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Trifluoromethane Molecular Orbital Calculations
The Highest Occupied Molecular Orbital (HOMO) for Trifluoromethane (CHF3) was determined using the Double Zeta Valence (DZV) level of theory.


The Lowest Unoccupied Molecular Orbital (LUMO) for CHF3 was based off of DZV calculations.


Th electrostatic potential of CHF3 was mapped; red represents high electrons density and blue represents low electron density.


The partial atomic charges for carbon, hydrogen, and fluorine in CHF3 were determined based on the DZV level of theory.

 
The bond lengths and bond angles for CHF3 were determined based on the DZV geometry optimization.

The DZV level of theory was chosen for this molecule because it determined the most accurate bond lengths and bond angles.

Table 1:
Experimental and literature values for bond lengths and angles for CHF3.1
Bond
Bond Length (Å)
Bond Angle (º)
C-H
1.098±0.008
---------------------
C-F
1.332±0.008
108.8

An IR spectrum for CHF3 can be seen by following the link below.
CHF3 IR Spectrum

Table 2:
The wavenumbers and the corresponding bending and/or stretching that occurs at the significant peaks on the IR spectra above.2
Wavenumber (1/cm)
Bond and Motion
~1150
C-F stretching
~1400
Csp3-bending
~3050
Csp3-H stretching
These different modes of vibration can be seen by clicking the buttons below.

The button Fluorine Bending Mode will appear in the box below. Insert information for Fluorine Bending Mode here and below.

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The button Fluorine Bending and Stretching will appear in the box below. Insert information for Fluorine Bending and Stretching here and below.

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The button Hydrogen Bending will appear in the box below. Insert information for Hydrogen Bending here and below.

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The button Hydrogen Stretching will appear in the box below. Insert information for Hydrogen Stretching here and below.

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Table 3: The dipole moments of CHF3 at the different levels of theory.1
Level of Theory
Dipole Moment (D)
AM1
2.079345
6-31G
2.372354
6-21G
2.106802
DZV
2.554768
Theoretical
1.651
The best calculated value was the result of the AM1 calculation. The smaller basis set allowed for a lower value, which was  closer to the theoretical value, although it still was not very accurate.



Based on template by A. Herráez as modified by J. Gutow
Page skeleton and JavaScript generated by export to web function using Jmol 12.2.34 2012-08-09 20:37 on Feb 25, 2013.