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Solution of unsteady linearized potential flow PDE

  1. Oct 1, 2015 #1
    Hi,

    I have a problem following the solution of a linearized potential flow equation in a publication by Fung.

    The problem describes potential flow over an oscillating plate. A boundary layer is approximated by defining a subsonic layer over the panel and supersonic flow above the subsonic flow. From the equation of motion (1) and (2) in combination with a standing wave condition of the wall (8) and traveling wave of the perturbations (9) and (10) it seems to be easy to get the solutions (12) and (13).

    https://dl.dropboxusercontent.com/u/20358584/fung1.png [Broken]
    https://dl.dropboxusercontent.com/u/20358584/fung2.png [Broken]

    Can anyobody give me hint of how to get to this solution? The paper is the following:
    [/PLAIN] [Broken]
    http://arc.aiaa.org/doi/abs/10.2514/3.1661

    Many thanks in advance!!!

    https://dl.dropboxusercontent.com/u/20358584/fung3.png [Broken]
     
    Last edited by a moderator: May 7, 2017
  2. jcsd
  3. Oct 1, 2015 #2

    Andy Resnick

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    When I am confronted with "it's easy to see that..." I usually first try substituting the answer into the expression and seeing what happens- sometimes there's an oddball change of variables or trig identity involved.
     
  4. Oct 29, 2015 #3
    I don't know. This doesn't help. What could he have done? I've heard that Duhamel's principle could be an approach of solving non-homogenious PDEs like the wave equation. Could the solution have something to do with this approach?

    Substituting (13) in (2) gives:
    [itex] \begin{equation} [-\frac{1}{a_{\delta}^2} \omega^2 - \frac{2M_{\delta}}{a_{\delta}} \alpha_{\nu}\omega + \beta_{\delta}^2\alpha_{\nu}^2 + \zeta_{\delta}^2] \cdot e^{i(\omega t + \alpha_{\nu} x)} \cdot [C_{\nu} sin(\zeta_{\nu}y ) + D_{\nu} cos(\zeta_{\nu}y) ] = 0 \end{equation} [/itex]
     
    Last edited: Oct 29, 2015
  5. Nov 2, 2015 #4
    Oh... the substitution was absolutely wrong. I need to find the correlation between the potential and z..
     
  6. Nov 4, 2015 #5
    I made some progress to get equation (14) and (15). Not sure if I can already corellate the fourer constant alpha with the wave number.

    [latex]
    The equation of motion:
    \begin{equation}
    \frac{1}{a^2}\frac{\partial^2\phi}{\partial t^2} + \frac{2M}{a} \frac{\partial^2 \phi}{\partial x \partial t} + \overline{\beta}^2 \frac{\partial^2 \phi}{\partial x^2} = \frac{\partial^2 \phi}{\partial y^2}
    \label{eq:01}
    \end{equation}
    The potential must oscillate harmonically:
    \begin{equation}
    \phi = \Psi(x,y)e^{i\omega t}
    \label{eq:02}
    \end{equation}
    This yields:
    \begin{equation}
    \Big(\frac{i\omega}{a}\Big)^2\Psi + 2i\frac{\omega M}{a} \frac{\partial \Psi}{\partial x} + \overline{\beta}^2 \frac{\partial^2 \Psi}{\partial x^2} = \frac{\partial^2 \Psi}{\partial y^2}
    \label{eq:03}
    \end{equation}
    A double Fourier transformation in x and y:
    \begin{equation}
    \Psi^* = \int_{-\infty}^{\infty}\int_{-\infty}^{\infty} e^{-i(\gamma y + \alpha x)} \Psi(x,y) dx dy
    \label{eq:04}
    \end{equation}
    If this Fourier transformation is applied to all terms of Eq.~(\ref{eq:03}) then $\Phi^*$ cancels out and (\ref{eq:03}) can be written as:
    \begin{equation}
    \frac{\omega^2}{a^2} + 2 \frac{\omega M}{a} \alpha + \overline{\beta}^2 \alpha^2 = \gamma^2
    \end{equation}
    This is equation (14) in the publication from Fung. The same approach for Fungs equation (2) yields (15). Can I already assume that $\gamma$ is $\gamma_{\nu}$ and $\alpha$ is $\alpha_{\nu}$?
    [/latex]
     
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