Transfer Functions
Wikipedia · Transfer function · CC BY-SA 4.0
The Laplace transform converts a differential equation into an algebraic one. The transfer function H(s) = Y(s)/U(s) captures the input-output relationship. Poles determine stability; zeros shape the response.
The Laplace domain
A linear time-invariant (LTI) system is described by a differential equation. The Laplace transform replaces derivatives with powers of the complex variable s. Differentiation becomes multiplication: if y(t) has transform Y(s), then y'(t) has transform sY(s). This turns calculus into algebra.
Poles and zeros
The transfer function is a ratio of polynomials in s. The roots of the numerator are zeros: frequencies where the output vanishes. The roots of the denominator are poles: frequencies where the output blows up. Poles in the left half-plane decay. Poles in the right half-plane grow. Poles on the imaginary axis oscillate forever.
Step response
Apply a unit step input (off to on at t=0) and watch the output. The step response reveals rise time, overshoot, settling time, and steady-state error. These four numbers summarize the system's behavior for most practical purposes.
First-order and second-order systems
A first-order system has one pole: H(s) = 1/(s + a). It rises exponentially with time constant 1/a. No overshoot. A second-order system has two poles: H(s) = wn^2/(s^2 + 2*zeta*wn*s + wn^2). The damping ratio zeta controls whether the response is overdamped (zeta greater than 1), critically damped (zeta = 1), or underdamped (zeta less than 1, the oscillating case).
Neighbors
Laplace transform — the mathematical tool behind transfer functions