Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -278.298178 |
| Energy at 298.15K | |
| HF Energy | -278.298178 |
| Nuclear repulsion energy | 122.398957 |
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 B3LYP/LANL2DZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3109 |
2988 |
0.00 |
|
|
|
| 2 |
Ag |
1526 |
1467 |
0.00 |
|
|
|
| 3 |
Ag |
1436 |
1380 |
0.00 |
|
|
|
| 4 |
Ag |
1101 |
1058 |
0.00 |
|
|
|
| 5 |
Ag |
969 |
931 |
0.00 |
|
|
|
| 6 |
Ag |
430 |
413 |
0.00 |
|
|
|
| 7 |
Au |
3199 |
3075 |
56.01 |
|
|
|
| 8 |
Au |
1191 |
1145 |
3.84 |
|
|
|
| 9 |
Au |
848 |
816 |
1.39 |
|
|
|
| 10 |
Au |
105 |
101 |
21.28 |
|
|
|
| 11 |
Bg |
3174 |
3050 |
0.00 |
|
|
|
| 12 |
Bg |
1293 |
1243 |
0.00 |
|
|
|
| 13 |
Bg |
1145 |
1100 |
0.00 |
|
|
|
| 14 |
Bu |
3114 |
2994 |
60.62 |
|
|
|
| 15 |
Bu |
1530 |
1471 |
8.84 |
|
|
|
| 16 |
Bu |
1370 |
1317 |
2.04 |
|
|
|
| 17 |
Bu |
985 |
947 |
148.89 |
|
|
|
| 18 |
Bu |
265 |
254 |
29.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13394.4 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 12874.7 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.
Geometric Data calculated at B3LYP/LANL2DZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.443 |
0.621 |
0.000 |
| C2 |
-0.443 |
-0.621 |
0.000 |
| F3 |
-0.443 |
1.775 |
0.000 |
| F4 |
0.443 |
-1.775 |
0.000 |
| H5 |
1.063 |
0.679 |
0.900 |
| H6 |
1.063 |
0.679 |
-0.900 |
| H7 |
-1.063 |
-0.679 |
0.900 |
| H8 |
-1.063 |
-0.679 |
-0.900 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5257 | 1.4553 | 2.3959 | 1.0942 | 1.0942 | 2.1838 | 2.1838 |
C2 | 1.5257 | | 2.3959 | 1.4553 | 2.1838 | 2.1838 | 1.0942 | 1.0942 | F3 | 1.4553 | 2.3959 | | 3.6590 | 2.0687 | 2.0687 | 2.6864 | 2.6864 | F4 | 2.3959 | 1.4553 | 3.6590 | | 2.6864 | 2.6864 | 2.0687 | 2.0687 | H5 | 1.0942 | 2.1838 | 2.0687 | 2.6864 | | 1.7994 | 2.5232 | 3.0991 | H6 | 1.0942 | 2.1838 | 2.0687 | 2.6864 | 1.7994 | | 3.0991 | 2.5232 | H7 | 2.1838 | 1.0942 | 2.6864 | 2.0687 | 2.5232 | 3.0991 | | 1.7994 | H8 | 2.1838 | 1.0942 | 2.6864 | 2.0687 | 3.0991 | 2.5232 | 1.7994 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
106.951 |
|
C1 |
C2 |
H7 |
111.874 |
| C1 |
C2 |
H8 |
111.874 |
|
C2 |
C1 |
F3 |
106.951 |
| C2 |
C1 |
H5 |
111.874 |
|
C2 |
C1 |
H6 |
111.874 |
| F3 |
C1 |
H5 |
107.631 |
|
F3 |
C1 |
H6 |
107.631 |
| F4 |
C2 |
H7 |
107.631 |
|
F4 |
C2 |
H8 |
107.631 |
| H5 |
C1 |
H6 |
110.624 |
|
H7 |
C2 |
H8 |
110.624 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.141 |
|
|
|
| 2 |
C |
-0.141 |
|
|
|
| 3 |
F |
-0.282 |
|
|
|
| 4 |
F |
-0.282 |
|
|
|
| 5 |
H |
0.212 |
|
|
|
| 6 |
H |
0.212 |
|
|
|
| 7 |
H |
0.212 |
|
|
|
| 8 |
H |
0.212 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.548 |
4.119 |
0.000 |
| y |
4.119 |
-31.661 |
0.000 |
| z |
0.000 |
0.000 |
-21.074 |
|
| Traceless |
| | x | y | z |
| x |
4.820 |
4.119 |
0.000 |
| y |
4.119 |
-10.350 |
0.000 |
| z |
0.000 |
0.000 |
5.531 |
|
| Polar |
| 3z2-r2 | 11.062 |
| x2-y2 | 10.113 |
| xy | 4.119 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.168 |
-0.228 |
0.000 |
| y |
-0.228 |
3.524 |
0.000 |
| z |
0.000 |
0.000 |
2.880 |
<r2> (average value of r
2) Å
2
| <r2> |
92.300 |
| (<r2>)1/2 |
