Jump to
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -278.190909 |
| Energy at 298.15K | |
| HF Energy | -278.190909 |
| Nuclear repulsion energy | 126.044340 |
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 B1B95/6-31G*
| 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 |
3080 |
2924 |
0.00 |
|
|
|
| 2 |
Ag |
1547 |
1469 |
0.00 |
|
|
|
| 3 |
Ag |
1482 |
1407 |
0.00 |
|
|
|
| 4 |
Ag |
1116 |
1059 |
0.00 |
|
|
|
| 5 |
Ag |
1101 |
1045 |
0.00 |
|
|
|
| 6 |
Ag |
462 |
439 |
0.00 |
|
|
|
| 7 |
Au |
3151 |
2991 |
72.85 |
|
|
|
| 8 |
Au |
1246 |
1183 |
2.79 |
|
|
|
| 9 |
Au |
820 |
779 |
0.03 |
|
|
|
| 10 |
Au |
134 |
127 |
11.26 |
|
|
|
| 11 |
Bg |
3125 |
2967 |
0.00 |
|
|
|
| 12 |
Bg |
1311 |
1245 |
0.00 |
|
|
|
| 13 |
Bg |
1194 |
1134 |
0.00 |
|
|
|
| 14 |
Bu |
3086 |
2929 |
67.37 |
|
|
|
| 15 |
Bu |
1558 |
1479 |
2.35 |
|
|
|
| 16 |
Bu |
1378 |
1308 |
19.13 |
|
|
|
| 17 |
Bu |
1131 |
1073 |
185.60 |
|
|
|
| 18 |
Bu |
268 |
254 |
17.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13594.8 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 12905.6 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 B1B95/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.422 |
0.628 |
0.000 |
| C2 |
-0.422 |
-0.628 |
0.000 |
| F3 |
-0.422 |
1.718 |
0.000 |
| F4 |
0.422 |
-1.718 |
0.000 |
| H5 |
1.058 |
0.662 |
0.890 |
| H6 |
1.058 |
0.662 |
-0.890 |
| H7 |
-1.058 |
-0.662 |
0.890 |
| H8 |
-1.058 |
-0.662 |
-0.890 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5136 | 1.3791 | 2.3461 | 1.0943 | 1.0943 | 2.1556 | 2.1556 |
C2 | 1.5136 | | 2.3461 | 1.3791 | 2.1556 | 2.1556 | 1.0943 | 1.0943 | F3 | 1.3791 | 2.3461 | | 3.5385 | 2.0245 | 2.0245 | 2.6193 | 2.6193 | F4 | 2.3461 | 1.3791 | 3.5385 | | 2.6193 | 2.6193 | 2.0245 | 2.0245 | H5 | 1.0943 | 2.1556 | 2.0245 | 2.6193 | | 1.7809 | 2.4951 | 3.0655 | H6 | 1.0943 | 2.1556 | 2.0245 | 2.6193 | 1.7809 | | 3.0655 | 2.4951 | H7 | 2.1556 | 1.0943 | 2.6193 | 2.0245 | 2.4951 | 3.0655 | | 1.7809 | H8 | 2.1556 | 1.0943 | 2.6193 | 2.0245 | 3.0655 | 2.4951 | 1.7809 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
108.305 |
|
C1 |
C2 |
H7 |
110.466 |
| C1 |
C2 |
H8 |
110.466 |
|
C2 |
C1 |
F3 |
108.305 |
| C2 |
C1 |
H5 |
110.466 |
|
C2 |
C1 |
H6 |
110.466 |
| F3 |
C1 |
H5 |
109.331 |
|
F3 |
C1 |
H6 |
109.331 |
| F4 |
C2 |
H7 |
109.331 |
|
F4 |
C2 |
H8 |
109.331 |
| H5 |
C1 |
H6 |
108.922 |
|
H7 |
C2 |
H8 |
108.922 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.015 |
|
|
|
| 2 |
C |
-0.015 |
|
|
|
| 3 |
F |
-0.310 |
|
|
|
| 4 |
F |
-0.310 |
|
|
|
| 5 |
H |
0.163 |
|
|
|
| 6 |
H |
0.163 |
|
|
|
| 7 |
H |
0.163 |
|
|
|
| 8 |
H |
0.163 |
|
|
|
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 |
-21.525 |
2.502 |
0.000 |
| y |
2.502 |
-27.920 |
0.000 |
| z |
0.000 |
0.000 |
-21.207 |
|
| Traceless |
| | x | y | z |
| x |
3.038 |
2.502 |
0.000 |
| y |
2.502 |
-6.554 |
0.000 |
| z |
0.000 |
0.000 |
3.516 |
|
| Polar |
| 3z2-r2 | 7.032 |
| x2-y2 | 6.395 |
| xy | 2.502 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.510 |
0.039 |
0.000 |
| y |
0.039 |
3.436 |
0.000 |
| z |
0.000 |
0.000 |
3.381 |
<r2> (average value of r
2) Å
2
| <r2> |
87.325 |
| (<r2>)1/2 |
9.345 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -278.191570 |
| Energy at 298.15K | |
| HF Energy | -278.191570 |
| Nuclear repulsion energy | 128.240105 |
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 B1B95/6-31G*
| 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 |
3116 |
2958 |
22.06 |
|
|
|
| 2 |
A |
3071 |
2916 |
40.18 |
|
|
|
| 3 |
A |
1527 |
1449 |
0.73 |
|
|
|
| 4 |
A |
1466 |
1391 |
21.01 |
|
|
|
| 5 |
A |
1317 |
1251 |
1.62 |
|
|
|
| 6 |
A |
1160 |
1102 |
61.73 |
|
|
|
| 7 |
A |
1144 |
1086 |
23.52 |
|
|
|
| 8 |
A |
896 |
850 |
19.73 |
|
|
|
| 9 |
A |
321 |
305 |
0.38 |
|
|
|
| 10 |
A |
147 |
139 |
2.98 |
|
|
|
| 11 |
B |
3130 |
2972 |
55.18 |
|
|
|
| 12 |
B |
3060 |
2904 |
15.96 |
|
|
|
| 13 |
B |
1523 |
1446 |
7.03 |
|
|
|
| 14 |
B |
1431 |
1358 |
14.88 |
|
|
|
| 15 |
B |
1274 |
1210 |
4.74 |
|
|
|
| 16 |
B |
1130 |
1073 |
44.40 |
|
|
|
| 17 |
B |
924 |
877 |
32.24 |
|
|
|
| 18 |
B |
492 |
467 |
14.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13564.5 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 12876.8 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 B1B95/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.262 |
0.704 |
0.511 |
| C2 |
-0.262 |
-0.704 |
0.511 |
| F3 |
-0.262 |
1.410 |
-0.549 |
| F4 |
0.262 |
-1.410 |
-0.549 |
| H5 |
-0.021 |
1.204 |
1.445 |
| H6 |
1.354 |
0.699 |
0.426 |
| H7 |
0.021 |
-1.204 |
1.445 |
| H8 |
-1.354 |
-0.699 |
0.426 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5028 | 1.3774 | 2.3654 | 1.0965 | 1.0949 | 2.1379 | 2.1414 |
C2 | 1.5028 | | 2.3654 | 1.3774 | 2.1379 | 2.1414 | 1.0965 | 1.0949 | F3 | 1.3774 | 2.3654 | | 2.8687 | 2.0194 | 2.0166 | 3.3001 | 2.5671 | F4 | 2.3654 | 1.3774 | 2.8687 | | 3.3001 | 2.5671 | 2.0194 | 2.0166 | H5 | 1.0965 | 2.1379 | 2.0194 | 3.3001 | | 1.7845 | 2.4079 | 2.5364 | H6 | 1.0949 | 2.1414 | 2.0166 | 2.5671 | 1.7845 | | 2.5364 | 3.0466 | H7 | 2.1379 | 1.0965 | 3.3001 | 2.0194 | 2.4079 | 2.5364 | | 1.7845 | H8 | 2.1414 | 1.0949 | 2.5671 | 2.0166 | 2.5364 | 3.0466 | 1.7845 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.349 |
|
C1 |
C2 |
H7 |
109.685 |
| C1 |
C2 |
H8 |
110.057 |
|
C2 |
C1 |
F3 |
110.349 |
| C2 |
C1 |
H5 |
109.685 |
|
C2 |
C1 |
H6 |
110.057 |
| F3 |
C1 |
H5 |
108.901 |
|
F3 |
C1 |
H6 |
108.776 |
| F4 |
C2 |
H7 |
108.901 |
|
F4 |
C2 |
H8 |
108.776 |
| H5 |
C1 |
H6 |
109.041 |
|
H7 |
C2 |
H8 |
109.041 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.006 |
|
|
|
| 2 |
C |
-0.006 |
|
|
|
| 3 |
F |
-0.306 |
|
|
|
| 4 |
F |
-0.306 |
|
|
|
| 5 |
H |
0.147 |
|
|
|
| 6 |
H |
0.165 |
|
|
|
| 7 |
H |
0.147 |
|
|
|
| 8 |
H |
0.165 |
|
|
|
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 |
2.453 |
2.453 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.293 |
1.378 |
0.000 |
| y |
1.378 |
-25.288 |
0.000 |
| z |
0.000 |
0.000 |
-21.771 |
|
| Traceless |
| | x | y | z |
| x |
2.237 |
1.378 |
0.000 |
| y |
1.378 |
-3.756 |
0.000 |
| z |
0.000 |
0.000 |
1.520 |
|
| Polar |
| 3z2-r2 | 3.040 |
| x2-y2 | 3.995 |
| xy | 1.378 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.439 |
0.041 |
0.000 |
| y |
0.041 |
3.545 |
0.000 |
| z |
0.000 |
0.000 |
3.477 |
<r2> (average value of r
2) Å
2
| <r2> |
78.681 |
| (<r2>)1/2 |
8.870 |