Jump to
S1C2
Energy calculated at G4
| | hartrees |
| Energy at 0K | -278.177771 |
| Energy at 298.15K | -278.172350 |
| HF Energy | -278.296146 |
| Nuclear repulsion energy | 125.849980 |
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/6-31G(2df,p)
| 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 |
3031 |
2924 |
0.00 |
|
|
|
| 2 |
Ag |
1518 |
1465 |
0.00 |
|
|
|
| 3 |
Ag |
1458 |
1407 |
0.00 |
|
|
|
| 4 |
Ag |
1096 |
1057 |
0.00 |
|
|
|
| 5 |
Ag |
1076 |
1038 |
0.00 |
|
|
|
| 6 |
Ag |
461 |
445 |
0.00 |
|
|
|
| 7 |
Au |
3097 |
2989 |
69.41 |
|
|
|
| 8 |
Au |
1238 |
1195 |
3.69 |
|
|
|
| 9 |
Au |
812 |
784 |
0.05 |
|
|
|
| 10 |
Au |
124 |
120 |
9.92 |
|
|
|
| 11 |
Bg |
3070 |
2963 |
0.00 |
|
|
|
| 12 |
Bg |
1298 |
1253 |
0.00 |
|
|
|
| 13 |
Bg |
1189 |
1148 |
0.00 |
|
|
|
| 14 |
Bu |
3037 |
2930 |
67.20 |
|
|
|
| 15 |
Bu |
1530 |
1476 |
1.96 |
|
|
|
| 16 |
Bu |
1373 |
1325 |
14.90 |
|
|
|
| 17 |
Bu |
1106 |
1068 |
179.45 |
|
|
|
| 18 |
Bu |
273 |
264 |
14.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13393.6 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 12924.9 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/6-31G(2df,p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.422 |
0.633 |
0.000 |
| C2 |
-0.422 |
-0.633 |
0.000 |
| F3 |
-0.422 |
1.722 |
0.000 |
| F4 |
0.422 |
-1.722 |
0.000 |
| H5 |
1.059 |
0.668 |
0.891 |
| H6 |
1.059 |
0.668 |
-0.891 |
| H7 |
-1.059 |
-0.668 |
0.891 |
| H8 |
-1.059 |
-0.668 |
-0.891 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5220 | 1.3770 | 2.3549 | 1.0964 | 1.0964 | 2.1636 | 2.1636 |
C2 | 1.5220 | | 2.3549 | 1.3770 | 2.1636 | 2.1636 | 1.0964 | 1.0964 | F3 | 1.3770 | 2.3549 | | 3.5449 | 2.0248 | 2.0248 | 2.6284 | 2.6284 | F4 | 2.3549 | 1.3770 | 3.5449 | | 2.6284 | 2.6284 | 2.0248 | 2.0248 | H5 | 1.0964 | 2.1636 | 2.0248 | 2.6284 | | 1.7827 | 2.5044 | 3.0741 | H6 | 1.0964 | 2.1636 | 2.0248 | 2.6284 | 1.7827 | | 3.0741 | 2.5044 | H7 | 2.1636 | 1.0964 | 2.6284 | 2.0248 | 2.5044 | 3.0741 | | 1.7827 | H8 | 2.1636 | 1.0964 | 2.6284 | 2.0248 | 3.0741 | 2.5044 | 1.7827 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.847 |
|
C1 |
C2 |
H7 |
110.144 |
| C1 |
C2 |
H8 |
110.144 |
|
C2 |
C1 |
F3 |
108.847 |
| C2 |
C1 |
H5 |
110.144 |
|
C2 |
C1 |
H6 |
110.144 |
| F3 |
C1 |
H5 |
109.474 |
|
F3 |
C1 |
H6 |
109.474 |
| F4 |
C2 |
H7 |
109.474 |
|
F4 |
C2 |
H8 |
109.474 |
| H5 |
C1 |
H6 |
108.747 |
|
H7 |
C2 |
H8 |
108.747 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.081 |
|
|
|
| 2 |
C |
-0.081 |
|
|
|
| 3 |
F |
-0.149 |
|
|
|
| 4 |
F |
-0.149 |
|
|
|
| 5 |
H |
0.115 |
|
|
|
| 6 |
H |
0.115 |
|
|
|
| 7 |
H |
0.115 |
|
|
|
| 8 |
H |
0.115 |
|
|
|
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
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
87.710 |
| (<r2>)1/2 |
9.365 |
Jump to
S1C1
Energy calculated at G4
| | hartrees |
| Energy at 0K | -6576.526703 |
| Energy at 298.15K | -6576.521394 |
