Dirac Delta Function (Unit Impulse Function)

The Dirac delta function (also called distribution) is used to model a point source or point charge in electrical engineering, physics, and other fields.

It is a a signal that is infinitesimally short in time but has infinite magnitude.

Formally learned in MATH213.

Dirac Delta Function \delta(x)

with

Some notes:

  • not a true function, but rather a “generalized function” or “distribution.”
  • Often used in mathematical modeling to represent a point of discontinuity or singularity in a system.
    • It is also used in the theory of Fourier Transform, where it serves as the kernel for the continuous-time Fourier transform

Laplace Transform of Unit Impulse Function

The Laplace Transform of the unit impulse function is 1:

  • I don’t think the prof proved this, a proof is here

Actually, the prof used this property to prove it

Theorem 1

If is a “well-behaved” function defined at then

\int_{-\infty}^\infty f(\tau) \delta(t - \tau) d\tau & = \int_{-\infty}^\infty f(t) \delta(t - \tau)d\tau \ & = f(t) \int_{-\infty}^\infty \delta(t - \tau) d\tau \ &= f(t) \ \end{align}$$

Apparently used in the Particle Filter and Optimal Transport problem from here.

This thing is very very useful, because if you want to figure out the transfer function of a system, you can simply use the Unit Impulse Function!