Dirac Delta Integration for Exponential Functions

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Homework Help Overview

The discussion revolves around the integration of a function involving the Dirac delta function, specifically focusing on the integral of an exponential function multiplied by the delta function. The original poster presents a problem involving the integration of \( x(t) = e^{at} u(t) \) with respect to \( \delta(\beta t - t_0) \), noting the lack of specific values for parameters \( a \), \( \beta \), and \( t_0 \).

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the properties of the Dirac delta function, particularly its behavior during integration and the implications of shifting and scaling. There is an exploration of the conditions under which the integral evaluates to zero or a non-zero value, depending on the limits of integration and the parameters involved.

Discussion Status

The conversation includes various attempts to clarify the integration process and the implications of different parameter values. Some participants suggest using substitutions to simplify the integration, while others express uncertainty about the correctness of their approaches. There is an acknowledgment of the need to consider scaling properties of the delta function, indicating a productive exploration of the topic.

Contextual Notes

Participants note the absence of specific values for parameters \( a \), \( \beta \), and \( t_0 \), which may affect the outcome of the integration. The discussion also highlights the importance of the limits of integration, particularly when considering the behavior of the delta function.

Jncik
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Homework Statement



find

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

for x(t) = e^{a t} u(t)

there is no information conserning a, β, or t_{0}...

The Attempt at a Solution



assuming that t_{0} is a constant\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<br />
 
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when you integrate, the delta function is only non-zero at t_0 and
\int f(t) \delta (t-t_0) = f(t_0)
 
thanks

hence the result is just

e^{\frac{a}{b}t_{0}}

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
 
Last edited:
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

\int f(t) \delta (\beta t-t_0) dt

now try making the substitution
u = \beta t-t_0
 
u = \beta t - t_{0} =&gt; du = \beta dt <br />

also

t = \frac{u + t_{0}}{\beta}

hence

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

which will give us

\frac{1}{\beta} f(\frac{t_{0}}{\beta}) = \frac{e^{\frac{a t_{0}}{\beta}}}{\beta} t_{0}&gt;0

: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 \delta is 0, and we just put the t 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 :)
 
no worries;)
 

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