Jump to
S1C2
Energy calculated at HF/cc-pVQZ
| | hartrees |
| Energy at 0K | -277.058852 |
| Energy at 298.15K | |
| HF Energy | -277.058852 |
| Nuclear repulsion energy | 127.230888 |
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/cc-pVQZ
| 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 |
3207 |
2913 |
0.00 |
237.63 |
0.06 |
0.10 |
| 2 |
Ag |
1647 |
1496 |
0.00 |
6.04 |
0.75 |
0.86 |
| 3 |
Ag |
1590 |
1444 |
0.00 |
2.47 |
0.31 |
0.47 |
| 4 |
Ag |
1179 |
1071 |
0.00 |
9.04 |
0.73 |
0.84 |
| 5 |
Ag |
1154 |
1048 |
0.00 |
8.42 |
0.15 |
0.25 |
| 6 |
Ag |
497 |
451 |
0.00 |
2.31 |
0.32 |
0.49 |
| 7 |
Au |
3272 |
2972 |
64.25 |
0.00 |
0.34 |
0.51 |
| 8 |
Au |
1351 |
1228 |
8.35 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
874 |
794 |
0.08 |
0.00 |
0.35 |
0.51 |
| 10 |
Au |
137 |
124 |
15.36 |
0.00 |
0.37 |
0.54 |
| 11 |
Bg |
3243 |
2946 |
0.00 |
100.21 |
0.75 |
0.86 |
| 12 |
Bg |
1411 |
1281 |
0.00 |
6.47 |
0.75 |
0.86 |
| 13 |
Bg |
1284 |
1167 |
0.00 |
0.96 |
0.75 |
0.86 |
| 14 |
Bu |
3211 |
2917 |
71.03 |
0.00 |
0.40 |
0.57 |
| 15 |
Bu |
1653 |
1502 |
4.27 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1484 |
1348 |
14.13 |
0.00 |
0.73 |
0.00 |
| 17 |
Bu |
1176 |
1069 |
282.91 |
0.00 |
0.27 |
0.42 |
| 18 |
Bu |
312 |
283 |
22.53 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 14340.0 cm
-1
Scaled (by 0.9084) Zero Point Vibrational Energy (zpe) 13026.5 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/cc-pVQZ
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 |
1.701 |
0.000 |
| F4 |
0.419 |
-1.701 |
0.000 |
| H5 |
1.042 |
0.677 |
0.882 |
| H6 |
1.042 |
0.677 |
-0.882 |
| H7 |
-1.042 |
-0.677 |
0.882 |
| H8 |
-1.042 |
-0.677 |
-0.882 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5116 | 1.3616 | 2.3301 | 1.0807 | 1.0807 | 2.1493 | 2.1493 |
C2 | 1.5116 | | 2.3301 | 1.3616 | 2.1493 | 2.1493 | 1.0807 | 1.0807 | F3 | 1.3616 | 2.3301 | | 3.5046 | 1.9907 | 1.9907 | 2.6121 | 2.6121 | F4 | 2.3301 | 1.3616 | 3.5046 | | 2.6121 | 2.6121 | 1.9907 | 1.9907 | H5 | 1.0807 | 2.1493 | 1.9907 | 2.6121 | | 1.7635 | 2.4860 | 3.0479 | H6 | 1.0807 | 2.1493 | 1.9907 | 2.6121 | 1.7635 | | 3.0479 | 2.4860 | H7 | 2.1493 | 1.0807 | 2.6121 | 1.9907 | 2.4860 | 3.0479 | | 1.7635 | H8 | 2.1493 | 1.0807 | 2.6121 | 1.9907 | 3.0479 | 2.4860 | 1.7635 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.273 |
|
C1 |
C2 |
H7 |
110.925 |
| C1 |
C2 |
H8 |
110.925 |
|
C2 |
C1 |
F3 |
108.273 |
| C2 |
C1 |
H5 |
110.925 |
|
C2 |
C1 |
H6 |
110.925 |
| F3 |
C1 |
H5 |
108.650 |
|
F3 |
C1 |
H6 |
108.650 |
| F4 |
C2 |
H7 |
108.650 |
|
F4 |
C2 |
H8 |
108.650 |
| H5 |
C1 |
H6 |
109.355 |
|
H7 |
C2 |
H8 |
109.355 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.067 |
|
|
|
| 2 |
C |
0.067 |
|
|
|
| 3 |
F |
-0.701 |
|
|
|
| 4 |
F |
-0.701 |
|
|
|
| 5 |
H |
0.317 |
|
|
|
| 6 |
H |
0.317 |
|
|
|
| 7 |
H |
0.317 |
|
|
|
| 8 |
H |
0.317 |
|
|
|
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 |
-22.037 |
3.412 |
0.000 |
| y |
3.412 |
-29.574 |
0.000 |
| z |
0.000 |
0.000 |
-21.309 |
|
| Traceless |
| | x | y | z |
| x |
3.405 |
3.412 |
0.000 |
| y |
3.412 |
-7.901 |
0.000 |
| z |
0.000 |
0.000 |
4.496 |
|
| Polar |
| 3z2-r2 | 8.993 |
| x2-y2 | 7.537 |
| xy | 3.412 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.982 |
-0.012 |
0.000 |
| y |
-0.012 |
4.115 |
0.000 |
| z |
0.000 |
0.000 |
3.710 |
<r2> (average value of r
2) Å
2
| <r2> |
86.596 |
| (<r2>)1/2 |
9.306 |
Jump to
S1C1
Energy calculated at HF/cc-pVQZ
