Lecture 33 Rotational spectroscopy: energies. Rotational spectroscopy In this lecture, we will...
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Transcript of Lecture 33 Rotational spectroscopy: energies. Rotational spectroscopy In this lecture, we will...
![Page 1: Lecture 33 Rotational spectroscopy: energies. Rotational spectroscopy In this lecture, we will consider the rotational energy levels. In the next lecture,](https://reader035.fdocuments.in/reader035/viewer/2022082209/5a4d1b6e7f8b9ab0599b4531/html5/thumbnails/1.jpg)
Lecture 33Rotational spectroscopy: energies
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Rotational spectroscopy
In this lecture, we will consider the rotational energy levels.
In the next lecture, we will focus more on selection rules and intensities.
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Diatomic molecule A rigid linear rotor in 3D =
the particle on a sphere
Moment of inertia
4
3
2
1
J = 0E
nerg
y
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Moments of inertiaPrincipal axis of rotation
Principal moment of inertia
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Linear rotors
Two equal nonzero moments of inertia (Ia and Ib)and the third (Ic) equal to zero
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Spherical rotors
Three equal moments of inertia
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Symmetric rotors
Two equal moments of inertia
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The rotational energy levels (in cm–1) = 1 / λ
= v / c = hv / hc = E / hc
The rotational constant B is given in cm–1
20B
12B
6B
2B0B
Ene
rgy
2B
4B
6B
8B
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Quantum in natureHow could
chemists know HF bond length
is 0.917Å?
Microwave spectroscopy
or computational
quantum chemistry
Wikipedia
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Spherical & linear rotors In units of cm–1:
( ) 1F J BJ J
20B
12B
6B
2B0B
Ene
rgy
2B
4B
6B
8B
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Symmetric rotors Classically,
Quantum-mechanical rotational terms are
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Symmetric rotorsK acts just like MJ. The only distinction is that K refers to rotation around
the principal axis, whereas MJ to externally fixed axis
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Degeneracy Linear rotors
(2J+1)-fold degeneracy (MJ = 0,±1,…, ±J) Symmetric rotors
(2J+1)-fold degeneracy (MJ = 0,±1,…, ±J) another 2-fold degeneracy (K = ±1,…, ±J)
[(A – B) ≠ 0 and K and –K give the same energy] Spherical rotors
(2J+1)-fold degeneracy (MJ = 0,±1,…, ±J) another (2J+1)-fold degeneracy (K = 0,±1,…, ±J)
[(A – B) = 0 and energy does not depend on K] K for shape, MJ for orientation.
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Zeeman effectMJ -degeneracy can be lifted by applying a static magnetic field.
−3−2−10+1+2+3
MJfieldon
fieldoff
First-order perturbation theory
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Zeeman effect
−3−2−10+1+2+3
MJfieldon
fieldoff
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Stark effect
2 2
2
, 1 ,
1 3,
2 1 2 1 2 3
J J
JJ
E J M hcBJ J a J M E
J J Ma J M
hcBJ J J J
MJ -degeneracy can also be lifted by applying a static electric field.
±10
MJfieldon
fieldoff
±2
±3
±4
Second-order perturbation theory
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Stark effect
2 2
2
, 1 ,
1 3,
2 1 2 1 2 3
J J
JJ
E J M hcBJ J a J M E
J J Ma J M
hcBJ J J J
±10
MJfieldon
fieldoff
±2
±3
±4
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Linear rotors
No degeneracy
2J+1 degenerateStark effect
Zeemaneffect
No rotationaround the axis
2ND order PT1ST order
PT
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Spherical rotors
2J+1 degenerate
2J+1 degenerateStark effect
Zeemaneffect
2ND order PT1ST order
PT
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Symmetric rotors
Doubly degenerate
2J+1 degenerateStark effect
Zeemaneffect
2ND order PT1ST order
PT
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Willis FlygareFrom UIUC Department of Chemistry website“Willis Flygare earned his bachelor's degree from St. Olaf College in 1958 and his doctorate from the University of California at Berkeley in 1961. He was a professor of chemistry at Illinois from 1961 until his death. During that period he developed a new experimental method involving the molecular Zeeman effect, and with it, he measured most of the known molecular quadrupole moments and magnetic susceptibility anisotropies. He developed a highly sensitive microwave spectrometer by combining molecular beams with Fourier transform techniques.”
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Summary We have learned about the rotational energy
levels of molecules in the rigid-rotor approximation.
We have classified rigid rotors into linear rotors, spherical rotors, symmetric rotors, and the rest.
We have discussed the energy levels and their degeneracy of these rotors.
We have learned about the Zeeman and Stark effects.