Elementary Signals
Sweep the upper limit and build the step
The narrow pulse in the middle is an impulse approximated by area 1. Slide the upper limit t to the right: area under the pulse accumulates, and that running value climbs onto the faint target step.
The impulse is a single point of area 1
The impulse δ(t) is the limit of a pulse whose width shrinks to 0 and height grows without bound while the area is pinned at 1. So it is defined by its area, not its value. Multiplied by another signal and integrated, it sifts out that signal’s value at a single point (the sifting property).
The step is the running integral of the impulse
The unit step u(t) is 0 for t < 0 and 1 for t ≥ 0. This is exactly the impulse integrated from the left up to t. Conversely, differentiating the step gives an impulse that spikes only at the jump. Integration and differentiation bind the two into one pair.
The exponential rate is itself
The exponential eᵃᵗ has a derivative equal to a times itself. So the sign of a decides its fate: a > 0 blows up, a < 0 decays toward 0, and a = 0 is constant. A system’s natural response always shows up in this shape.
Back to the first screen
The accumulated area the slider swept up was the step itself. While the limit crossed the impulse, the area filled from 0 to 1 and drew the step’s jump; once past, it locked at 1. The impulse and the step are one pair joined by a single integration, and the exponential is the third letter whose rate is itself. These three become the bricks for every signal ahead.
The impulse is the lead of the next chapter. The impulse response is the output when a single impulse enters a system, and from there convolution opens the way to compute the output of any input from that response. The exponential becomes the test signal that cracks systems in Laplace and Fourier. The next unit, operations on a signal, is about shifting and stretching a signal along the time axis.