Dirac Delta Integration for Exponential Functions

In summary, the integral for x(t) = e^{a t} u(t) with no given information for a, β, or t_{0} is equal to e^{\frac{a}{β}t_{0}} when integrating from 0 to +∞. This is due to the properties of shifting and translating the delta function, and can also be found by making a substitution and using the scaling properties of the delta function.
  • #1
Jncik
103
0

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 =
\int_{-\infty}^{+\infty} e^{at}u(t) \delta (\beta t - t_{0}) dt
= \int_{0}^{+\infty} e^{at} \delta (\beta t - t_{0}) dt
= \int_{0}^{+\infty} e^{\frac{a}{b}t_{0}} dt
= +\infty
[/tex]
 
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  • #2
when you integrate, the delta function is only non-zero at [itex] t_0 [/itex] and
[tex] \int f(t) \delta (t-t_0) = f(t_0)[/tex]
 
  • #4
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
 
Last edited:
  • #5
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]
 
  • #6
[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..
 
  • #7
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.
 
  • #8
yes you're right, thanks for your help :)
 
  • #9
no worries;)
 

What is Dirac delta integration?

Dirac delta integration is a mathematical concept used to describe the behavior of the Dirac delta function. This function is also known as the unit impulse function and is typically represented by the symbol δ (delta). It is used to model a point-like source of energy or mass in physics and engineering problems.

What is the purpose of Dirac delta integration?

The purpose of Dirac delta integration is to allow for the integration of the Dirac delta function, which is not a typical function in the traditional sense. It is defined as zero everywhere except at the origin, where it is infinite. By using Dirac delta integration, we can solve problems that involve point-like sources or distributions of energy or mass.

How is Dirac delta integration used in physics?

In physics, Dirac delta integration is used to model point-like sources of energy or mass, such as a point charge in electromagnetism or a point mass in classical mechanics. It is also commonly used in quantum mechanics to represent quantum states and operators.

What is the relationship between the Dirac delta function and the Heaviside step function?

The Dirac delta function can be thought of as the derivative of the Heaviside step function. The Heaviside step function is defined as 0 for negative values and 1 for positive values. When the derivative of this function is taken, it results in the Dirac delta function. This relationship is often used in Dirac delta integration to simplify equations and solve problems.

What are the limitations of using Dirac delta integration?

One limitation of using Dirac delta integration is that it is not a typical function and does not follow the same rules of integration as other functions. This can make it difficult to work with and understand for those who are not familiar with it. Another limitation is that it is an idealized mathematical concept and does not always accurately represent the real world. Therefore, it should be used with caution and in conjunction with other methods when solving physical problems.

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