If you really want to learn how to do it, probably the best place to learn this is to find a good textbook. Personally, I like "Introduction to Quantum Mechanics", by David J. Griffiths (ISBN 0-13-124405-1) as a very good introductory text. The math involved is partial differential equations, and linear algebra - these are math subjects people usually learn after doing calculus. <br /><br />Bearing in mind that this is not going to be nearly as good an explanation as you would get from a textbook, I can maybe give you a flavor for how the math works. So there are more or less three different ways of doing the math for quantum mechanics: the Schrodinger way, the Heisenberg way, and the Feynman way. They have very different philosophies and strengths/weaknesses but you can show that mathematically they're all equivalent. In the schrodinger way, everything is encapsulated in the wavefunction. In the simplest case, consider just a single particle, and say we'd like to know where it's going to be at a given time t. In classical physics you might say you'd like to know the position as a function of time, x(t). In the Schrodinger method for quantum mechanics what you'd like to know is the wavefunction Psi(x,t) (it's some function of a space coordinate and time, meaning you give a value for t and a value for x then you get out a value for Psi. Psi can look like anything, the only constraint is that the area under the curve Psi*Psi_bar must be 1 (Psi_bar is the complex conjugate of Psi), or in other words the integral of the amplitude squared of Psi from minus infinity to +infinity must be 1). Psi has the following interpretation: Psi(x,t) * Psi(x,t)_bar *dx is the probability of finding the particle between x and (x+dx) at time t when you do an experiment to detect it (Note that after doing the experiment the wavefunction will be peaked at precisely where you found the particle). So if at time t=t0 the function Psi(x,t0) is very broad then the particle is really u <div class="Discussion_UserSignature"> </div>