Wavefunction Evolution Problem: Solving for \phi_1

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SUMMARY

The discussion focuses on solving the wavefunction evolution problem for \phi_1 = A \sin \omega t \cos k(x+ct). The participants derive the second spatial derivative and the first temporal derivative of \phi_1, leading to a substitution into Schrödinger's Equation. The final equation presented, \hbar k^2 = i \cdot 2m (\tan k(x+ct) - \omega \cot \omega t), raises questions about the validity of the solution due to the mismatch between constants and functions of space and time. Suggestions include using complex exponentials via Euler's Theorem to further analyze the wavefunction.

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  • Understanding of wavefunctions and their evolution in quantum mechanics
  • Familiarity with Schrödinger's Equation and its applications
  • Knowledge of trigonometric identities and complex exponentials
  • Basic proficiency in calculus, particularly partial derivatives
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Domnu
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Problem
Describe the evolution in time of [tex]\phi_1 = A \sin \omega t \cos k(x+ct)[/tex].

Attempt at Solution
We have that

[tex]\partial^2 \phi_1 / \partial x^2 = -Ak^2 \sin \omega t \cos k(x+ct)[/tex]
[tex]\partial \phi_1 / \partial t = A \sin \omega t (-kc \cdot \sin k(x+ct)) + A \omega \cos \omega t \cos k(x+ct)[/tex]

Now, by Schroedinger's Equation,

[tex]-h^2/2m \cdot \partial^2\phi_1 / \partial x^2 = i \hbar \cdot \partial \phi_1 / \partial[/tex]

So, substituting, we have

[tex]\hbar^2 / 2m \cdot Ak^2 \sin \omega t \cos k(x+ct) = ihA \sin \omega t \cdot kc \sin k(x+ct) - i\hbar A \omega \cos \omega t \cos k(x+ct)[/tex]

[tex]\iff \hbar^2/2m \cdot k^2 \cdot \sin \omega t = i \hbar \sin \omega t \tan k(x+ct) - i \hbar \omega \cos \omega t[/tex]

[tex]\iff \hbar^2/2m \cdot k^2 = i\hbar \tan k(x+ct) - i \hbar \omega \cot \omega t[/tex]

[tex]\iff \hbar k^2 = i \cdot 2m (\tan \k(x+ct) - \omega \cot \omega t)[/tex]

Is this it? What am I to do now?
 
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What is [itex]\phi[/itex]?

(Sidenote: Looking at the function, the first term is a time dependent term whereas the second term is basically a "traveling wave" (for want of a better term...its actually the wavefunction of a free particle).)

I don't know what [itex]\phi[/itex] is, but if its the total wavefunction (we usually use [itex]\psi(x,t)[/itex] for it..lol :-p) and if your algebra is correct, the last equation doesn't make sense: the left hand side is a constant, whereas the right hand side is a function of space and time...for it to hold, [itex]x+ct[/itex] and [itex]\omega t[/itex] both should be constants (by a simple argument).

You could play around a bit by writing the whole thing as a bunch of complex exponentials, using Euler's Theorem...

[tex]\phi(x,t) = A\left(\frac{e^{i\omega t}-e^{-i\omega t}}{2i}\right)\left(\frac{e^{i(kx+kct)}+e^{-i(kx+kct)}}{2}\right)[/tex]

See if that helps...
 

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