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Math Exercises

Delta function intuition

To understand why the delta function under an integral picks out a particular value of the integrand, it may help to think of it as the limit of a sequence of steps.

Let δ(t)\delta(t) be the Dirac delta function. We can approximate it with a sequence of rectangular pulses δn(t)\delta_n(t):

δn(t)={hn,twn20,t>wn2 \delta_n(t) = \begin{cases} h_n, & |t| \le \frac{w_n}{2} \\ 0, & |t| > \frac{w_n}{2} \end{cases}

Each pulse has area 1: δn(t)dt=hnwn=1\int_{-\infty}^{\infty} \delta_n(t) \, dt = h_n w_n = 1

In the limit, the delta function is obtained as: δ(t)=limnδn(t),wn0,hn\delta(t) = \lim_{n \to \infty} \delta_n(t), \quad w_n \to 0, \quad h_n \to \infty

The key property under an integral is: f(t)δ(ta)dt=f(a)\int_{-\infty}^{\infty} f(t) \, \delta(t-a) \, dt = f(a) where f(t)f(t) is any continuous function.

Each δn(ta)\delta_n(t-a) is a pulse centered at t=at=a, so in the limit, the integral “picks out” f(a)f(a). See a visual below

Approximation of delta function by narrowing rectangular pulses