For a box of length a, the wave functions which satisfies the Schrödinger equation is:
Y(x, t) = S cn yn(x)exp(-i En t / h)
where the sum goes from 1 to infinity, h is ``h bar,'' for which I can't find the markup code, and
yn(x) = sqrt(2/a) sin(nπx/a) and En = h2/(2m) (n π/a)2
Since all of the energies En are multiples of E1, any state has period
T = 2πh/E1 = 4 m a2/(hπ)
For a 1 gram particle in a 1 cm box, this period is about 1.2*1027sec, or about 4*1019 years. On the other hand, for an electron in a box 10-10 meters across, the period is about 10-16 seconds.
The figures show the probability density, |Y(x, t)|2, as a function of time for a particle in a superposition of the first three modes:
Y(x, t) = [ a y1(x)exp(-i E1 t / h) + b y2(x)exp(-i E2 t / h) + c y3(x)exp(-i E3 t / h) ]/sqrt(a2 + b2 + c2)
The wave function is normalized for any choice of a, b, and c. The dotted line shows the average probability density, 1/a.
First mode (stationary state).
Second mode (stationary state).
Initial state in left.
Symmetric initial state.
In all of these, you can click on ``scrollbar'' to change a, b, c, and d. The parameters a, b, and c are the amplitudes of the first three modes. The parameter d determines how fast time advances. (The period T is scaled to 2π/d seconds, with the default value of d=1/2.) The ``clock'' in the upper right goes around once for each period.
These graphs were produced by DPGraph, which is a fast program for viewing time-dependent graphs.