots for different t.

    2 Identity relating the reflection and and transmis-

    sion coifficients in a rod

    Let the rod cross section S(x) vary from one constant thorugh some general profile to

    another constant, i.e.,

    (H.2.3)S(x) S(x) S2, xS1, x ;

    where S1, S2 are two different constants. Consider monochromatic wave of fixed fre-

    quency so that

    U(x)eitu(x, t) = [ ] (H.2.4)

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    with2

    (S(U)) + SU= 0, < x

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    whered

    kx(x) = (H.3.13)dx

    By assuming that A(x), kx(x), h(x) vary slowly in x within a wavelength. show that to

    the leading order

    k(x) =

    kx(x)2

    + 2

    =

    gh(x) (H.3.14)

    What is the direction of local wave number vector k(x) = kx(x)ex + ey?

    How does the direction of wave, and the wave length and phase velocity change from

    deeper to shallower water?

    I will ask you to study the second order later.

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