Dirac Delta Integration for Exponential Functions

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Jncik
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Homework Statement



find

[tex]\int_{-\infty}^{+\infty} x(t) \delta (\beta t - t_{0}) dt[/tex]

for [tex]x(t) = e^{a t} u(t)[/tex]

there is no information conserning a, β, or [tex]t_{0}[/tex]...

The Attempt at a Solution



assuming that [tex]t_{0}[/tex] is a constant[tex]\int_{-\infty}^{+\infty} x(t) \delta (\beta t - t_{0}) dt = <br /> \int_{-\infty}^{+\infty} e^{at}u(t) \delta (\beta t - t_{0}) dt <br /> = \int_{0}^{+\infty} e^{at} \delta (\beta t - t_{0}) dt <br /> = \int_{0}^{+\infty} e^{\frac{a}{b}t_{0}} dt<br /> = +\infty[/tex]
 
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thanks

hence the result is just

[tex]e^{\frac{a}{b}t_{0}}[/tex]

it would be 0 if we didn't integrate from 0 to infinity but from k>0 to infinity

correct?

edit: actually it would not be 0 if the integration was from k>t0/β
 
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you've got the right idea on the k>t0/b stuff, but i think you need to be careful with the scaling properties of the delta function

[tex]\int f(t) \delta (\beta t-t_0) dt[/tex]

now try making the substitution
[tex]u = \beta t-t_0[/tex]
 
[tex]u = \beta t - t_{0} => du = \beta dt [/tex]

also

[tex]t = \frac{u + t_{0}}{\beta}[/tex]

hence

[tex]\int_{-t_{0}}^{+\infty} f(\frac{u+t_{0}}{\beta}) \delta(u) \frac{du}{\beta}[/tex]

which will give us

[tex]\frac{1}{\beta} f(\frac{t_{0}}{\beta}) = \frac{e^{\frac{a t_{0}}{\beta}}}{\beta}[/tex] [tex]t_{0}>0[/tex]

:S, seems complicated... is this correct? In my previous attempt I forgot to change the variables.. I thought that we just had to search when the function inside [tex]\delta[/tex] is 0, and we just put the [tex]t[/tex] for which δ is 0, in the function before δ..
 
that looks good to me - you could do it either way if you remember the scaling & translation properties of the delta function.

Whilst slightly longer I prefer the substitution as you don't need to remember any rules, and we got that extra factor of 1/beta correct without needing to remember it.
 
yes you're right, thanks for your help :)