Jump to
S1C2
Energy calculated at MP2=FULL/6-31G*
| | hartrees |
| Energy at 0K | -277.531974 |
| Energy at 298.15K | |
| HF Energy | -276.920646 |
| Nuclear repulsion energy | 125.519166 |
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 MP2=FULL/6-31G*
| 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 |
3137 |
2956 |
0.00 |
|
|
|
| 2 |
Ag |
1591 |
1499 |
0.00 |
|
|
|
| 3 |
Ag |
1510 |
1423 |
0.00 |
|
|
|
| 4 |
Ag |
1136 |
1070 |
0.00 |
|
|
|
| 5 |
Ag |
1105 |
1042 |
0.00 |
|
|
|
| 6 |
Ag |
468 |
441 |
0.00 |
|
|
|
| 7 |
Au |
3218 |
3032 |
56.90 |
|
|
|
| 8 |
Au |
1264 |
1191 |
2.93 |
|
|
|
| 9 |
Au |
841 |
792 |
0.10 |
|
|
|
| 10 |
Au |
142 |
134 |
13.04 |
|
|
|
| 11 |
Bg |
3196 |
3011 |
0.00 |
|
|
|
| 12 |
Bg |
1338 |
1261 |
0.00 |
|
|
|
| 13 |
Bg |
1218 |
1147 |
0.00 |
|
|
|
| 14 |
Bu |
3142 |
2960 |
51.67 |
|
|
|
| 15 |
Bu |
1599 |
1507 |
2.00 |
|
|
|
| 16 |
Bu |
1399 |
1318 |
16.87 |
|
|
|
| 17 |
Bu |
1117 |
1052 |
170.73 |
|
|
|
| 18 |
Bu |
279 |
263 |
19.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13849.5 cm
-1
Scaled (by 0.9422) Zero Point Vibrational Energy (zpe) 13049.0 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 MP2=FULL/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.428 |
0.623 |
0.000 |
| C2 |
-0.428 |
-0.623 |
0.000 |
| F3 |
-0.428 |
1.724 |
0.000 |
| F4 |
0.428 |
-1.724 |
0.000 |
| H5 |
1.058 |
0.660 |
0.892 |
| H6 |
1.058 |
0.660 |
-0.892 |
| H7 |
-1.058 |
-0.660 |
0.892 |
| H8 |
-1.058 |
-0.660 |
-0.892 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5110 | 1.3948 | 2.3466 | 1.0924 | 1.0924 | 2.1558 | 2.1558 |
C2 | 1.5110 | | 2.3466 | 1.3948 | 2.1558 | 2.1558 | 1.0924 | 1.0924 | F3 | 1.3948 | 2.3466 | | 3.5526 | 2.0333 | 2.0333 | 2.6220 | 2.6220 | F4 | 2.3466 | 1.3948 | 3.5526 | | 2.6220 | 2.6220 | 2.0333 | 2.0333 | H5 | 1.0924 | 2.1558 | 2.0333 | 2.6220 | | 1.7834 | 2.4935 | 3.0656 | H6 | 1.0924 | 2.1558 | 2.0333 | 2.6220 | 1.7834 | | 3.0656 | 2.4935 | H7 | 2.1558 | 1.0924 | 2.6220 | 2.0333 | 2.4935 | 3.0656 | | 1.7834 | H8 | 2.1558 | 1.0924 | 2.6220 | 2.0333 | 3.0656 | 2.4935 | 1.7834 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.652 |
|
C1 |
C2 |
H7 |
110.777 |
| C1 |
C2 |
H8 |
110.777 |
|
C2 |
C1 |
F3 |
107.652 |
| C2 |
C1 |
H5 |
110.777 |
|
C2 |
C1 |
H6 |
110.777 |
| F3 |
C1 |
H5 |
109.075 |
|
F3 |
C1 |
H6 |
109.075 |
| F4 |
C2 |
H7 |
109.075 |
|
F4 |
C2 |
H8 |
109.075 |
| H5 |
C1 |
H6 |
109.437 |
|
H7 |
C2 |
H8 |
109.437 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2=FULL/6-31G*
