Understanding Inverse Laplace Transforms with Initial Conditions

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The discussion focuses on solving a differential equation using the inverse Laplace transform with initial conditions. The user successfully applies the Laplace transform to the equation, incorporating the initial conditions to derive an expression for Y in the s-domain. However, confusion arises when attempting to compute the inverse Laplace transform, particularly with convolution integrals. Suggestions are made to consider alternative methods, such as using partial fractions instead of completing the square for simplification. Overall, the user seeks clarity on the convolution integrals and alternative approaches to the problem.
Knissp
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Homework Statement


y'' + 2y' + 2y = t^2 + 4t
y(0) = 0
y'(0) = -1

Homework Equations


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

The Attempt at a Solution



Take the Laplace transform of both sides.

L(y'' + 2y' + 2y) = L(t^2 + 4t)

By linearity:

L(y'') + 2L(y') + 2L(y) = L(t^2) + 4L(t)

Substitute:

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

Plug in initial conditions:

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

Solve for Y:

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

Y = \frac {\frac{2}{s^3} + \frac{4}{s^2} + 1}{s^2 + 2s + 2}

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

Rewrite:


Y = \frac{1}{s^2 + 2s + 2} (\frac{2}{s^3} + \frac{4}{s^2} + 1)

Distribute:

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}

Completing the square:

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}

Now to take the inverse Laplace transform of both sides:

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})

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)

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

L^{-1}(\frac{1}{(s+1)^2 + 1} \frac{2}{s^3})

= e^{-t}sin(t) * t^2

= \int_0^t (e^{-(t-v)}sin(t-v))(v^2)) dv

L^{-1}(\frac{1}{(s+1)^2 + 1} \frac{4}{s^2})[/tex<br /> <br /> = e^{-t}sin(t) * 4t<br /> <br /> = \int_0^t (e^{-(t-v)}sin(t-v))(4v) dv <br /> <br /> I don&#039;t know how to figure those convolution integrals. Any ideas? <br /> Alternatively, is there a better way to approach the problem?
 
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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.
 
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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