Solving Partial Differential Equations with Laplace Transform

In summary, the conversation discusses solving a PDE using the Laplace transform and applying initial conditions. The final calculation for the solution in Laplace space is incorrect, as it does not depend on x. The step involving the characteristic equation is also incorrect, as the PDE is not homogeneous.
  • #1
mliuzzolino
58
0

Homework Statement



[itex]

\dfrac{\partial^2 \varphi }{ \partial x^2} - \dfrac{\partial ^2 \varphi }{\partial t^2} = 1

[/itex]

Initial Conditions:

[itex] \varphi (x, 0) = 1; \varphi_t (x, 0) = 1 [/itex]

Boundary Condition:

[itex] \varphi (0, t) = 1 [/itex]


On [itex] 0 \leq x < \infty, 0 \leq t < \infty [/itex]


Homework Equations



Let [itex] {\Phi} [/itex] denote the Laplace transform from t to s.

The Attempt at a Solution



Apply Laplace Transform to PDE:

[itex]

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

[/itex]

Apply Initial Conditions:

[itex]

\dfrac{\partial^2 \Phi }{ \partial x^2} - s^2\Phi + s + 1 - \dfrac{1}{s} = 0

[/itex]




[itex]

\dfrac{\partial^2 \Phi }{ \partial x^2} - s^2\Phi + \dfrac{s^2 + s - 1}{s} = 0

[/itex]


This leads to the eigenvalue being something like:

[itex]

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

[/itex]

which is always positive for both cases.

The solution in Laplace space should be something like:

[itex]

\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}

[/itex]

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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  • #2
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.
 
  • #3
mliuzzolino said:
[itex]

\dfrac{\partial^2 \Phi }{ \partial x^2} - s^2\Phi + \dfrac{s^2 + s - 1}{s} = 0

[/itex]This leads to the eigenvalue being something like:

[itex]

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

[/itex]

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?
 

What is the Laplace transform?

The Laplace transform is a mathematical tool used to solve differential equations. It transforms a function of time into a function of complex frequency, making it easier to solve certain types of equations.

How is the Laplace transform used to solve partial differential equations?

The Laplace transform can be applied to both sides of a partial differential equation, converting it into an algebraic equation. This algebraic equation can then be solved for the unknown function.

What are the advantages of using Laplace transform to solve partial differential equations?

The Laplace transform allows for the transformation of a differential equation into an algebraic equation, which can be easier to solve. It also allows for the solution of initial value problems and boundary value problems.

Are there any limitations to using Laplace transform to solve partial differential equations?

Yes, the Laplace transform method can only be applied to linear partial differential equations with constant coefficients. It also cannot be used to solve equations with discontinuous or non-smooth coefficients.

What is the inverse Laplace transform and how is it used in solving partial differential equations?

The inverse Laplace transform is used to transform a function in the frequency domain back to the time domain. It is used to obtain the solution to the original partial differential equation after it has been solved using the Laplace transform method.

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