| | hartrees |
| Energy at 0K | -277.059425 |
| Energy at 298.15K | |
| HF Energy | -277.059425 |
| Nuclear repulsion energy | 129.312699 |
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/cc-pVQZ
| 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 |
3240 |
2944 |
21.49 |
76.91 |
0.74 |
0.85 |
| 2 |
A |
3203 |
2910 |
45.76 |
217.02 |
0.02 |
0.04 |
| 3 |
A |
1624 |
1475 |
0.71 |
1.14 |
0.75 |
0.86 |
| 4 |
A |
1580 |
1435 |
14.47 |
1.40 |
0.06 |
0.11 |
| 5 |
A |
1417 |
1287 |
5.68 |
7.17 |
0.66 |
0.80 |
| 6 |
A |
1235 |
1122 |
34.99 |
1.87 |
0.08 |
0.16 |
| 7 |
A |
1216 |
1105 |
88.68 |
3.61 |
0.74 |
0.85 |
| 8 |
A |
938 |
853 |
28.13 |
7.27 |
0.14 |
0.24 |
| 9 |
A |
347 |
316 |
0.29 |
0.30 |
0.27 |
0.42 |
| 10 |
A |
160 |
146 |
4.34 |
0.07 |
0.75 |
0.86 |
| 11 |
B |
3255 |
2957 |
52.46 |
9.92 |
0.75 |
0.86 |
| 12 |
B |
3189 |
2897 |
12.11 |
31.88 |
0.75 |
0.86 |
| 13 |
B |
1621 |
1473 |
7.54 |
5.30 |
0.75 |
0.86 |
| 14 |
B |
1533 |
1393 |
11.80 |
0.01 |
0.75 |
0.86 |
| 15 |
B |
1378 |
1252 |
10.78 |
1.95 |
0.75 |
0.86 |
| 16 |
B |
1196 |
1087 |
63.97 |
3.69 |
0.75 |
0.86 |
| 17 |
B |
989 |
898 |
55.74 |
2.29 |
0.75 |
0.86 |
| 18 |
B |
543 |
493 |
20.46 |
0.37 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 14332.3 cm
-1
Scaled (by 0.9084) Zero Point Vibrational Energy (zpe) 13019.5 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/cc-pVQZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.260 |
0.705 |
0.503 |
| C2 |
-0.260 |
-0.705 |
0.503 |
| F3 |
-0.260 |
1.406 |
-0.539 |
| F4 |
0.260 |
-1.406 |
-0.539 |
| H5 |
-0.031 |
1.199 |
1.422 |
| H6 |
1.337 |
0.714 |
0.413 |
| H7 |
0.031 |
-1.199 |
1.422 |
| H8 |
-1.337 |
-0.714 |
0.413 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5021 | 1.3599 | 2.3540 | 1.0826 | 1.0811 | 2.1258 | 2.1383 |
C2 | 1.5021 | | 2.3540 | 1.3599 | 2.1258 | 2.1383 | 1.0826 | 1.0811 | F3 | 1.3599 | 2.3540 | | 2.8593 | 1.9855 | 1.9838 | 3.2733 | 2.5614 | F4 | 2.3540 | 1.3599 | 2.8593 | | 3.2733 | 2.5614 | 1.9855 | 1.9838 | H5 | 1.0826 | 2.1258 | 1.9855 | 3.2733 | | 1.7676 | 2.3982 | 2.5268 | H6 | 1.0811 | 2.1383 | 1.9838 | 2.5614 | 1.7676 | | 2.5268 | 3.0319 | H7 | 2.1258 | 1.0826 | 3.2733 | 1.9855 | 2.3982 | 2.5268 | | 1.7676 | H8 | 2.1383 | 1.0811 | 2.5614 | 1.9838 | 2.5268 | 3.0319 | 1.7676 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.572 |
|
C1 |
C2 |
H7 |
109.587 |
| C1 |
C2 |
H8 |
110.679 |
|
C2 |
C1 |
F3 |
110.572 |
| C2 |
C1 |
H5 |
109.587 |
|
C2 |
C1 |
H6 |
110.679 |
| F3 |
C1 |
H5 |
108.220 |
|
F3 |
C1 |
H6 |
108.178 |
| F4 |
C2 |
H7 |
108.220 |
|
F4 |
C2 |
H8 |
108.178 |
| H5 |
C1 |
H6 |
109.554 |
|
H7 |
C2 |
H8 |
109.554 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.064 |
|
|
|
| 2 |
C |
0.064 |
|
|
|
| 3 |
F |
-0.685 |
|
|
|
| 4 |
F |
-0.685 |
|
|
|
| 5 |
H |
0.314 |
|
|
|
| 6 |
H |
0.306 |
|
|
|
| 7 |
H |
0.314 |
|
|
|
| 8 |
H |
0.306 |
|
|
|
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 |
2.882 |
2.882 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.567 |
1.800 |
0.000 |
| y |
1.800 |
-26.227 |
0.000 |
| z |
0.000 |
0.000 |
-22.418 |
|
| Traceless |
| | x | y | z |
| x |
2.756 |
1.800 |
0.000 |
| y |
1.800 |
-4.234 |
0.000 |
| z |
0.000 |
0.000 |
1.479 |
|
| Polar |
| 3z2-r2 | 2.958 |
| x2-y2 | 4.660 |
| xy | 1.800 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.818 |
0.037 |
0.000 |
| y |
0.037 |
4.081 |
0.000 |
| z |
0.000 |
0.000 |
3.941 |
<r2> (average value of r
2) Å
2
| <r2> |
78.310 |
| (<r2>)1/2 |
8.849 |