Proving a complex wave satisfies Helmholtz equation

Matt Chu
Messages
16
Reaction score
0

Homework Statement



Consider a harmonic wave given by

$$\Psi (x, t) = U(x, y, z) e^{-i \omega t}$$

where ##U(x, y, z)## is called the complex amplitude. Show that ##U## satisfies the Helmholtz equation:

$$ (\nabla + k^2) U (x, y, z) = 0 $$

Homework Equations



Everything important already in the problem.

The Attempt at a Solution


[/B]
The first thing I attempted to do was to express ##U## in terms of ##\Psi## and ##e^{-i \omega t}##. This led me to a long set of derivations that in no way gave me anything remotely close to zero. I'm confused as to how to solve this, as the ##k## component of the Helmholtz equation seems to be problematic; it seems the only way to prove that the whole expression equals zero would be if ##U = 0##.
 
Physics news on Phys.org
Hello Matt,

How do you make use of the given that ##\Psi## is a harmonic wave ? What equation does ##\Psi## satisfy ?
 
BvU said:
Hello Matt,

How do you make use of the given that ##\Psi## is a harmonic wave ? What equation does ##\Psi## satisfy ?

Yeah, just figured that out a few minutes ago.
 
Good! makes it an easy exercise.
 
##|\Psi|^2=\frac{1}{\sqrt{\pi b^2}}\exp(\frac{-(x-x_0)^2}{b^2}).## ##\braket{x}=\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dx\,x\exp(-\frac{(x-x_0)^2}{b^2}).## ##y=x-x_0 \quad x=y+x_0 \quad dy=dx.## The boundaries remain infinite, I believe. ##\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dy(y+x_0)\exp(\frac{-y^2}{b^2}).## ##\frac{2}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,y\exp(\frac{-y^2}{b^2})+\frac{2x_0}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,\exp(-\frac{y^2}{b^2}).## I then resolved the two...
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