| | hartrees |
| Energy at 0K | -277.532315 |
| Energy at 298.15K | |
| HF Energy | -276.919917 |
| Nuclear repulsion energy | 127.913424 |
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 MP2=FULL/6-31G*
| 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 |
3184 |
3000 |
15.82 |
|
|
|
| 2 |
A |
3125 |
2944 |
35.18 |
|
|
|
| 3 |
A |
1571 |
1480 |
0.04 |
|
|
|
| 4 |
A |
1497 |
1411 |
19.83 |
|
|
|
| 5 |
A |
1336 |
1259 |
0.85 |
|
|
|
| 6 |
A |
1181 |
1112 |
0.06 |
|
|
|
| 7 |
A |
1159 |
1092 |
71.75 |
|
|
|
| 8 |
A |
916 |
863 |
25.55 |
|
|
|
| 9 |
A |
334 |
314 |
0.49 |
|
|
|
| 10 |
A |
151 |
142 |
3.32 |
|
|
|
| 11 |
B |
3196 |
3011 |
42.14 |
|
|
|
| 12 |
B |
3116 |
2936 |
13.04 |
|
|
|
| 13 |
B |
1568 |
1478 |
5.12 |
|
|
|
| 14 |
B |
1462 |
1377 |
13.13 |
|
|
|
| 15 |
B |
1291 |
1216 |
3.78 |
|
|
|
| 16 |
B |
1129 |
1064 |
33.33 |
|
|
|
| 17 |
B |
939 |
884 |
34.70 |
|
|
|
| 18 |
B |
510 |
481 |
16.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13831.7 cm
-1
Scaled (by 0.9422) Zero Point Vibrational Energy (zpe) 13032.2 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.
Geometric Data calculated at MP2=FULL/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.265 |
0.702 |
0.524 |
| C2 |
-0.265 |
-0.702 |
0.524 |
| F3 |
-0.265 |
1.399 |
-0.558 |
| F4 |
0.265 |
-1.399 |
-0.558 |
| H5 |
-0.022 |
1.217 |
1.446 |
| H6 |
1.354 |
0.696 |
0.432 |
| H7 |
0.022 |
-1.217 |
1.446 |
| H8 |
-1.354 |
-0.696 |
0.432 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5009 | 1.3920 | 2.3635 | 1.0951 | 1.0931 | 2.1430 | 2.1416 |
C2 | 1.5009 | | 2.3635 | 1.3920 | 2.1430 | 2.1416 | 1.0951 | 1.0931 | F3 | 1.3920 | 2.3635 | | 2.8488 | 2.0273 | 2.0243 | 3.3084 | 2.5609 | F4 | 2.3635 | 1.3920 | 2.8488 | | 3.3084 | 2.5609 | 2.0273 | 2.0243 | H5 | 1.0951 | 2.1430 | 2.0273 | 3.3084 | | 1.7876 | 2.4342 | 2.5423 | H6 | 1.0931 | 2.1416 | 2.0243 | 2.5609 | 1.7876 | | 2.5423 | 3.0457 | H7 | 2.1430 | 1.0951 | 3.3084 | 2.0273 | 2.4342 | 2.5423 | | 1.7876 | H8 | 2.1416 | 1.0931 | 2.5609 | 2.0243 | 2.5423 | 3.0457 | 1.7876 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
109.514 |
|
C1 |
C2 |
H7 |
110.305 |
| C1 |
C2 |
H8 |
110.312 |
|
C2 |
C1 |
F3 |
109.514 |
| C2 |
C1 |
H5 |
110.305 |
|
C2 |
C1 |
H6 |
110.312 |
| F3 |
C1 |
H5 |
108.607 |
|
F3 |
C1 |
H6 |
108.494 |
| F4 |
C2 |
H7 |
108.607 |
|
F4 |
C2 |
H8 |
108.494 |
| H5 |
C1 |
H6 |
109.565 |
|
H7 |
C2 |
H8 |
109.565 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability