Particle in a Cube: Find Wavefunction w/Initial Conditions

  • Thread starter Thread starter chill_factor
  • Start date Start date
  • Tags Tags
    Cube Particle
chill_factor
Messages
898
Reaction score
5

Homework Statement



Problem 13.7.17 in Mathematical Methods in Physical Sciences:

Find the wavefunction of a particle in a cube, referring to 13.3.6.

0 < x < L, 0 < y < L, 0 < z < L

13.3.6:

Find the wavefunction of a particle in a square 0 < x < L, 0 < y < L. Assume V = 0.

Homework Equations



-(hbar)^2/2m * Laplacian(ψ) = i(hbar)*∂(ψ)/∂t

The Attempt at a Solution



Use separation of variables.

ψ = U(x,y,z)T(t)

Substitute UT into the equation and then divide both sides by UT to separate it into time dependent and time independent parts.

(hbar)^2/2m * Laplacian(U) - E*U = 0
i(hbar)*∂(ψ)/∂t = T

Solve the time dependent ordinary differential equation for T:

T = exp(-iEt/hbar)

If the time independent schrodinger equation was in 1-D, it would be:

-(hbar)^2/2m * ∂(U)/∂x = E*U

Assume E = k^2, where k^2 = 2Em/(hbar)^2

∂(U)/∂x = -k^2*U

U must be a sin or cos function in terms of U(x) but due to boundary conditions that it must be 0 at x=0 and x=L, it cannot be cos which would be nonzero at x = 0.

U = sin(kx), k = n∏/L where n = 1,2,3...

By analog with the 1-D case, the 3-D solutions should be:

Ux = sin k1 * x
Uy = sin k2 * y
Uz = sin k3 * z

with the constants K being all a constant (n,m,p) times ∏/L .

The final solution is then ψ = UxUyUzT = Ʃ A(nmp)sin(k1x)sin(k2y)sin(k3z)exp(-iEt/hbar)

Now we attempt to use initial conditions to set up a triple Fourier series and find A(nmp) where the 1-D analog would be the Fourier series

A(n) = (2/L) * ∫(initial condition functions) sin(kx)dx from 0 to L.

The problem does NOT give initial conditions so I have no idea how to solve the problem now. What can I possibly assume for the initial conditions such that I can obtain a solution?
 
Physics news on Phys.org
Given that no initial conditions are specified, it's probably asking for a generic solution, which you have.
 
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top