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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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