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Mathematics 8 Online
OpenStudy (astrophysics):

@ganeshie8

OpenStudy (astrophysics):

Ooh it shows college...anyways wanna do a fun convolution integral problem

OpenStudy (astrophysics):

\[\phi'(t) = 1/2 \int\limits_{0}^{t} (t- \xi)^2 \phi(\xi) = -t , \phi(0)=1\]

OpenStudy (astrophysics):

So solve the integro differential using laplace and then I think the funner part is by differentiating the integro diff equations a sufficient amount of times convert it into a ivp and then verify the solution as it should be the same as the first one

ganeshie8 (ganeshie8):

I have no clue what these are, could you teach me some pretending that il pick up fast :)

OpenStudy (astrophysics):

Oh that should be - after the phi'

OpenStudy (astrophysics):

Ah yeah..you know the convolution integral right

OpenStudy (astrophysics):

I don't know too much about all the symbols haha but I thought this problem was fun, but this is called the integro - differential equations where both derivatives and integrals of a known function appear

ganeshie8 (ganeshie8):

\[f*g = \int\limits_{0}^{t} f(u)g(t-u)\,du\] ?

OpenStudy (astrophysics):

Right that's the convolution integral

ganeshie8 (ganeshie8):

thats the only convolution i remember from ODE

OpenStudy (astrophysics):

\[\phi'(t) - 1/2 \int\limits\limits_{0}^{t} (t- \xi)^2 \phi(\xi) = -t , \phi(0)=1\] fixed

OpenStudy (astrophysics):

Yeah haha the theory in DE's is pretty difficult I think

ganeshie8 (ganeshie8):

you want to differentiate both sides with respect to \(t\) is it ?

OpenStudy (astrophysics):

d/dt yup

ganeshie8 (ganeshie8):

that might give us a nice form for the right hand side to use convolution

ganeshie8 (ganeshie8):

\[t^2*\phi=\int\limits\limits_{0}^{t} (t- \xi)^2 \phi(\xi) d\xi \] ?

OpenStudy (astrophysics):

Looks good

ganeshie8 (ganeshie8):

how do you differentiate a convolution ?

OpenStudy (astrophysics):

Same way as everything else \[\phi ''(t) - 1/2 \int\limits_{0}^{t} 2(t- \xi) \phi(\xi) d \xi = -1\] taking the derivative respect to t

ganeshie8 (ganeshie8):

why are we allowed to swap the derivative and integral ?

ganeshie8 (ganeshie8):

FTC tells me \[\dfrac{d}{d\color{red}{t}} \int\limits_0^{\color{red}{t}} f(\xi)\,d\xi = f(t)\]

OpenStudy (astrophysics):

Well we're really using the relation between laplace transform and convolution

ganeshie8 (ganeshie8):

\[F(s)G(s) = \mathcal{L(f*g)}\] that one ?

ganeshie8 (ganeshie8):

i don't see the connection..

OpenStudy (astrophysics):

It's because the integral is the convolution between f(t)=t^2 and phi(t)

ganeshie8 (ganeshie8):

right, that still doesn't explain how we can exchange derivative and integral

ganeshie8 (ganeshie8):

maybe lets just proceed assuming that swap is legitimate...

OpenStudy (astrophysics):

Haha, wait no I want to know, I was just doing the math not thinking about that

ganeshie8 (ganeshie8):

we can get back to that detail later... maybe in the end of this thread :) so do we have : \[\phi ''(t) - \int\limits_{0}^{t} (t- \xi) \phi(\xi) d \xi = -1\]

ganeshie8 (ganeshie8):

next you want to take laplace transform both sides is it ?

ganeshie8 (ganeshie8):

\[\phi ''(t) - t*\phi = -1\] taking laplace transform seems to be the most logical thing to do next

OpenStudy (astrophysics):

Oh ok I see you're going with taking the derivative first then laplace, I used laplace right away so I had \[\phi'(t) - 1/2 (t^2 \phi(t)) = t\] because of the ivp

OpenStudy (astrophysics):

Ok it shouldn't matter yeahhh

ganeshie8 (ganeshie8):

i don't want to take derivative first, i don't believe we can exchange derivative and integral...

ganeshie8 (ganeshie8):

lets go with ur equation may be : \[\phi'(t) - 1/2 (t^2* \phi(t)) = -t\]

OpenStudy (astrophysics):

yeah that looks a bit weird otherwise lol

OpenStudy (astrophysics):

I see it's part of this https://en.wikipedia.org/wiki/Volterra_integral_equation ok, keep going

ganeshie8 (ganeshie8):

\[s\Phi(s) - 1-1/2 \mathcal{L}(t^2)\mathcal{L}(\phi(t)) = -\mathcal{L}(t)\]

ganeshie8 (ganeshie8):

\[s\Phi(s) - 1- \dfrac{\mathcal{L}({\phi}(t))}{s^3} = -\dfrac{1}{s^2}\]

OpenStudy (astrophysics):

Looks good

ganeshie8 (ganeshie8):

i can isolate \(\Phi(s)\) but what next ?

OpenStudy (astrophysics):

wait a sec it should be

ganeshie8 (ganeshie8):

what to do with that \(\mathcal{L}(\phi(t))\) ?

OpenStudy (astrophysics):

\[s \Phi(s) - 1 - \frac{ \Phi(s) }{ s^3 }=-1/s^2\] right

ganeshie8 (ganeshie8):

right right

ganeshie8 (ganeshie8):

we can solve \(\phi(t)\) then

OpenStudy (astrophysics):

Yup

ganeshie8 (ganeshie8):

\(\Phi(s) = \dfrac{1}{s^2+1}\)

OpenStudy (astrophysics):

I got \[\frac{ s }{ s^2+1 }\]

ganeshie8 (ganeshie8):

\(\phi(t) = \sin t\)

OpenStudy (astrophysics):

I got cost xD

ganeshie8 (ganeshie8):

i may be wrong, im doing all my calculations in my unreliable head..

OpenStudy (astrophysics):

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

OpenStudy (astrophysics):

Yeah should work out to be cost

OpenStudy (astrophysics):

But w/e you got it

ganeshie8 (ganeshie8):

yeah phi = cost looks good to me

OpenStudy (astrophysics):

I actually spent the least amount of time on convolution but it seems pretty useful

OpenStudy (astrophysics):

Oh so we can do \[\frac{ d }{ dt } (\int\limits_{0}^{t} (t- \xi)\phi(\xi)d \xi )\] and apply the fundamental theorem of calc and product rule

ganeshie8 (ganeshie8):

to my knowledge \(\frac{ d }{ dt } (\int\limits_{0}^{t} (t- \xi)\phi(\xi)d \xi )\) is \(0\)

ganeshie8 (ganeshie8):

i may be off... could you elaborate a bit..

OpenStudy (astrophysics):

\[\frac{ d }{ dt } (\int\limits\limits_{0}^{t} (t- \xi)\phi(\xi)d \xi ) = \frac{ d }{ dt }(\int\limits_{0}^{t}t \phi(\xi)d \xi))-\frac{ d }{ dt }(\int\limits_{0}^{t}\xi \phi(\xi) d \xi))\]

OpenStudy (astrophysics):

Maybe I'm doing it wrong..

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