Jump to
S1C2
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -277.030979 |
| Energy at 298.15K | |
| HF Energy | -277.030979 |
| Nuclear repulsion energy | 127.282769 |
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 HF/6-311+G(3df,2p)
| 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 |
3206 |
2913 |
0.00 |
222.72 |
0.06 |
0.12 |
| 2 |
Ag |
1647 |
1497 |
0.00 |
6.24 |
0.75 |
0.86 |
| 3 |
Ag |
1590 |
1444 |
0.00 |
2.56 |
0.28 |
0.44 |
| 4 |
Ag |
1182 |
1074 |
0.00 |
9.08 |
0.72 |
0.84 |
| 5 |
Ag |
1155 |
1050 |
0.00 |
8.18 |
0.15 |
0.26 |
| 6 |
Ag |
497 |
452 |
0.00 |
2.24 |
0.34 |
0.50 |
| 7 |
Au |
3272 |
2973 |
64.03 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1352 |
1229 |
8.32 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
873 |
793 |
0.05 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
138 |
125 |
15.71 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3243 |
2946 |
0.00 |
102.68 |
0.75 |
0.86 |
| 12 |
Bg |
1408 |
1280 |
0.00 |
6.76 |
0.75 |
0.86 |
| 13 |
Bg |
1286 |
1168 |
0.00 |
1.10 |
0.75 |
0.86 |
| 14 |
Bu |
3209 |
2916 |
70.33 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1652 |
1501 |
4.55 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1483 |
1348 |
13.64 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1180 |
1072 |
282.03 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
312 |
283 |
22.99 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 14341.9 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 13031.0 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 HF/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.419 |
0.629 |
0.000 |
| C2 |
-0.419 |
-0.629 |
0.000 |
| F3 |
-0.419 |
1.700 |
0.000 |
| F4 |
0.419 |
-1.700 |
0.000 |
| H5 |
1.042 |
0.678 |
0.882 |
| H6 |
1.042 |
0.678 |
-0.882 |
| H7 |
-1.042 |
-0.678 |
0.882 |
| H8 |
-1.042 |
-0.678 |
-0.882 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5120 | 1.3603 | 2.3291 | 1.0813 | 1.0813 | 2.1503 | 2.1503 |
C2 | 1.5120 | | 2.3291 | 1.3603 | 2.1503 | 2.1503 | 1.0813 | 1.0813 | F3 | 1.3603 | 2.3291 | | 3.5020 | 1.9897 | 1.9897 | 2.6121 | 2.6121 | F4 | 2.3291 | 1.3603 | 3.5020 | | 2.6121 | 2.6121 | 1.9897 | 1.9897 | H5 | 1.0813 | 2.1503 | 1.9897 | 2.6121 | | 1.7650 | 2.4869 | 3.0496 | H6 | 1.0813 | 2.1503 | 1.9897 | 2.6121 | 1.7650 | | 3.0496 | 2.4869 | H7 | 2.1503 | 1.0813 | 2.6121 | 1.9897 | 2.4869 | 3.0496 | | 1.7650 | H8 | 2.1503 | 1.0813 | 2.6121 | 1.9897 | 3.0496 | 2.4869 | 1.7650 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.246 |
|
C1 |
C2 |
H7 |
110.940 |
| C1 |
C2 |
H8 |
110.940 |
|
C2 |
C1 |
F3 |
108.246 |
| C2 |
C1 |
H5 |
110.940 |
|
C2 |
C1 |
H6 |
110.940 |
| F3 |
C1 |
H5 |
108.621 |
|
F3 |
C1 |
H6 |
108.621 |
| F4 |
C2 |
H7 |
108.621 |
|
F4 |
C2 |
H8 |
108.621 |
| H5 |
C1 |
H6 |
109.404 |
|
H7 |
C2 |
H8 |
109.404 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.293 |
|
|
|
| 2 |
C |
0.293 |
|
|
|
| 3 |
F |
-0.545 |
|
|
|
| 4 |
F |
-0.545 |
|
|
|
| 5 |
H |
0.126 |
|
|
|
| 6 |
H |
0.126 |
|
|
|
| 7 |
H |
0.126 |
|
|
|
| 8 |
H |
0.126 |
|
|
|
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 |
-22.053 |
3.482 |
0.000 |
| y |
3.482 |
-29.669 |
0.000 |
| z |
0.000 |
0.000 |
-21.324 |
|
| Traceless |
| | x | y | z |
| x |
3.443 |
3.482 |
0.000 |
| y |
3.482 |
-7.980 |
0.000 |
| z |
0.000 |
0.000 |
4.537 |
|
| Polar |
| 3z2-r2 | 9.074 |
| x2-y2 | 7.615 |
| xy | 3.482 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.886 |
-0.033 |
0.000 |
| y |
-0.033 |
4.036 |
0.000 |
| z |
0.000 |
0.000 |
3.618 |
<r2> (average value of r
2) Å
2
| <r2> |
86.553 |
| (<r2>)1/2 |
9.303 |
Jump to
S1C1
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -277.031554 |
| Energy at 298.15K | |
| HF Energy | -277.031554 |
| Nuclear repulsion energy | 129.407359 |
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 HF/6-311+G(3df,2p)
| 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 |
3239 |
2943 |
21.74 |
78.42 |
0.75 |
0.85 |
| 2 |
A |
3202 |
2909 |
44.89 |
203.37 |
0.02 |
0.04 |
| 3 |
A |
1624 |
1476 |
0.76 |
1.20 |
0.73 |
0.84 |
| 4 |
A |
1580 |
1436 |
14.67 |
1.56 |
0.05 |
0.10 |
| 5 |
A |
1417 |
1287 |
5.80 |
7.51 |
0.67 |
0.80 |
| 6 |
A |
1238 |
1124 |
44.49 |
1.97 |
0.12 |
0.22 |
| 7 |
A |
1218 |
1107 |
79.70 |
3.53 |
0.72 |
0.84 |
| 8 |
A |
941 |
855 |
27.31 |
6.92 |
0.14 |
0.25 |
| 9 |
A |
347 |
316 |
0.31 |
0.28 |
0.28 |
0.44 |
| 10 |
A |
161 |
147 |
4.42 |
0.07 |
0.75 |
0.86 |
| 11 |
B |
3254 |
2957 |
52.26 |
10.48 |
0.75 |
0.86 |
| 12 |
B |
3187 |
2896 |
12.13 |
33.00 |
0.75 |
0.86 |
| 13 |
B |
1622 |
1473 |
7.64 |
5.48 |
0.75 |
0.86 |
| 14 |
B |
1532 |
1392 |
10.96 |
0.02 |
0.75 |
0.86 |
| 15 |
B |
1379 |
1253 |
10.62 |
2.12 |
0.75 |
0.86 |
| 16 |
B |
1200 |
1090 |
64.16 |
3.78 |
0.75 |
0.86 |
| 17 |
B |
989 |
899 |
54.75 |
2.32 |
0.75 |
0.86 |
| 18 |
B |
543 |
494 |
20.84 |
0.37 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 14335.8 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 13025.5 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 HF/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.260 |
0.705 |
0.504 |
| C2 |
-0.260 |
-0.705 |
0.504 |
| F3 |
-0.260 |
1.403 |
-0.540 |
| F4 |
0.260 |
-1.403 |
-0.540 |
| H5 |
-0.033 |
1.200 |
1.422 |
| H6 |
1.338 |
0.715 |
0.414 |
| H7 |
0.033 |
-1.200 |
1.422 |
| H8 |
-1.338 |
-0.715 |
0.414 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5025 | 1.3583 | 2.3520 | 1.0833 | 1.0818 | 2.1270 | 2.1390 |
C2 | 1.5025 | | 2.3520 | 1.3583 | 2.1270 | 2.1390 | 1.0833 | 1.0818 | F3 | 1.3583 | 2.3520 | | 2.8535 | 1.9847 | 1.9830 | 3.2724 | 2.5606 | F4 | 2.3520 | 1.3583 | 2.8535 | | 3.2724 | 2.5606 | 1.9847 | 1.9830 | H5 | 1.0833 | 2.1270 | 1.9847 | 3.2724 | | 1.7691 | 2.4014 | 2.5273 | H6 | 1.0818 | 2.1390 | 1.9830 | 2.5606 | 1.7691 | | 2.5273 | 3.0334 | H7 | 2.1270 | 1.0833 | 3.2724 | 1.9847 | 2.4014 | 2.5273 | | 1.7691 | H8 | 2.1390 | 1.0818 | 2.5606 | 1.9830 | 2.5273 | 3.0334 | 1.7691 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.499 |
|
C1 |
C2 |
H7 |
109.620 |
| C1 |
C2 |
H8 |
110.673 |
|
C2 |
C1 |
F3 |
110.499 |
| C2 |
C1 |
H5 |
109.620 |
|
C2 |
C1 |
H6 |
110.673 |
| F3 |
C1 |
H5 |
108.227 |
|
F3 |
C1 |
H6 |
108.183 |
| F4 |
C2 |
H7 |
108.227 |
|
F4 |
C2 |
H8 |
108.183 |
| H5 |
C1 |
H6 |
109.589 |
|
H7 |
C2 |
H8 |
109.589 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.296 |
|
|
|
| 2 |
C |
0.296 |
|
|
|
| 3 |
F |
-0.550 |
|
|
|
| 4 |
F |
-0.550 |
|
|
|
| 5 |
H |
0.125 |
|
|
|
| 6 |
H |
0.129 |
|
|
|
| 7 |
H |
0.125 |
|
|
|
| 8 |
H |
0.129 |
|
|
|
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 |
2.912 |
2.912 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.581 |
1.829 |
0.000 |
| y |
1.829 |
-26.249 |
0.000 |
| z |
0.000 |
0.000 |
-22.465 |
|
| Traceless |
| | x | y | z |
| x |
2.776 |
1.829 |
0.000 |
| y |
1.829 |
-4.226 |
0.000 |
| z |
0.000 |
0.000 |
1.451 |
|
| Polar |
| 3z2-r2 | 2.901 |
| x2-y2 | 4.668 |
| xy | 1.829 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.727 |
0.026 |
0.000 |
| y |
0.026 |
3.993 |
0.000 |
| z |
0.000 |
0.000 |
3.860 |
<r2> (average value of r
2) Å
2
| <r2> |
78.202 |
| (<r2>)1/2 |
8.843 |