Laplace {sint unit step (t-pi/2)}
By the definition of the transform,\[\mathscr{L}\left\{\sin t~u\left(t-\frac{\pi}{2}\right)\right\}=\int_0^\infty \sin t~u\left(t-\frac{\pi}{2}\right)e^{-st}~dt\] By definition of the unit step function, \[u\left(t-\frac{\pi}{2}\right)=\begin{cases}1&\text{for }t<\frac{\pi}{2}\\ \\ 0&\text{for }t\ge\frac{\pi}{2} \end{cases}\] So, the integral is \[\begin{align*}\int_0^\infty \sin t~u\left(t-\frac{\pi}{2}\right)e^{-st}~dt &=\int_0^{\pi/2} \sin t~u\left(t-\frac{\pi}{2}\right)e^{-st}~dt\\ &~~~~~~~+\int_{\pi/2}^\infty \sin t~u\left(t-\frac{\pi}{2}\right)e^{-st}~dt\\ &=\int_0^{\pi/2} \sin t~(0)e^{-st}~dt+\int_{\pi/2}^\infty \sin t~(1)e^{-st}~dt\\ &=\int_{\pi/2}^\infty \sin t~e^{-st}~dt \end{align*}\] Integrate by parts!
but it will be better with the form {f(t-a) U (t-a)}
sorry
What I got is \[(\frac{ 1 }{ s^2+1 }+\frac{ 1 }{ s })e^{-\frac{ pis }{ 2 }}\]
is that correct?
Just a moment, I'm writing it out on paper to check.
Okay, so I've finally got the answer. Your answer isn't correct. The \(\dfrac{1}{s}\) shouldn't be there. You should have \[e^{\frac{\pi}{2}s}\frac{s}{s^2+1}\] Notice that \(\dfrac{s}{s^2+1}\) is the transform of \(\cos t\). But, \(\sin\left(t-\dfrac{\pi}{2}\right)=\cos t\).
Thank you!!! But... I do not understand why (t−π 2 )=cost
I mean... you don't distribute t and π/2???
This is what i did:
This is what i did:\[a=\frac{ \pi }{ 2 }\] and \[f(t-a)=sint\]
This is what i did:\[a=\frac{ \pi }{ 2 }\] and \[f(t-a)=sint\] \[f(t)=\sin (t+a)\]
\[f(t)=sint + \sin \frac{ \pi }{ 2 }\]
\[f(t)= sint+1\]\[f(t)=sint + \sin \frac{ \pi }{ 2 }\]
Sorry, just split the last two answers I continue:
\[F(s)=\frac{ 1 }{ s^2+1 }+\frac{ 1 }{ s }\] Shall you please explain me what is wrong in my procedure??? In the other hand, I have another transformation: Laplace {(Cos2t) U (t-pi)} and my answer is \[(\frac{ s }{ s^2+4 }+\frac{ 1 }{ s })\[e^{-\pi s}\] I did it with the same procedure I explained you before. Following your answer, I guess de 1/s is wronsg, but.... why??? You´re a master for this, do you mind to help me with some other transformations??? I understand most of this calculus, but saddly these last technics are not so clear for me. Yesterday, I was trying to solve Laplace ^-1 \[{\frac{ (1+e^{-2s})^{2}} }{ s+2 }\] or {(1+e^-2s)^2}/(s+2) And honestly, I do not know either how to begin. Excuse me for annoying you with this but it seems you are the only one can help me. My apologies for my English, I´m from Colombia...
The problem is that \[\sin(a+b)\not=\sin(a)+\sin(b)\] (Distribution doesn't work.) However, \[\sin(a\pm b)=\sin(a)\cos(b)\pm\cos(b)\sin(a)\] So, \[\begin{align*}\sin\left(t\pm\frac{\pi}{2}\right)&=\sin(t)\cos\left(\frac{\pi}{2}\right)+\cos(t)\sin\left(\frac{\pi}{2}\right)\\ &=0+\cos(t)\\ &=\cos t \end{align*}\]
And now your next question is \[\mathscr{L}^{-1}\left\{\frac{1+e^{-2s}}{s+2}\right\}\] First, break up the fraction so you have \[\mathscr{L}^{-1}\left\{\frac{1}{s+2}+\frac{e^{-2s}}{s+2}\right\}\] The normal and inverse transform operators are linear, which means that \(\mathscr{L}^{-1}\left\{f(t)+g(t)\right\}=\mathscr{L}^{-1}\left\{f(t)\right\}+\mathscr{L}^{-1}\left\{g(t)\right\}\) So you then have \[\mathscr{L}^{-1}\left\{\frac{1}{s+2}\right\}+\mathscr{L}^{-1}\left\{\frac{e^{-2s}}{s+2}\right\}\] The first term should be fairly simple: \(e^{-2t}\). The second is somewhat different; it's the product of an exponential function and the transform of \(e^{-2t}\). When you're given a transform of the form \(e^{-cs}F(s)\), its inverse transform would be \(u(t-c)f(t-c)\). Here, \(c=-2\) and \(f(t)=e^{-2t}\), so \(f(t-c)=e^{-2(t-2)}\). So, \[\mathscr{L}^{-1}\left\{\frac{e^{-2s}}{s+2}\right\}=e^{-2(t-2)} u(t-2)\] And don't worry about bothering - happy to help.
Join our real-time social learning platform and learn together with your friends!