9.607 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -278.298850 |
| Energy at 298.15K | |
| HF Energy | -278.298850 |
| Nuclear repulsion energy | 124.301995 |
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 B3LYP/LANL2DZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3161 |
3039 |
18.57 |
|
|
|
| 2 |
A |
3096 |
2976 |
45.85 |
|
|
|
| 3 |
A |
1493 |
1435 |
2.70 |
|
|
|
| 4 |
A |
1427 |
1372 |
6.10 |
|
|
|
| 5 |
A |
1272 |
1223 |
1.92 |
|
|
|
| 6 |
A |
1121 |
1077 |
3.75 |
|
|
|
| 7 |
A |
1070 |
1029 |
44.05 |
|
|
|
| 8 |
A |
845 |
812 |
29.28 |
|
|
|
| 9 |
A |
320 |
308 |
1.09 |
|
|
|
| 10 |
A |
142 |
136 |
7.40 |
|
|
|
| 11 |
B |
3172 |
3049 |
35.05 |
|
|
|
| 12 |
B |
3084 |
2964 |
13.52 |
|
|
|
| 13 |
B |
1492 |
1434 |
14.50 |
|
|
|
| 14 |
B |
1411 |
1357 |
5.12 |
|
|
|
| 15 |
B |
1218 |
1170 |
4.19 |
|
|
|
| 16 |
B |
1045 |
1005 |
29.14 |
|
|
|
| 17 |
B |
880 |
846 |
47.31 |
|
|
|
| 18 |
B |
469 |
451 |
21.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13358.8 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 12840.5 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.
Geometric Data calculated at B3LYP/LANL2DZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.296 |
0.697 |
0.519 |
| C2 |
-0.296 |
-0.697 |
0.519 |
| F3 |
-0.296 |
1.484 |
-0.546 |
| F4 |
0.296 |
-1.484 |
-0.546 |
| H5 |
0.067 |
1.214 |
1.460 |
| H6 |
1.376 |
0.669 |
0.344 |
| H7 |
-0.067 |
-1.214 |
1.460 |
| H8 |
-1.376 |
-0.669 |
0.344 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5138 | 1.4508 | 2.4275 | 1.0974 | 1.0951 | 2.1607 | 2.1662 |
C2 | 1.5138 | | 2.4275 | 1.4508 | 2.1607 | 2.1662 | 1.0974 | 1.0951 | F3 | 1.4508 | 2.4275 | | 3.0268 | 2.0564 | 2.0622 | 3.3702 | 2.5691 | F4 | 2.4275 | 1.4508 | 3.0268 | | 3.3702 | 2.5691 | 2.0564 | 2.0622 | H5 | 1.0974 | 2.1607 | 2.0564 | 3.3702 | | 1.8038 | 2.4324 | 2.6222 | H6 | 1.0951 | 2.1662 | 2.0622 | 2.5691 | 1.8038 | | 2.6222 | 3.0609 | H7 | 2.1607 | 1.0974 | 3.3702 | 2.0564 | 2.4324 | 2.6222 | | 1.8038 | H8 | 2.1662 | 1.0951 | 2.5691 | 2.0622 | 2.6222 | 3.0609 | 1.8038 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
109.913 |
|
C1 |
C2 |
H7 |
110.666 |
| C1 |
C2 |
H8 |
111.244 |
|
C2 |
C1 |
F3 |
109.913 |
| C2 |
C1 |
H5 |
110.666 |
|
C2 |
C1 |
H6 |
111.244 |
| F3 |
C1 |
H5 |
106.783 |
|
F3 |
C1 |
H6 |
107.365 |
| F4 |
C2 |
H7 |
106.783 |
|
F4 |
C2 |
H8 |
107.365 |
| H5 |
C1 |
H6 |
110.715 |
|
H7 |
C2 |
H8 |
110.715 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.133 |
|
|
|
| 2 |
C |
-0.133 |
|
|
|
| 3 |
F |
-0.275 |
|
|
|
| 4 |
F |
-0.275 |
|
|
|
| 5 |
H |
0.188 |
|
|
|
| 6 |
H |
0.221 |
|
|
|
| 7 |
H |
0.188 |
|
|
|
| 8 |
H |
0.221 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
3.577 |
3.577 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.210 |
2.415 |
0.000 |
| y |
2.415 |
-27.669 |
0.000 |
| z |
0.000 |
0.000 |
-21.993 |
|
| Traceless |
| | x | y | z |
| x |
3.621 |
2.415 |
0.000 |
| y |
2.415 |
-6.068 |
0.000 |
| z |
0.000 |
0.000 |
2.447 |
|
| Polar |
| 3z2-r2 | 4.895 |
| x2-y2 | 6.459 |
| xy | 2.415 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.015 |
-0.069 |
0.000 |
| y |
-0.069 |
3.374 |
0.000 |
| z |
0.000 |
0.000 |
3.237 |
<r2> (average value of r
2) Å
2
| <r2> |
83.608 |
| (<r2>)1/2 |
9.144 |