- 218 Views
- Uploaded on
- Presentation posted in: General

CHEM 515 Spectroscopy

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -

CHEM 515Spectroscopy

Vibrational Spectroscopy III

x

Q3

z

Q2

Q1

- Mathematically, the mass-weighted Cartesian coordinates (Cartesian force constant model) are very convenient. Ab initio calculation utilizes such a model in molecule optimization.
- A more recognizable way to define the atomic displacement in molecular modeling program is by utilizing internal coordinates.

- It is much convenient to transform from Cartesian coordinates to internal coordinates.
- These are the main four internal coordinate out of which other internal coordinated can be defined.

r1

r2

θ

- The internal displacement of atoms can be defined as change in the three coordinates.
- Δr1
- Δr2
- Δθ

- More preferably than internal coordinates is the use of symmetry coordinates.
- The concept of molecule symmetry “group theory” is applied with help of projection operators to generate the required 3N – 6 symmetry coordinates.

Symmetry specie

Normalization factor

Projection operator

Operation

New coordinate obtained from Inti upon operation R

Character for symmetry specie γ

- This totally symmetric projection operator is used to get a set of symmetric coordinates by linear combinations of internal coordinates.
- This method is also known as “Symmetry-Adapted Linear Combinations; SALCs)” as proposed by A. F. Cotton.

Symmetry specie

Normalization factor

Operation

New coordinate obtained from Inti upon operation R

Character for symmetry specie γ

- We are very concerned with the symmetry of each normal mode of vibration in a molecule.
- Each normal mode of vibration will form a basis for an irreducible representation (Γ) of the point group of the molecule.
- The objective is to determine what the character (trace) is for the transformation matrix corresponding to a particular operation in a specific molecule.

- H2O has C2v symmetry.
- Operation E results in the following transformations:

- The transformations in the x, y and z modes can be represented with the following matrix transformation:
- Trace of E matrix is equal to 9.

- The operation C2 is more interesting!
- Operation C2 results in the following transformations:

- The transformations in the x, y and z modes can be represented with the following matrix transformation:
- Trace of C2 matrix is equal to –1.

- The matrix transformation method is very cumbersome. However, it can be streamlined tremendously another procedure.
- Alternative Method:
- Count unshifted atoms per each operation.
- Multiply by contribution per unshifted atom to get the reducible representation (Γ).
- Determine (Γ) for each symmetry operation.
- Subtract Γtrans and Γrot from Γtot.
Γvib = Γtot – Γtrans – Γrot .

- 1. Count unshifted atoms per each operation.

- 2. Multiply by contribution per unshifted atom to get the reducible representation (Γ).

- 2. Multiply by contribution per unshifted atom to get the reducible representation (Γ).

- 3. Determine (Γ) for each symmetry operation.
ηi : number of times the irreducible representation (Γ) appears for the symmetry operation i.

h : order of the point group.

R : an operation of the group.

χR : character of the operation R in the reducible represent.

χiR : character of the operation R in the irreducible represent.

CR : number of members of class to which R belongs.

- 3. Determine (Γ) for each symmetry operation.

Γtot = 3A1 + A2 + 2B1 + 3B2

- Number of irreducible representations Γtot must equal to 3N for the molecule.

- Subtract Γtrans and Γrot from Γtot.

Γtot = 3A1 + A2 + 2B1 + 3B2

- Γvib = 2A1 + B2
The difference between A and B species is that the character under the principal rotational operation, which is in this case C2, is always +1 for A and –1 for B representations. The subscripts 1 and 2 are considered arbitrary labels.

A1

A1

B2

- Γvib = 2A1 + B2
None of these motions are degenerate. One can spot the degeneracy associated with a special normal mode of vibration when the irreducible representation has a value of 2 at least, such as E operation in C3v and C4v point groups.

A1

A1

B2

Physical Chemistry

By Robert G. Mortimer

- For molecules having a center of symmetry (i), the vibration that is symmetric w.r.t the center of symmetry is Raman active but not IR active, whereas those that are antisymmetric w.r.t the center of symmetry are IR active but not Raman active.

Ranges in cm-1:

- C-H stretch 2980 – 2850
- CH2 wag 1470 – 1450
- CH2 rock 740 – 720
- CH2 wag 1390 – 1370
- CH2 twist 1470 - 1440