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OpenStudy (anonymous):
Laplace of the following:
L { t ∗ 4δ (t-1) ∗ u(t-2) }
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OpenStudy (anonymous):
I know how to do it for 2 functions, but am not sure how to go about it for 3
OpenStudy (zzr0ck3r):
why not the definition?
OpenStudy (zzr0ck3r):
hmm I forget how to do this, that is the dirac and heaviside functions?
OpenStudy (anonymous):
yeah they are the dirac and heaviside.
Can I write\[ L{f(t)*g(t)*h(t)} = F(s)G(s)H(s)\]
OpenStudy (zzr0ck3r):
well from - infinity to 2 its going to be 0 right?
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OpenStudy (zzr0ck3r):
hmm undeifined at 1
OpenStudy (anonymous):
I guess so...I don't understand the heaviside or dirac function so well, Sort of just follow the formula
OpenStudy (zzr0ck3r):
heaviside u(t-a) is 0 below (a) and 1 above and dirac(t-b) is infinite at b but the area under the graph is always one
OpenStudy (zzr0ck3r):
so i think since its 0 up untill 2 and the dirac will be area 1 at 1 all we have to look at is
int(4t*e^9-st) from 2 to infinity
OpenStudy (zzr0ck3r):
hmm maybe not, I have to go to a party man, sorry I cant help more. good luck
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OpenStudy (anonymous):
np, thanks for trying anyway
OpenStudy (anonymous):
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