The problem, like all energy-conserving 1D problems, reduces to quadratures: that is, it reduces to solving a 1D integral. In this specific case (with no centrifugal barrier) that integral is exactly solvable.
To get this, you simply repeat the same steps that you do in the work-energy theorem: ...
There is a very quick and clean way of doing this, which is presented in
Building an Orthonormal Basis from a 3D Unit Vector Without Normalization. JR Frisvad. J. Graphics Tools 16 no. 3, 151 (2012).
Suppose you have a normalized vector $\vec n=(n_x,n_y,n_z)^T$, and you want a rotation matr...
Yes. It boils down to the orientation-averaged polarizability of the molecule, which is a perfectly calculable property of the molecule and it has been accessible to quantum-chemistry methods for many decades.
In essence, you take the molecule in its ground state (or in some thermal ensemble, as...
Not testable or observable, dont waste your time, research flat earth and realise the lies, the guys giving you the answer is full of sh1t..
Pretending to know something he knows jack about..
Funny sheeple..
