Understanding Inverse Laplace Transforms with Initial Conditions

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SUMMARY

The discussion focuses on solving the differential equation y'' + 2y' + 2y = t^2 + 4t using the Laplace transform method with initial conditions y(0) = 0 and y'(0) = -1. The solution process involves taking the Laplace transform of both sides, substituting initial conditions, and solving for Y in the frequency domain. The user expresses confusion regarding the inverse Laplace transform, particularly with convolution integrals, and seeks alternative methods such as partial fractions for simplification.

PREREQUISITES
  • Understanding of Laplace transforms and their properties
  • Familiarity with differential equations and initial value problems
  • Knowledge of convolution integrals in the context of inverse Laplace transforms
  • Experience with completing the square and partial fraction decomposition
NEXT STEPS
  • Study the properties of Laplace transforms, specifically linearity and initial conditions
  • Learn how to perform convolution integrals for inverse Laplace transforms
  • Explore partial fraction decomposition techniques for simplifying rational functions
  • Review examples of solving second-order differential equations using Laplace transforms
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Students and professionals in mathematics, engineering, or physics who are working with differential equations and Laplace transforms, particularly those seeking to deepen their understanding of inverse transforms and convolution techniques.

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Homework Statement


[tex]y'' + 2y' + 2y = t^2 + 4t[/tex]
[tex]y(0) = 0[/tex]
[tex]y'(0) = -1[/tex]

Homework Equations


[tex]L(y) = Y[/tex]
[tex]L(y') = sY - y(0)[/tex]
[tex]L(y'') = s^2 Y - s y(0) - y'(0)[/tex]
[tex]L(t^n) = \frac {n!}{s^{n+1}}[/tex]
[tex]L(a*b) = AB[/tex]
[tex]a*b = L^{-1}(AB)[/tex]

The Attempt at a Solution



Take the Laplace transform of both sides.

[tex]L(y'' + 2y' + 2y) = L(t^2 + 4t)[/tex]

By linearity:

[tex]L(y'') + 2L(y') + 2L(y) = L(t^2) + 4L(t)[/tex]

Substitute:

[tex](s^2 Y - s y(0) - y'(0)) + 2(sY - y(0)) + 2Y = \frac{2}{s^3} + \frac{4}{s^2}[/tex]

Plug in initial conditions:

[tex](s^2 Y + 1) + 2(sY) + 2Y = \frac{2}{s^3} + \frac{4}{s^2}[/tex]

Solve for Y:

[tex]Y (s^2 + 2s + 2) -1 = \frac{2}{s^3} + \frac{4}{s^2}[/tex]

[tex]Y = \frac {\frac{2}{s^3} + \frac{4}{s^2} + 1}{s^2 + 2s + 2}[/tex]

Now I must take the inverse Laplace transform. This is where I get confused.

Rewrite:


[tex]Y = \frac{1}{s^2 + 2s + 2} (\frac{2}{s^3} + \frac{4}{s^2} + 1)[/tex]

Distribute:

[tex]Y = \frac{1}{s^2 + 2s + 2} \frac{2}{s^3} + \frac{1}{s^2 + 2s + 2} \frac{4}{s^2} + \frac{1}{s^2 + 2s + 2}[/tex]

Completing the square:

[tex]Y = \frac{1}{(s+1)^2 + 1} \frac{2}{s^3} + \frac{1}{(s+1)^2 + 1} \frac{4}{s^2} + \frac{1}{(s+1)^2 + 1}[/tex]

Now to take the inverse Laplace transform of both sides:

[tex]y = L^{-1}(\frac{1}{(s+1)^2 + 1} \frac{2}{s^3}) + L^{-1}(\frac{1}{(s+1)^2 + 1} \frac{4}{s^2}) + L^{-1}(\frac{1}{(s+1)^2 + 1})[/tex]

[tex]y = L^{-1}(\frac{1}{(s+1)^2 + 1} \frac{2}{s^3}) + L^{-1}(\frac{1}{(s+1)^2 + 1} \frac{4}{s^2}) + e^{-t}sin(t)[/tex]

So now I need to do the separate inverse transforms (via convolutions):

[tex]L^{-1}(\frac{1}{(s+1)^2 + 1} \frac{2}{s^3})[/tex]

[tex]= e^{-t}sin(t) * t^2[/tex]

[tex]= \int_0^t (e^{-(t-v)}sin(t-v))(v^2)) dv[/tex]

[tex]L^{-1}(\frac{1}{(s+1)^2 + 1} \frac{4}{s^2})[/tex<br /> <br /> [tex]= e^{-t}sin(t) * 4t[/tex]<br /> <br /> [tex]= \int_0^t (e^{-(t-v)}sin(t-v))(4v) dv[/tex] <br /> <br /> I don't know how to figure those convolution integrals. Any ideas? <br /> Alternatively, is there a better way to approach the problem?[/tex]
 
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Perhaps you might have better luck using partial fractions, instead of completing the square... I don't know for sure since I didn't do it, but it's a suggestion you might want to look into.
 

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