(a) The Schrodinger equation is
(b) By separation of variables, we can take that the wave function to be the product of three wave functions each of a one-dimensional infinite well potential. The wave function of the lowest energy level is
The corresponding energy is E111 = 3h2r2/2mL2.
(c) For a set of quantum numbers nx, ny, nz for the three dimensions, the energy is
Hence the number N of states whose energy is less than or equal to E is equal to the number of sets of three positive integers nx, ny, nz satisfying the inequality
\(n_X^2 + n_y^2 + n_z^2 \le \frac{2mL^2}{h^2\pi^2} E\)
Consider a Cartesian coordinate system of axes nx, ny, nz. The number N required is numerically equal to the volume in the first quadrant of a sphere of radius (2mL2E/h2π2)1/2, provided N ≥ 1. Thus