Jump to
S1C2
Energy calculated at HF/6-31G
| | hartrees |
| Energy at 0K | -276.840964 |
| Energy at 298.15K | |
| HF Energy | -276.840964 |
| Nuclear repulsion energy | 124.924868 |
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/6-31G
| 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 |
3286 |
2967 |
0.00 |
202.13 |
0.10 |
0.18 |
| 2 |
Ag |
1686 |
1522 |
0.00 |
22.23 |
0.75 |
0.85 |
| 3 |
Ag |
1587 |
1433 |
0.00 |
3.18 |
0.70 |
0.83 |
| 4 |
Ag |
1186 |
1071 |
0.00 |
12.96 |
0.50 |
0.67 |
| 5 |
Ag |
1104 |
997 |
0.00 |
14.38 |
0.43 |
0.60 |
| 6 |
Ag |
479 |
433 |
0.00 |
3.83 |
0.47 |
0.64 |
| 7 |
Au |
3368 |
3041 |
47.74 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1322 |
1194 |
6.71 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
909 |
820 |
0.04 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
133 |
120 |
26.11 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3343 |
3018 |
0.00 |
118.70 |
0.75 |
0.86 |
| 12 |
Bg |
1428 |
1290 |
0.00 |
17.67 |
0.75 |
0.86 |
| 13 |
Bg |
1263 |
1140 |
0.00 |
10.46 |
0.75 |
0.86 |
| 14 |
Bu |
3291 |
2971 |
38.28 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1694 |
1530 |
3.41 |
0.00 |
0.45 |
0.62 |
| 16 |
Bu |
1493 |
1348 |
11.74 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
1115 |
1007 |
196.98 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
296 |
267 |
35.98 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 14491.4 cm
-1
Scaled (by 0.9029) Zero Point Vibrational Energy (zpe) 13084.3 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/6-31G
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.435 |
0.615 |
0.000 |
| C2 |
-0.435 |
-0.615 |
0.000 |
| F3 |
-0.435 |
1.735 |
0.000 |
| F4 |
0.435 |
-1.735 |
0.000 |
| H5 |
1.048 |
0.671 |
0.883 |
| H6 |
1.048 |
0.671 |
-0.883 |
| H7 |
-1.048 |
-0.671 |
0.883 |
| H8 |
-1.048 |
-0.671 |
-0.883 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5071 | 1.4186 | 2.3498 | 1.0763 | 1.0763 | 2.1527 | 2.1527 |
C2 | 1.5071 | | 2.3498 | 1.4186 | 2.1527 | 2.1527 | 1.0763 | 1.0763 | F3 | 1.4186 | 2.3498 | | 3.5773 | 2.0283 | 2.0283 | 2.6346 | 2.6346 | F4 | 2.3498 | 1.4186 | 3.5773 | | 2.6346 | 2.6346 | 2.0283 | 2.0283 | H5 | 1.0763 | 2.1527 | 2.0283 | 2.6346 | | 1.7658 | 2.4891 | 3.0519 | H6 | 1.0763 | 2.1527 | 2.0283 | 2.6346 | 1.7658 | | 3.0519 | 2.4891 | H7 | 2.1527 | 1.0763 | 2.6346 | 2.0283 | 2.4891 | 3.0519 | | 1.7658 | H8 | 2.1527 | 1.0763 | 2.6346 | 2.0283 | 3.0519 | 2.4891 | 1.7658 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
106.830 |
|
C1 |
C2 |
H7 |
111.793 |
| C1 |
C2 |
H8 |
111.793 |
|
C2 |
C1 |
F3 |
106.830 |
| C2 |
C1 |
H5 |
111.793 |
|
C2 |
C1 |
H6 |
111.793 |
| F3 |
C1 |
H5 |
107.993 |
|
F3 |
C1 |
H6 |
107.993 |
| F4 |
C2 |
H7 |
107.993 |
|
F4 |
C2 |
H8 |
107.993 |
| H5 |
C1 |
H6 |
110.232 |
|
H7 |
C2 |
H8 |
110.232 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.087 |
|
|
|
| 2 |
C |
0.087 |
|
|
|
| 3 |
F |
-0.462 |
|
|
|
| 4 |
F |
-0.462 |
|
|
|
| 5 |
H |
0.188 |
|
|
|
| 6 |
H |
0.188 |
|
|
|
| 7 |
H |
0.188 |
|
|
|
| 8 |
H |
0.188 |
|
|
|
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 |
-21.688 |
4.347 |
0.000 |
| y |
4.347 |
-32.036 |
0.000 |
| z |
0.000 |
0.000 |
-21.183 |
|
| Traceless |
| | x | y | z |
| x |
4.922 |
4.347 |
0.000 |
| y |
4.347 |
-10.601 |
0.000 |
| z |
0.000 |
0.000 |
5.679 |
|
| Polar |
| 3z2-r2 | 11.358 |
| x2-y2 | 10.349 |
| xy | 4.347 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.083 |
-0.139 |
0.000 |
| y |
-0.139 |
3.101 |
0.000 |
| z |
0.000 |
0.000 |
2.917 |
<r2> (average value of r
2) Å
2
