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All results from a given calculation for CFCl2 (dichlorofluoromethyl radical)

using model chemistry: B2PLYP=FULL/6-31+G**

19 10 17 12 22

States and conformations

State Conformation minimum conformation conformer description state description
1 1 yes CS 2A'
Energy calculated at B2PLYP=FULL/6-31+G**
 hartrees
Energy at 0K-1057.847252
Energy at 298.15K 
HF Energy-1057.655315
Nuclear repulsion energy198.774735
The energy at 298.15K was derived from the energy at 0K and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B2PLYP=FULL/6-31+G**
Mode Number Symmetry Frequency
(cm-1)
Scaled Frequency
(cm-1)
IR Intensities
(km mol-1)
Raman Act
4/u)
Dep P Dep U
1 A' 1150 1094 265.14 1.45 0.72 0.84
2 A' 622 592 11.91 16.42 0.07 0.13
3 A' 467 444 0.93 2.04 0.53 0.69
4 A' 289 275 0.00 4.66 0.61 0.76
5 A" 931 886 327.37 2.24 0.75 0.86
6 A" 381 363 0.57 2.78 0.75 0.86

Unscaled Zero Point Vibrational Energy (zpe) 1920.3 cm-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 1826.2 cm-1
See section III.C.1 List or set vibrational scaling factors to change the scale factors used here.
See section III.C.2 Calculate a vibrational scaling factor for a given set of molecules to determine the least squares best scaling factor.
Rotational Constants (cm-1) from geometry optimized at B2PLYP=FULL/6-31+G**
ABC
0.24756 0.10900 0.07669

See section I.F.4 to change rotational constant units
Geometric Data calculated at B2PLYP=FULL/6-31+G**

Point Group is Cs

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
C1 0.163 0.432 0.000
F2 -0.725 1.436 0.000
Cl3 0.163 -0.456 1.480
Cl4 0.163 -0.456 -1.480

Atom - Atom Distances (Å)
  C1 F2 Cl3 Cl4
C11.34021.72591.7259
F21.34022.56072.5607
Cl31.72592.56072.9600
Cl41.72592.56072.9600

picture of dichlorofluoromethyl radical state 1 conformation 1
More geometry information
Calculated Bond Angles
atom1 atom2 atom3 angle atom1 atom2 atom3 angle
F2 C1 Cl3 112.665 F2 C1 Cl4 112.665
Cl3 C1 Cl4 118.081
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability