notes/uni/mmme/2xxx/2046_dynamics_and_control/control.md

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2023-01-30 20:36:47 +00:00
---
author: Akbar Rahman
date: \today
title: MMME2046 // Control
tags: [ mmme2046, uon, uni, control ]
uuid:
---
# System and Block Diagrams
# Laplace Transform
$$F(s) = \mathscr L {F(t)} = \int^\infty_0 f(t)e^{-st} \mathrm{d}t$$
where $s = \alpha + j\omega$
The function $F(s)$ is often much easier to manipulate than periodic function $f(t)$.
## Final Value Theorem
As $f(t)$ tends to infinity, $sF(s)$ tends to 0.
## Example
$$\dot x_o = ax_o = ax_i$$
where $x_o$ is the output and $x_i$ is the input
Take the Laplace transform:
$$sX_o(s) + aX_o(s) = aX_i(s)$$
Rearrange to get equation for the transfer function:
$$G(s) = \frac{X_o}{X_i} = \frac{a}{s+a}$$
$$ X_o = GX_i $$
If $X_i$ is a unit step, then:
$$X_i = \frac1s$$
and
$$X_o = \frac{a}{s(s+a)}$$
Taking the inverse gives:
$$X_0 = 1 - e^{-at}$$