Signals & systems

Laplace transform

The Laplace transform is the Fourier transform's more powerful cousin: it turns differential equations — the hard calculus that describes circuits, mechanics, and control loops — into ordinary algebra you can solve by hand. Instead of testing a system only with steady sine waves (frequency jω), it tests it with sinusoids that also grow or decay, captured by a complex frequency s = σ + jω. Engineers reach for it the way a carpenter reaches for a power tool: the same job, far less sweat.

Its superpower is that calculus operations become arithmetic in the s-domain: differentiation becomes multiplying by s, integration becomes dividing by s, and an initial-condition messy ODE for an RLC circuit collapses into a tidy algebraic fraction. Solve the algebra, then transform back. This is why control engineers describe systems by their transfer function H(s) and study the locations of its poles and zeros in the complex s-plane — those locations instantly tell you whether the system is stable, fast, or prone to ringing.

X(s) = ∫₀^∞ x(t)·e^(−s·t) dt, with s = σ + jω

Set σ = 0 (so s = jω) and the Laplace transform reduces to the Fourier transform — Fourier lives on the imaginary axis of the s-plane. The discrete-time analogue used in DSP is the z-transform.

Also called
拉氏變換s-domain