Rigid rotator Flashcards
Basic theory
2D, particle on a ring
What can it help us understand?
Cyclic molecules like aromatics
Angular momentum equation
J = Iw
Where J is angular momentum, I is the moment of Inertia and w is the angular velocity
Moment of Inertia equation
I = mr^2
m is mass and r is distance from axis of rotation
What is the axis of rotation for rigid rotator?
Jz as particle is confined in the x and y plane so we only have rotation about the z axis
What values can the quantum number m_l take
m_l = 0,±1,±2,….,±l
Jz simplification
Jz=±Iw=±mr^2w=±mvr=±pr
Why can Jz = ± value
Jz will vary based on direction of rotation, if clockwise Jz>0, if anticlockwise Jz<0
Boundary condition for rigid rotator
Cyclic motion, so for constructive interference of our wavefunction we must have our Ψ repeat after 2pi radians of rotation.
If there is deconstructive interference particle will destroy itself
Boundary condition equation
Ψ(ϕ=0)=Ψ(ϕ=2pi)
Derivation to show quantised wavelength
λ*m_l =2pir
λ=2pir/m_l
m_l is the quantum number so wavelength is quantised
Derivation to show quantised energy
Jz=±pr
p=h/λ
Jz=±hr/λ
λ=2pir/m_l
Jz=±m_lℏ
E=Jz^2/2I
E=m_l^2ℏ^2/2I
So energy is quantised
Double degeneracy
Since quantum number which can be + and - is squared then our energy can have 2 of the same values when m_l =|value| >0
Zero point energy
Can be 0 as m_l is can be 0, which means we have no idea for the probability density which fits with schrodingers
Rigid rotator Schrodinger equation
(-(ℏ^2)/2m)(∇^2Ψ) =EΨ