Use the Laplace Transform to solve the "integral equation" y'(t)=sin(t)+the integral (from 0 to t) y(t-u)cos(u)du with y(0)=0
Use the convolution theorem for the transform of the integral. \[y'(t)=\sin t+\int_0^t (t-u)\cos u~du\] where you would have \[\mathcal{L}\left\{\int_0^t f(t-u)g(u)~du\right\}=\mathcal{L}\{f(t)\}\times\mathcal{L}\{g(t)\}\]
In this case, \(f(t-u)=t-u\) and \(g(u)=\cos u\), so you would have \[\mathcal{L}\left\{\int_0^t (t-u)\cos u~du\right\}=\mathcal{L}\{t\}\times\mathcal{L}\{\cos t\}\]
there is a y under the integral too. will that change the process?
Sorry, must have missed it. The question is \[y'(t)=\sin t+\int_0^t y(t-u)\cos u~du\] right? In this case, you can still use the convolution theorem, but set \(f(t-u)=y(t-u)\) (assuming that's written to mean \(y\) as a function of \(t-u\), and not the function \(y(t)\) times \(t-u\)), so you have \[\begin{align*} \mathcal{L}\left\{y'(t)\right\}&=\mathcal{L}\left\{\sin t\right\}+\mathcal{L}\left\{\int_0^t y(t-u)\cos u~du\right\}\\\\ s\mathcal{L}\left\{y(t)\right\}-y(0)&=\mathcal{L}\left\{\sin t\right\}+\mathcal{L}\left\{y(t)\right\}\mathcal{L}\left\{\cos t\right\}\\\\ \mathcal{L}\left\{y(t)\right\}\left(s-\mathcal{L}\left\{\cos t\right\}\right)&=\mathcal{L}\left\{\sin t\right\} \end{align*}\]
ok i follow you. but this doesn't solve it does it? you would have the laplace of sin(t) divided by (s-laplace cos(t)).....that gives the laplace of y?
Right, you have to take the transforms of the sine and cosine, and you have an equaiton of the form \(\mathcal{L}\{y\}=\cdots\), then you'd solve for \(y\) by taking the inverse transform, \(\mathcal{L}^{-1}\left\{\mathcal{L}\{y\}\right\}=y=\mathcal{L}^{-1}\{\cdots\}\).
so I have L(y)= 1/s^3......so to take the inverse laplace transform of each side my final answer would be y=...something. wolfram showed me that the inverse laplace transform of 1/s^3 is t^2/2, but I have no idea how to actually find that. Can you show me how they got that answer?
wait, i am watching a khan academy video and I think since t^n=n!/s^n+1
It comes from the fact that \[\mathcal{L}\{t^n\}=\frac{n!}{s^{n+1}}\]
then 1/s^3 is the same as 2!/2s^2+1
which gives t^2/2 as the original function?
Yes
YESSSSSSS. so wait, is this all I have to do? I'm done?
Yes that's it :) The nice thing about solving ODES with initial conditions and the Laplace transform is no pesky \(C\)s to deal with.
So seriously I am done with this problem? That seemed so simple now that you showed the steps. What the heck lol! Thanks so much
Yes, you're done! You're welcome!
Would you be able to help me with something else really quick? It's another laplace transform. All i have to do is find the laplace transform of (1-e^-t)/t but this one isn't as nice as the last one in my opinion.
Wolfram says the laplace transform of that is ln(1+(1/s)) but I cannot figure out how they got it
Sure. For this one, you'll use the formula \[\mathcal{L}\left\{\frac{1}{t}f(t)\right\}=\int_s^\infty F(u)~du\] where \(F(u)=\mathcal{L}\{f(t)\}\). In this case, \(f(t)=1-e^{-t}\), so the transform would be \[\mathcal{L}\left\{\frac{1}{t}(1-e^{-t})\right\}=\int_s^\infty \mathcal{L}_s\{1-e^{-t}\}~du\] (The subscript on the Laplace operator is meant to denote that we're transforming from the \(t\) domain to \(s\).
Also, the formula was taken from this neat resource here: http://tutorial.math.lamar.edu/pdf/Laplace_Table.pdf
Slight correction, that subscript should be a \(u\), not an \(s\).
sweet! I think my problem is the 1-e^-t. if it was just the e part the it would just be 1/s+1 but thats not correct is it
\[\mathcal{L}\left\{1-e^{-t}\right\}=\mathcal{L}\{1\}-\mathcal{L}\{e^{-t}\}=\frac{1}{s}-\frac{1}{s+1}\]
which when integrated becomes..... ln(u)-ln(u+1) from s to infinity?
Right.
Hmm that integral doesn't seem to converge...
so...do I take the limit of that then?
yeah something's not right
I have a class in 15 min, but I'll get back to this when I have a chance. (unless someone else can clear up the issue here)
thank you so much! I will wait for your help, you have helped so much in the past!!!
Alright, it doesn't look like we did anything wrong. I must have been thinking too far ahead of my actual computation. You have \[y=\int_s^\infty\left(\frac{1}{u}-\frac{1}{u+1}\right)~du\] Like you mentioned, we'll need to consider the limit: \[y=\lim_{t\to\infty}\int_s^t\left(\frac{1}{u}-\frac{1}{u+1}\right)~du\] which gives \[y=\lim_{t\to\infty}\bigg[\ln u-\ln (u+1)\bigg]_s^t\] By the FTC we get \[y=\lim_{t\to\infty}\bigg[\ln t-\ln (t+1)\bigg]-\ln s+\ln(s+1)=\ln\frac{s+1}{s}\] as desired.
this looks great! thanks so much!!!! but what is the FTC?
Fundamental theorem of calc, the one that says if \(F(x)\) is the antiderivative of \(f(x)\), then \[\int_a^b f(x)~dx=F(b)-F(a)\]
Join our real-time social learning platform and learn together with your friends!