| <r2> |
89.309 |
| (<r2>)1/2 |
9.450 |
Jump to
S1C1
Energy calculated at HF/6-31G
| | hartrees |
| Energy at 0K | -276.839397 |
| Energy at 298.15K | |
| HF Energy | -276.839397 |
| Nuclear repulsion energy | 126.931924 |
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/6-31G
| 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 |
3334 |
3010 |
14.57 |
95.97 |
0.72 |
0.84 |
| 2 |
A |
3276 |
2958 |
26.60 |
165.76 |
0.02 |
0.04 |
| 3 |
A |
1664 |
1503 |
0.74 |
3.85 |
0.75 |
0.86 |
| 4 |
A |
1572 |
1420 |
13.50 |
2.69 |
0.64 |
0.78 |
| 5 |
A |
1408 |
1271 |
1.92 |
23.46 |
0.73 |
0.84 |
| 6 |
A |
1227 |
1108 |
2.81 |
4.33 |
0.39 |
0.56 |
| 7 |
A |
1190 |
1074 |
59.50 |
7.31 |
0.69 |
0.82 |
| 8 |
A |
939 |
848 |
42.08 |
9.12 |
0.14 |
0.25 |
| 9 |
A |
348 |
315 |
0.80 |
0.41 |
0.34 |
0.51 |
| 10 |
A |
142 |
128 |
8.28 |
0.12 |
0.70 |
0.82 |
| 11 |
B |
3346 |
3021 |
29.42 |
12.92 |
0.75 |
0.86 |
| 12 |
B |
3263 |
2946 |
11.81 |
44.64 |
0.75 |
0.86 |
| 13 |
B |
1667 |
1505 |
5.54 |
16.85 |
0.75 |
0.86 |
| 14 |
B |
1559 |
1408 |
11.18 |
0.90 |
0.75 |
0.86 |
| 15 |
B |
1352 |
1221 |
5.97 |
6.88 |
0.75 |
0.86 |
| 16 |
B |
1159 |
1047 |
27.73 |
4.39 |
0.75 |
0.86 |
| 17 |
B |
985 |
889 |
59.06 |
6.49 |
0.75 |
0.86 |
| 18 |
B |
521 |
471 |
28.43 |
0.85 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 14476.2 cm
-1
Scaled (by 0.9029) Zero Point Vibrational Energy (zpe) 13070.6 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 HF/6-31G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.285 |
0.692 |
0.516 |
| C2 |
-0.285 |
-0.692 |
0.516 |
| F3 |
-0.285 |
1.437 |
-0.544 |
| F4 |
0.285 |
-1.437 |
-0.544 |
| H5 |
0.044 |
1.208 |
1.432 |
| H6 |
1.351 |
0.676 |
0.365 |
| H7 |
-0.044 |
-1.208 |
1.432 |
| H8 |
-1.351 |
-0.676 |
0.365 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4974 | 1.4160 | 2.3788 | 1.0787 | 1.0768 | 2.1349 | 2.1386 |
C2 | 1.4974 | | 2.3788 | 1.4160 | 2.1349 | 2.1386 | 1.0787 | 1.0768 | F3 | 1.4160 | 2.3788 | | 2.9309 | 2.0167 | 2.0213 | 3.3108 | 2.5354 | F4 | 2.3788 | 1.4160 | 2.9309 | | 3.3108 | 2.5354 | 2.0167 | 2.0213 | H5 | 1.0787 | 2.1349 | 2.0167 | 3.3108 | | 1.7696 | 2.4173 | 2.5758 | H6 | 1.0768 | 2.1386 | 2.0213 | 2.5354 | 1.7696 | | 2.5758 | 3.0220 | H7 | 2.1349 | 1.0787 | 3.3108 | 2.0167 | 2.4173 | 2.5758 | | 1.7696 | H8 | 2.1386 | 1.0768 | 2.5354 | 2.0213 | 2.5758 | 3.0220 | 1.7696 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
109.443 |
|
C1 |
C2 |
H7 |
110.896 |
| C1 |
C2 |
H8 |
111.306 |
|
C2 |
C1 |
F3 |
109.443 |
| C2 |
C1 |
H5 |
110.896 |
|
C2 |
C1 |
H6 |
111.306 |
| F3 |
C1 |
H5 |
107.105 |
|
F3 |
C1 |
H6 |
107.581 |
| F4 |
C2 |
H7 |
107.105 |
|
F4 |
C2 |
H8 |
107.581 |
| H5 |
C1 |
H6 |
110.359 |
|
H7 |
C2 |
H8 |
110.359 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.090 |
|
|
|
| 2 |
C |
0.090 |
|
|
|
| 3 |
F |
-0.454 |
|
|
|
| 4 |
F |
-0.454 |
|
|
|
| 5 |
H |
0.169 |
|
|
|
| 6 |
H |
0.195 |
|
|
|
| 7 |
H |
0.169 |
|
|
|
| 8 |
H |
0.195 |
|
|
|
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 |
3.774 |
3.774 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.321 |
2.511 |
0.000 |
| y |
2.511 |
-27.695 |
0.000 |
| z |
0.000 |
0.000 |
-22.262 |
|
| Traceless |
| | x | y | z |
| x |
3.658 |
2.511 |
0.000 |
| y |
2.511 |
-5.903 |
0.000 |
| z |
0.000 |
0.000 |
2.246 |
|
| Polar |
| 3z2-r2 | 4.491 |
| x2-y2 | 6.374 |
| xy | 2.511 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.977 |
-0.072 |
0.000 |
| y |
-0.072 |
3.064 |
0.000 |
| z |
0.000 |
0.000 |
3.132 |
<r2> (average value of r
2) Å
2
| <r2> |
80.604 |
| (<r2>)1/2 |
8.978 |