Understanding Inverse Laplace Transforms with Initial Conditions

In summary, the problem involves finding the inverse Laplace transform of an equation with initial conditions. The solution involves taking the Laplace transform of both sides, using linearity to substitute, plugging in initial conditions, solving for Y, and taking the inverse Laplace transform of both sides. The final solution involves using convolution integrals, but there may be alternative methods such as using partial fractions.
  • #1
Knissp
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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

[tex]= e^{-t}sin(t) * 4t [/tex]

[tex]= \int_0^t (e^{-(t-v)}sin(t-v))(4v) dv [/tex]

I don't know how to figure those convolution integrals. Any ideas?
Alternatively, is there a better way to approach the problem?
 
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  • #2
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.
 

FAQ: Understanding Inverse Laplace Transforms with Initial Conditions

What is a Laplace Transform?

A Laplace transform is a mathematical operation that converts a function of time into a function of a complex variable known as the Laplace variable. It is commonly used in engineering and physics to solve differential equations.

What is an Inverse Laplace Transform?

An inverse Laplace transform is the mathematical operation that converts a function of the Laplace variable back into a function of time. It is the reverse of the Laplace transform and is used to find the original function from its Laplace transform.

How is a Laplace Transform represented mathematically?

The Laplace transform of a function f(t) is denoted as F(s) and is defined by the integral F(s) = ∫f(t)e^(-st)dt, where s is the Laplace variable and e is the mathematical constant.

What are the applications of Laplace Transforms?

Laplace transforms have various applications in engineering and physics, including solving differential equations, analyzing control systems, and studying the behavior of electrical circuits and mechanical systems.

What are the properties of Laplace Transforms?

Some common properties of Laplace transforms include linearity, time-shifting, differentiation, integration, and convolution. These properties make it easier to solve complex problems involving Laplace transforms.

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