3:40 "if it's not simple -it's- *in* spherical coordinates" 3:58 -SI- *psi* 7:18, 8:48, 8:55, 8:58, 9:11, 13:35 and everywhere else: -row- *rho* 8:00 That tells you that the -case will kind of- *k^2 cannot* get quantized. 8:38 -vessel- *Bessel* 14:20 ... -difference- *different* from 0... 16:23 There is no way we can make -problems- *progress* with this problem...
Love you sir. From IIT Delhi. Thanks MIT.
5:33 -Parliamentary session- Parametrization
13:56 -there are some beautiful- under azimuthal
Thanks 🤍❤️
Thank you sr. I liked the explanation.
This is helpful ❤️🤍
Plane wave
3:40 "if it's not simple -it's- *in* spherical coordinates"
3:58 -SI- *psi*
7:18, 8:48, 8:55, 8:58, 9:11, 13:35 and everywhere else: -row- *rho*
8:00 That tells you that the -case will kind of- *k^2 cannot* get quantized.
8:38 -vessel- *Bessel*
14:20 ... -difference- *different* from 0...
16:23 There is no way we can make -problems- *progress* with this problem...
neat