Schrodinger Equation
#Physics #Chemistry
Universal Danker Video
Non-relativistic and doesn't account for electron spin. The Dirac Equation accounts for these issues
Topics
Solution
$\displaystyle \Psi(\vec{r},t)=\psi(\vec{r})\phi(t),\phi (t)=e^{-iEt/\hbar}$
- Solved by separation of variables
- Must be square integrable
$\displaystyle \Psi(\vec{r},t)=\sum_{n = 1}^{\infty}c_{n}\psi_{n}(\vec{r})e^{-iE_{n}t/\hbar}$
- A wave function can be the linear combination of a bunch of wave functions, which by Fourier's Theorem, can represent any type of wave function that satisfies the Schrodinger equation
- $\displaystyle \psi_{n}(\vec{r})$ is the time-independent solution for the $\displaystyle n$th wave function
- $\displaystyle c_{n}$ is the wave function weighting coefficient
- $\displaystyle E_{n}$ is the energy of the $\displaystyle n$th wave function
- Each $\displaystyle \psi_{n}$ is orthogonality to each other
How to Solve
Given $\displaystyle V(x)$ and $\displaystyle \Psi(x,0)$, solve $\displaystyle \Psi(x,t)$
- Solve the TISE $\displaystyle \hat{H}\psi=E\psi$
- $\displaystyle \psi(x)=\sum_{n}c_{n}\psi_{n}(x)$
- $\displaystyle c_{n}=\int \psi_{n}^{*}(x)\Psi_{(x,0)} , \mathrm{d}x$
- Use $\displaystyle \Psi(x,t)=\sum_{n}c_{n}\psi_{n}(x)e^{-iE_{n}t/\hbar}=\sum_{n = 1}^{\infty}c_{n}\Psi_{n}(x,t)$