Solving Differential Equations with Laplace Transforms

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Discussion Overview

The discussion revolves around the application of Laplace transforms to solve a specific differential equation, \(\frac{dy}{dt} = e^{wt}y\). Participants explore the validity of using Laplace transforms for equations with non-constant coefficients and the implications of initial conditions on the solutions derived.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant introduces a differential equation and seeks to verify the effectiveness of the Laplace transform method.
  • Another participant argues that the Laplace transform is typically not applied to equations with non-constant coefficients, suggesting that the problem may not be suitable for this method.
  • A different participant asserts that the equation is linear and that the Laplace transform can be used, but expresses confusion over the implications of the derived functional equation for \(Y(s)\).
  • Some participants discuss the conditions under which the Laplace transform yields valid solutions, particularly noting that the initial condition \(y(0) = 0\) leads to \(Y(s) = 0\) for certain values of \(w\).
  • Concerns are raised regarding the existence of non-trivial solutions and the conditions under which the Laplace transform can be applied, particularly emphasizing that solutions may only exist for \(w < 0\).

Areas of Agreement / Disagreement

Participants do not reach a consensus on the applicability of the Laplace transform to the given differential equation. There are competing views on the conditions under which valid solutions can be derived, particularly regarding the values of \(w\) and the implications of initial conditions.

Contextual Notes

Limitations include the unclear applicability of the Laplace transform to equations with non-constant coefficients and the unresolved nature of the functional equation for \(Y(s)\). The discussion highlights the dependence on the behavior of solutions as influenced by the parameter \(w\).

KFC
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I am reading a text about Laplace transform in solving differential equations. Seems that this method is so powerful. To practice how it works, I makeup a very simple problem

[tex]\frac{dy}{dt} = e^{wt}y[/tex]

This equation could be solved by variable separation and then intergrate LHS and RHS. But I would like to check that Laplace transform works. Let's

[tex]Y = \mathcal{L}[y][/tex]

is the Laplace transform of y. Note that

[tex]\mathcal{L}[dy/dt] = sY(s) - y(0)[/tex]

and

[tex]\mathcal{L}[e^{wt}y] =Y(s-w)[/tex]

where s is the parameter for Laplace transform. Hence, in Laplace domain, above equation becomes

[tex]sY(s) = Y(s-w)[/tex]

(assuming y(0)=0) My question is : there is a shift in the variable s, so how to solve this equation to get Y?
 
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You don't. The problem with your simple example is that you chose a problem with a coefficient that is not constant, and the Laplace transform typically isn't applied to such problems.

Generally the Laplace transform is applied to linear ODEs with constant coefficients and a non-zero, time dependent right hand side. The Laplace transform is especially helpful when the RHS is discontinuous. For such problems you'll be able to solve for Y(s) and then do the inverse transform.

For your problem, you've gotten yourself a functional equation for Y(s), that I'm not sure how to solve. That doesn't mean it's not possible to solve it, but I'm not familiar with solving such problems.

Your relation almost looks like it's a Gamma function: recall the Gamma function has the functional relation

[tex]\Gamma(z+1) = z\Gamma(z)[/tex],

so for w = -1, [itex]Y(s) = \Gamma(s)[/itex] (this is apparently the unique solution, but I don't know how you'd show that). Of course, then you'd have to find the inverse laplace transform of a Gamma function, which usually isn't in the common tables!

So, generally, you wouldn't use the Laplace transform to solve that particular problem.
 
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[tex]\frac{dy}{dt} = e^{wt}y[/tex]


This DE is linear. It is perfectly alright to use Laplace transform method as long as you can solve the transformed equation.

The solution for [tex]sY(s) = Y(s-w)[/tex] is Y(s)=0 :biggrin:

But this seem to contradict the solution given by Mute if w=-1.
So in order that to be able to solve [tex]\frac{dy}{dt} = e^{wt}y[/tex]
using Laplace transform, I suspect w must be negative and less than -1.

But the original equation can be solve for all value of w :confused:
 
Thanks for reply. Follow your reply, I still have some questions. First of all, we know that y(t=0) is the initial condition, but in what reason to make Y(s)=0?

matematikawan said:
[tex]\frac{dy}{dt} = e^{wt}y[/tex]


This DE is linear. It is perfectly alright to use Laplace transform method as long as you can solve the transformed equation.

The solution for [tex]sY(s) = Y(s-w)[/tex] is Y(s)=0 :biggrin:

But this seem to contradict the solution given by Mute if w=-1.
So in order that to be able to solve [tex]\frac{dy}{dt} = e^{wt}y[/tex]
using Laplace transform, I suspect w must be negative and less than -1.

But the original equation can be solve for all value of w :confused:
 
KFC said:
Thanks for reply. Follow your reply, I still have some questions. First of all, we know that y(t=0) is the initial condition, but in what reason to make Y(s)=0?

The reason, which I didn't notice before, is that if you solve your original equation, you find

[tex]\ln |y(t)| = \frac{e^{wt}}{w} + C \Rightarrow y(t) = A\exp\left[\frac{e^{wt}}{w}\right][/tex]

The initial condition y(0) = 0 is satisfied only for A = 0, which means y(t) = 0 for all t, and the laplace transform of zero is zero.

So, for w = -1 the gamma function solution for Y(s) seems to be erroneous, since Y(s) should be zero...

Of course, the trivial solution, Y(s) = 0 for all s also satisfies that relation, so I guess it's probably just the case that although the functional equation has non-trivial solutions, it's the trivial solution that needs to be picked to solve the ODE in this case. (I suppose it could also be the case that the inverse laplace transform of the non-trivial solution for Y(s) is zero, but that seems unlikely; they can't be analytic everywhere, as the Gamma function certainly isn't and we don't get a different solution for y(t) if w = -1).

Edit: Hm, maybe this is part of what's going on: in the other Laplace transform thread, Bobbybear mentioned that in order for something to be Laplace transformable, y(t) and its derivative cannot grow faster than the Laplace transform kernal, [itex]\exp[-st][/itex], which as you can see, the nonzero solutions of this ODE don't! An exponential to an exponential grows way too fast for the Laplace transform to yield a finite result, unless w < 0, in which case the solution itself decays to zero as t -> infinity. (there could be other conditions on w, like matematikawan predicts, but that doesn't come out of this basic analysis)

So, part of the problem here is that the Laplace transform of y(t) only exists for w < 0. This still doesn't tell us how to pick which solution to the functional equation to use - though I suspect there is only the trivial solution and then a unique solution, so perhaps it's just a matter of checking if the inverse transform of the nontrivial solution satisfies the given initial conditions.
 
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