Uploaded August 2022 | Updated September 2026, 3 hours ago
In this video, I demonstrate a way of using Lagrange multipliers to solve for when a ball looses contact with a circle that it's rolling off of. This technique could be applied to other cases where a constraint applies for only some of the time evolution of a system, and it is necessary to calculate the point where it stops applying.
Typo at 2:25: On the RHS of the first equation of motion, there should be a square on the theta-dot.
In this video, I demonstrate a way of using Lagrange multipliers to solve for when a ball looses contact with a circle that it's rolling off of. This technique could be applied to other cases where a constraint applies for only some of the time evolution of a system, and it is necessary to calculate the point where it stops applying.
Typo at 2:25: On the RHS of the first equation of motion, there should be a square on the theta-dot.


![Annoying Ass Spinor Spherical Harmonics Identity | Quantum Mechanics
In this video, I show how to do a tricky homework problem that I had a while ago.
My Quantum Mechanics Lecture Series:
https://www.youtube.com/playlist?list=PLSpklniGdSfSsAFCzO-YWGlJ4TNv8sMdy
Typo: At 5:43, it should be Y(l , m+½) = (Sqrt { [ ( 2l + 1 ) ÷ 4π ] ⋅ ( l − m − ½ )! ÷ ( l + m + ½ )! } )⋅[exp i(m+½)φ]⋅P(l , m+½) Annoying Ass Spinor Spherical Harmonics Identity | Quantum Mechanics](https://i.ytimg.com/vi/ssdQWpWru-E/mqdefault.jpg)







