| If you have an electronic circuit, you can model each element with a differential equation. E.g. voltage across a capacitor is modelled as the integral of current, voltage across an inductor is dI/dt. This is a useful fact for a simple circuit in a classroom, but the differential equations for any circuit with more than a few components soon become insanely complex. With the Laplace transform you (more or less) replace an integral with 1/s and a differential with s, plus some constants derived from the component values. Then you can simplify for s, and use the Inverse Laplace Transform to convert the final expression in s into an expression in t. You have now solved an insanely complex differential equation with some basic algebra, and your final expression in t - with component constants, and some exponentials that appear after the inverse transform - accurately models how the circuit responds over time. There's also a related fairly simple trick for converting the s-domain representation into a frequency/phase plot which tells you how the circuit operates in the frequency domain. And another related fairly simple trick for converting the continuous s-domain into the z-domain for DSP calculations over a sampled time series. Because the same theory also applies in other domains - spring/mass systems, and so on - you can use the same technique there too. |
Examples
Converting numbers to logs allows you to multiply and divide by mere addition and subtraction. If you wonder why RF engineers represent power in db this is why.
Mapping an equation in terms of forces integrated over a path to one using vectors and energy.