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Help - Missing Step - Gas in a Tube

  1. Feb 22, 2004 #1
    Help ASAP --- Missing Step --- Gas in a Tube

    I am dealing with finding normal modes of oscillations in a continuum

    I have no problems with the string example, but now I have a gas in a tube, one side of the gas has pressure= p_0 and the other side p_0+delta p, they're separated by a wall that is lifted at t=0. This is a tube closed in the extremes.

    So, I've started with the classic wave equation for the tube
    rho is the density, P is the pressure, psi the movement
    (second partial derivatire of psi on t = second partial derivative of psi on x, times - rho_0 )and proposing the typical solution psi(x, t)= A cos(kx)cos(omega*t+phi). I also know the relationship between the speed of sound and pressure and density, and the value of delta rho.

    I start with the boundary conditions to solve for k, and now it is time to write out the initial conditions, and from there solve for A and phi. According to the string example, one of these conditions will end up as a function f(x) to be solved by Fourier.

    The problem is, I can't see for the life of me which are the initial conditions in a gas! And I can't see what kind of function it would be either. In a string I just see where the string is at time=0 and what velocity it has (usually 0), and according to its shape, I find the f(x) to use Fourier with.

    Please, anyone answer this, I've been trying to find it for the last 5 hours with no luck, the library is closed and my exam is tomorrow morning. And I apologize for the lack of LATeX.


  2. jcsd
  3. Feb 23, 2004 #2

    Tom Mattson

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    It would help if you would state the problem as it appears in the book.
  4. Feb 23, 2004 #3

    It's not a problem from a book, it's just the physical description of of oscillations of gas in a tube solved using Fourier analysis. It is not explained in the books I have, and I couldn't find the step by step analysis online (the usual example is a string) so that's why I asked. Anyway, my exam was this morning. Thanks.

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