(Schrodinger's Eqn.) - sign switching and I'm not sure why.
Hey, folks. I'm watching a lecture where somebody is showing the normalization of the waveform and they're messing around with i/some complex conjugates in the derivation/"proof" of this, but a sign switch occurs and I don't understand why. Here's the specific math below:
\[i \hbar \frac{\partial \psi(x,t)}{\partial t} = \bigg( - \frac{\hbar ^2}{2m} \frac{\partial^2 \psi(x,t)}{\partial x^2}+ V(x,t)\bigg) \psi (x,t)\] And then, assume the next pat has already been arrived at/achieved:
(Sorry, give me a minute. I'm getting confused.)
They divide through by \[i \hbar \]on the right hand side, but the sign changes for the first term from negative to positive, and the second from positive to negative. Why does this happen? @agent0smith
e.g.\[\frac{\partial \psi (x,t)}{\partial t} = \bigg(i\frac{\hbar}{2m}\frac{\partial^2 \psi(x,t)}{\partial x^2} -i\frac{V(x,t)}{\hbar}\bigg)\psi(x,t)\]
I'm assuming it has to do with the i, but I'm not certain at all.
@dan815
They multiplied both sides by i, and divided both sides by h. Then multiplied both sides by -1.
Just multiple both sides by -i/h, you get it
They explicitly said that they divided through by i, I don't really get why they said that, but this derivation makes sense. Thank you, guys.
You're allowed to divide through by i, right? Is that not allowed? I'm not big on complex/imaginary numbers.
If they divided by i, then they had to also multiply both sides by i^2. Kinda pointless.
Why would they have to multiply both sides through by i^2? Why wouldn't you be allowed to keep it as is?
Again, to be clear here, is i just not allowed to be in your denominator or something because of it equaling sqrt(-1)?
I just meant if they did what they said they did. I think they just misspoke. Yeah it's just one of those things like square roots being in denominators. I don't think they ever divided by i, anyway.
Alright, cool. Thank you!
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