Solving Partial Differential Equations with Laplace Transform

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The discussion focuses on solving a partial differential equation (PDE) using the Laplace transform. The initial and boundary conditions are provided, and the Laplace transform is applied to the PDE, leading to a derived equation. The eigenvalue is calculated, indicating it is always positive, which raises concerns about the behavior of the solution as x approaches infinity. Participants suggest reviewing the characteristic equation and the assumption of the solution form, noting that the ordinary differential equation is not homogeneous, which may lead to incorrect conclusions about the solution. The conversation emphasizes the importance of verifying each step in the solution process.
mliuzzolino
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Homework Statement



<br /> <br /> \dfrac{\partial^2 \varphi }{ \partial x^2} - \dfrac{\partial ^2 \varphi }{\partial t^2} = 1<br /> <br />

Initial Conditions:

\varphi (x, 0) = 1; \varphi_t (x, 0) = 1

Boundary Condition:

\varphi (0, t) = 1


On 0 \leq x &lt; \infty, 0 \leq t &lt; \infty


Homework Equations



Let {\Phi} denote the Laplace transform from t to s.

The Attempt at a Solution



Apply Laplace Transform to PDE:

<br /> <br /> \dfrac{\partial^2 \Phi }{ \partial x^2} - s^2\Phi + s\varphi (x, 0) + \varphi _t (x, 0) = \dfrac{1}{s}<br /> <br />

Apply Initial Conditions:

<br /> <br /> \dfrac{\partial^2 \Phi }{ \partial x^2} - s^2\Phi + s + 1 - \dfrac{1}{s} = 0<br /> <br />




<br /> <br /> \dfrac{\partial^2 \Phi }{ \partial x^2} - s^2\Phi + \dfrac{s^2 + s - 1}{s} = 0<br /> <br />


This leads to the eigenvalue being something like:

<br /> <br /> r = \dfrac{s^3 \pm \sqrt{s^6 - 4s(s^2 + s - 1)}}{2s}<br /> <br />

which is always positive for both cases.

The solution in Laplace space should be something like:

<br /> <br /> \Phi (x, s) = A(s) e ^{\dfrac{s^3 + \sqrt{s^6 - 4s(s^2 + s - 1)}}{2s}x} + B(s) e ^{\dfrac{s^3 - \sqrt{s^6 - 4s(s^2 + s - 1)}}{2s}x}<br /> <br />

and since the eigenvalue is always positive, as x goes to infinity the exponential terms will explode, requiring both A(s) and B(s) to be equal to 0.

What am I doing wrong? Any ideas?
 
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I would check your final calculation for the solution Φ in Laplace space. It seems to not depend on x, which is weird. If you're still working on this, that is.
 
mliuzzolino said:
<br /> <br /> \dfrac{\partial^2 \Phi }{ \partial x^2} - s^2\Phi + \dfrac{s^2 + s - 1}{s} = 0<br /> <br />This leads to the eigenvalue being something like:

<br /> <br /> r = \dfrac{s^3 \pm \sqrt{s^6 - 4s(s^2 + s - 1)}}{2s}<br /> <br />

which is always positive for both cases.

I would double-check this step. It looks like you assumed a solution ##\Phi(x,s) = e^{rx}##, and then tried to solve the characteristic equation ##r^2 - s^2 r + (s^2 + s -1)/s = 0##, but this equation for r is not correct. Your purely ordinary differential equation in x is not homogeneous - only two of your terms depend on ##\Phi##. If you plug in ##\Phi(x,s) = e^{rx}##, what happens when you try to divide out the ##e^{rx}## to get the characteristic equation for r?
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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