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OpenStudy (anonymous):
L{sin2t*sin2t}
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OpenStudy (lgbasallote):
wouldn't that be \[\mathcal L \{ \sin^2 (2t) \}\]
??
hartnn (hartnn):
does * here denote convolution?
OpenStudy (lgbasallote):
i thought that was multiplication lol
OpenStudy (anonymous):
solution plz
OpenStudy (cwrw238):
thats a Laplace transform right?
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hartnn (hartnn):
u know L(sin2t) ?
hartnn (hartnn):
if u know it,L{sin 2t * sin 2t} is just L(sin2t).L(sin2t). ok?
OpenStudy (zzr0ck3r):
im guessig its convolution
hartnn (hartnn):
and L(sin 2t)=2/(s^2+4)
so whats the final answer?
hartnn (hartnn):
its convolution thats why i can separate into two laplace transforms........
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OpenStudy (zzr0ck3r):
yeah just saw that
OpenStudy (anonymous):
\[\mathcal L \{ \sin^2 (2t) \}=\frac{1}{2}\mathcal L \{ 1-\cos (4t) \}=\frac{1}{2}(\frac{1}{s}-\frac{s}{s^2+16})=\frac{8}{s(s^2+16)}\]
OpenStudy (anonymous):
\[\begin{equation} \mbox{L}\left\{ f_{1} (t) \, f_{2} (t) \right\} = \frac{1}{2 \pi {\rm j}} \int\limits\limits^{c + {\rm j}\infty}_{c - {\rm j}\infty} F_{1} (p) \, F_{2} (s - p) \, {\rm d}p\ . \end{equation}\]
hartnn (hartnn):
its convolution in time domain
OpenStudy (anonymous):
Ah - OK then the dual of this is the more known case.
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