Rigid rotator Flashcards

1
Q

Basic theory

A

2D, particle on a ring

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2
Q

What can it help us understand?

A

Cyclic molecules like aromatics

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3
Q

Angular momentum equation

A

J = Iw
Where J is angular momentum, I is the moment of Inertia and w is the angular velocity

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4
Q

Moment of Inertia equation

A

I = mr^2
m is mass and r is distance from axis of rotation

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5
Q

What is the axis of rotation for rigid rotator?

A

Jz as particle is confined in the x and y plane so we only have rotation about the z axis

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6
Q

What values can the quantum number m_l take

A

m_l = 0,±1,±2,….,±l

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7
Q

Jz simplification

A

Jz=±Iw=±mr^2w=±mvr=±pr

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8
Q

Why can Jz = ± value

A

Jz will vary based on direction of rotation, if clockwise Jz>0, if anticlockwise Jz<0

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9
Q

Boundary condition for rigid rotator

A

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

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10
Q

Boundary condition equation

A

Ψ(ϕ=0)=Ψ(ϕ=2pi)

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11
Q

Derivation to show quantised wavelength

A

λ*m_l =2pir
λ=2pir/m_l
m_l is the quantum number so wavelength is quantised

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12
Q

Derivation to show quantised energy

A

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

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13
Q

Double degeneracy

A

Since quantum number which can be + and - is squared then our energy can have 2 of the same values when m_l =|value| >0

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14
Q

Zero point energy

A

Can be 0 as m_l is can be 0, which means we have no idea for the probability density which fits with schrodingers

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15
Q

Rigid rotator Schrodinger equation

A

(-(ℏ^2)/2m)(∇^2Ψ) =EΨ

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16
Q

Laplacian for rigid rotator

A

∇^2 for 2d= d^2/dx^2+ d^2/dy^2
Convert to spherical coordinates:
d^2/dr^2 +(1/r)d/dr+(1/r2)d^2/dϕ^2
For us r is constant so
∇^2 = (1/r^2)d^2/dϕ^2
Where ϕ is our angle of rotation
(remember these are partial derivatives)

17
Q

Simplified schrodinger equation for rigid rotator

A

(-(ℏ^2)/2I)(d^2Ψ/dϕ^2) =EΨ
Where I is the moment of inertia

18
Q

General solution for wavefunction

A

Ψ =Ae^im_lϕ
Where i is the (-1)^1/2
m_l is our quantum number and ϕ is our angle of rotation
A is just a constant

19
Q

Calculating constant A process

A

Use normalisation integral:
∫ΨΨdx = 1
Remember we will be in spherical so change x to ϕ
And remember that Ψ
will be - as it is a complex number so cancels out.
Integral is between 0 and 2pi, will eventually give
A =(1/2pi)^1/2

20
Q

Calculating Energy

A

Sub in general equation for Ψ into simplified Schrodinger’s, solve for E.
Will get E = (ℏ^2m_l^2)/2I =Jz^2/2I