| HF Energy | -278.297330 |
| Nuclear repulsion energy | 128.111992 |
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/6-31G(2df,p)
| 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 |
3065 |
2958 |
23.99 |
90.99 |
0.75 |
0.86 |
| 2 |
A |
3025 |
2919 |
37.03 |
167.77 |
0.03 |
0.06 |
| 3 |
A |
1500 |
1448 |
0.65 |
2.15 |
0.59 |
0.75 |
| 4 |
A |
1443 |
1393 |
13.82 |
4.19 |
0.69 |
0.81 |
| 5 |
A |
1306 |
1260 |
1.99 |
17.01 |
0.71 |
0.83 |
| 6 |
A |
1146 |
1106 |
30.72 |
1.57 |
0.17 |
0.29 |
| 7 |
A |
1123 |
1084 |
54.59 |
3.28 |
0.74 |
0.85 |
| 8 |
A |
879 |
849 |
17.37 |
6.25 |
0.25 |
0.39 |
| 9 |
A |
319 |
308 |
0.29 |
0.21 |
0.34 |
0.51 |
| 10 |
A |
144 |
139 |
2.68 |
0.03 |
0.75 |
0.86 |
| 11 |
B |
3079 |
2971 |
53.40 |
13.09 |
0.75 |
0.86 |
| 12 |
B |
3014 |
2909 |
15.57 |
36.63 |
0.75 |
0.86 |
| 13 |
B |
1495 |
1443 |
7.35 |
12.81 |
0.75 |
0.86 |
| 14 |
B |
1419 |
1369 |
10.49 |
1.37 |
0.75 |
0.86 |
| 15 |
B |
1268 |
1224 |
5.63 |
4.72 |
0.75 |
0.86 |
| 16 |
B |
1109 |
1070 |
40.38 |
2.74 |
0.75 |
0.86 |
| 17 |
B |
914 |
882 |
33.84 |
3.29 |
0.75 |
0.86 |
| 18 |
B |
494 |
477 |
12.89 |
0.44 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13370.9 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 12902.9 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/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.260 |
0.709 |
0.513 |
| C2 |
-0.260 |
-0.709 |
0.513 |
| F3 |
-0.260 |
1.408 |
-0.551 |
| F4 |
0.260 |
-1.408 |
-0.551 |
| H5 |
-0.031 |
1.208 |
1.448 |
| H6 |
1.354 |
0.708 |
0.435 |
| H7 |
0.031 |
-1.208 |
1.448 |
| H8 |
-1.354 |
-0.708 |
0.435 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5109 | 1.3757 | 2.3703 | 1.0983 | 1.0971 | 2.1451 | 2.1496 |
C2 | 1.5109 | | 2.3703 | 1.3757 | 2.1451 | 2.1496 | 1.0983 | 1.0971 | F3 | 1.3757 | 2.3703 | | 2.8644 | 2.0222 | 2.0171 | 3.3055 | 2.5787 | F4 | 2.3703 | 1.3757 | 2.8644 | | 3.3055 | 2.5787 | 2.0222 | 2.0171 | H5 | 1.0983 | 2.1451 | 2.0222 | 3.3055 | | 1.7871 | 2.4165 | 2.5395 | H6 | 1.0971 | 2.1496 | 2.0171 | 2.5787 | 1.7871 | | 2.5395 | 3.0564 | H7 | 2.1451 | 1.0983 | 3.3055 | 2.0222 | 2.4165 | 2.5395 | | 1.7871 | H8 | 2.1496 | 1.0971 | 2.5787 | 2.0171 | 2.5395 | 3.0564 | 1.7871 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.319 |
|
C1 |
C2 |
H7 |
109.590 |
| C1 |
C2 |
H8 |
109.998 |
|
C2 |
C1 |
F3 |
110.319 |
| C2 |
C1 |
H5 |
109.590 |
|
C2 |
C1 |
H6 |
109.998 |
| F3 |
C1 |
H5 |
109.143 |
|
F3 |
C1 |
H6 |
108.790 |
| F4 |
C2 |
H7 |
109.143 |
|
F4 |
C2 |
H8 |
108.790 |
| H5 |
C1 |
H6 |
108.972 |
|
H7 |
C2 |
H8 |
108.972 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.066 |
|
|
|
| 2 |
C |
-0.066 |
|
|
|
| 3 |
F |
-0.153 |
|
|
|
| 4 |
F |
-0.153 |
|
|
|
| 5 |
H |
0.103 |
|
|
|
| 6 |
H |
0.116 |
|
|
|
| 7 |
H |
0.103 |
|
|
|
| 8 |
H |
0.116 |
|
|
|
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 |
2.328 |
2.328 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
78.869 |
| (<r2>)1/2 |
8.881 |