Jump to
S1C2
Energy calculated at QCISD/cc-pVDZ
| | hartrees |
| Energy at 0K | -376.666405 |
| Energy at 298.15K | |
| HF Energy | -375.806654 |
| Nuclear repulsion energy | 190.306659 |
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 QCISD/cc-pVDZ
| 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 |
3163 |
3035 |
34.25 |
|
|
|
| 2 |
A |
3128 |
3001 |
31.17 |
|
|
|
| 3 |
A |
3095 |
2970 |
20.04 |
|
|
|
| 4 |
A |
1501 |
1440 |
3.22 |
|
|
|
| 5 |
A |
1487 |
1426 |
20.70 |
|
|
|
| 6 |
A |
1426 |
1368 |
30.00 |
|
|
|
| 7 |
A |
1353 |
1298 |
30.85 |
|
|
|
| 8 |
A |
1272 |
1220 |
14.77 |
|
|
|
| 9 |
A |
1195 |
1147 |
103.91 |
|
|
|
| 10 |
A |
1162 |
1115 |
83.70 |
|
|
|
| 11 |
A |
1146 |
1100 |
117.67 |
|
|
|
| 12 |
A |
1118 |
1073 |
43.95 |
|
|
|
| 13 |
A |
925 |
887 |
34.18 |
|
|
|
| 14 |
A |
585 |
561 |
4.85 |
|
|
|
| 15 |
A |
477 |
458 |
19.09 |
|
|
|
| 16 |
A |
432 |
414 |
5.82 |
|
|
|
| 17 |
A |
241 |
231 |
8.43 |
|
|
|
| 18 |
A |
119 |
115 |
7.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 11913.3 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 11429.6 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 QCISD/cc-pVDZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.774 |
-0.594 |
-0.282 |
| C2 |
0.470 |
0.021 |
0.329 |
| F3 |
-1.882 |
0.108 |
0.150 |
| F4 |
1.537 |
-0.759 |
-0.008 |
| F5 |
0.675 |
1.264 |
-0.183 |
| H6 |
-0.701 |
-0.536 |
-1.383 |
| H7 |
-0.857 |
-1.648 |
0.036 |
| H8 |
0.412 |
0.101 |
1.429 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5170 | 1.3815 | 2.3335 | 2.3587 | 1.1040 | 1.1036 | 2.1948 |
C2 | 1.5170 | | 2.3606 | 1.3645 | 1.3594 | 2.1479 | 2.1522 | 1.1036 | F3 | 1.3815 | 2.3606 | | 3.5313 | 2.8263 | 2.0397 | 2.0368 | 2.6261 | F4 | 2.3335 | 1.3645 | 3.5313 | | 2.2054 | 2.6361 | 2.5541 | 2.0176 | F5 | 2.3587 | 1.3594 | 2.8263 | 2.2054 | | 2.5642 | 3.2972 | 2.0046 | H6 | 1.1040 | 2.1479 | 2.0397 | 2.6361 | 2.5642 | | 1.8085 | 3.0899 | H7 | 1.1036 | 2.1522 | 2.0368 | 2.5541 | 3.2972 | 1.8085 | | 2.5703 | H8 | 2.1948 | 1.1036 | 2.6261 | 2.0176 | 2.0046 | 3.0899 | 2.5703 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.044 |
|
C1 |
C2 |
F5 |
110.054 |
| C1 |
C2 |
H8 |
112.810 |
|
C2 |
C1 |
F3 |
108.970 |
| C2 |
C1 |
H6 |
109.053 |
|
C2 |
C1 |
H7 |
109.414 |
| F3 |
C1 |
H6 |
109.788 |
|
F3 |
C1 |
H7 |
109.581 |
| F4 |
C2 |
F5 |
108.119 |
|
F4 |
C2 |
H8 |
109.204 |
| F5 |
C2 |
H8 |
108.505 |
|
H6 |
C1 |
H7 |
110.014 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at QCISD/cc-pVDZ
| | hartrees |
| Energy at 0K | -376.663836 |
| Energy at 298.15K | |
| HF Energy | -375.803626 |
| Nuclear repulsion energy | 193.119274 |
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 QCISD/cc-pVDZ
| 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' |
3103 |
2977 |
70.49 |
|
|
|
| 2 |
A' |
3082 |
2957 |
8.67 |
|
|
|
| 3 |
A' |
1497 |
1437 |
7.42 |
|
|
|
| 4 |
A' |
1468 |
1408 |
37.02 |
|
|
|
| 5 |
A' |
1429 |
1371 |
28.26 |
|
|
|
| 6 |
A' |
1212 |
1163 |
109.11 |
|
|
|
| 7 |
A' |
1126 |
1080 |
17.93 |
|
|
|
| 8 |
A' |
895 |
858 |
40.74 |
|
|
|
| 9 |
A' |
766 |
735 |
51.27 |
|
|
|
| 10 |
A' |
523 |
502 |
13.41 |
|
|
|
| 11 |
A' |
233 |
224 |
2.20 |
|
|
|
| 12 |
A" |
3147 |
3019 |
27.96 |
|
|
|
| 13 |
A" |
1423 |
1365 |
42.17 |
|
|
|
| 14 |
A" |
1294 |
1241 |
20.81 |
|
|
|
| 15 |
A" |
1179 |
1131 |
101.36 |
|
|
|
| 16 |
A" |
976 |
937 |
53.93 |
|
|
|
| 17 |
A" |
369 |
354 |
0.04 |
|
|
|
| 18 |
A" |
114 |
110 |
2.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 11917.5 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 11433.7 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 QCISD/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.742 |
-0.833 |
0.000 |
| C2 |
0.357 |
0.633 |
0.000 |
| F3 |
-0.390 |
-1.619 |
0.000 |
| F4 |
-0.390 |
0.922 |
1.100 |
| F5 |
-0.390 |
0.922 |
-1.100 |
| H6 |
1.340 |
-1.050 |
-0.903 |
| H7 |
1.340 |
-1.050 |
0.903 |
| H8 |
1.252 |
1.282 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.5159 | 1.3779 | 2.3605 | 2.3605 | 1.1047 | 1.1047 | 2.1758 |
C2 | 1.5159 | | 2.3721 | 1.3607 | 1.3607 | 2.1481 | 2.1481 | 1.1059 | F3 | 1.3779 | 2.3721 | | 2.7685 | 2.7685 | 2.0330 | 2.0330 | 3.3331 | F4 | 2.3605 | 1.3607 | 2.7685 | | 2.2007 | 3.3006 | 2.6303 | 2.0091 | F5 | 2.3605 | 1.3607 | 2.7685 | 2.2007 | | 2.6303 | 3.3006 | 2.0091 | H6 | 1.1047 | 2.1481 | 2.0330 | 3.3006 | 2.6303 | | 1.8065 | 2.5020 | H7 | 1.1047 | 2.1481 | 2.0330 | 2.6303 | 3.3006 | 1.8065 | | 2.5020 | H8 | 2.1758 | 1.1059 | 3.3331 | 2.0091 | 2.0091 | 2.5020 | 2.5020 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.172 |
|
C1 |
C2 |
F5 |
110.172 |
| C1 |
C2 |
H8 |
111.208 |
|
C2 |
C1 |
F3 |
110.020 |
| C2 |
C1 |
H6 |
109.097 |
|
C2 |
C1 |
H7 |
109.097 |
| F3 |
C1 |
H6 |
109.459 |
|
F3 |
C1 |
H7 |
109.459 |
| F4 |
C2 |
F5 |
107.932 |
|
F4 |
C2 |
H8 |
108.636 |
| F5 |
C2 |
H8 |
108.636 |
|
H6 |
C1 |
H7 |
109.695 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability