Jump to
S1C2
Energy calculated at PBE1PBE/6-311G**
| | hartrees |
| Energy at 0K | -79.742851 |
| Energy at 298.15K | -79.748764 |
| HF Energy | -79.742851 |
| Nuclear repulsion energy | 42.265500 |
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 PBE1PBE/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1g |
3049 |
2926 |
0.00 |
260.26 |
0.01 |
0.01 |
| 2 |
A1g |
1424 |
1366 |
0.00 |
2.96 |
0.74 |
0.85 |
| 3 |
A1g |
1027 |
985 |
0.00 |
9.55 |
0.27 |
0.42 |
| 4 |
A1u |
312 |
299 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3050 |
2926 |
58.59 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1399 |
1342 |
2.92 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3108 |
2982 |
0.00 |
145.25 |
0.75 |
0.86 |
| 7 |
Eg |
3108 |
2982 |
0.00 |
145.24 |
0.75 |
0.86 |
| 8 |
Eg |
1501 |
1440 |
0.00 |
24.51 |
0.75 |
0.86 |
| 8 |
Eg |
1501 |
1440 |
0.00 |
24.51 |
0.75 |
0.86 |
| 9 |
Eg |
1215 |
1166 |
0.00 |
0.59 |
0.75 |
0.86 |
| 9 |
Eg |
1215 |
1166 |
0.00 |
0.59 |
0.75 |
0.86 |
| 10 |
Eu |
3133 |
3006 |
64.42 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3133 |
3006 |
64.42 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1501 |
1440 |
11.94 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1501 |
1440 |
11.94 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
824 |
791 |
5.52 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
824 |
791 |
5.52 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16411.8 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 15745.5 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 PBE1PBE/6-311G**
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.761 |
| C2 |
0.000 |
0.000 |
-0.761 |
| H3 |
0.000 |
1.018 |
1.160 |
| H4 |
-0.882 |
-0.509 |
1.160 |
| H5 |
0.882 |
-0.509 |
1.160 |
| H6 |
0.000 |
-1.018 |
-1.160 |
| H7 |
-0.882 |
0.509 |
-1.160 |
| H8 |
0.882 |
0.509 |
-1.160 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5216 | 1.0938 | 1.0938 | 1.0938 | 2.1743 | 2.1743 | 2.1743 |
C2 | 1.5216 | | 2.1743 | 2.1743 | 2.1743 | 1.0938 | 1.0938 | 1.0938 | H3 | 1.0938 | 2.1743 | | 1.7636 | 1.7636 | 3.0875 | 2.5342 | 2.5342 | H4 | 1.0938 | 2.1743 | 1.7636 | | 1.7636 | 2.5342 | 2.5342 | 3.0875 | H5 | 1.0938 | 2.1743 | 1.7636 | 1.7636 | | 2.5342 | 3.0875 | 2.5342 | H6 | 2.1743 | 1.0938 | 3.0875 | 2.5342 | 2.5342 | | 1.7636 | 1.7636 | H7 | 2.1743 | 1.0938 | 2.5342 | 2.5342 | 3.0875 | 1.7636 | | 1.7636 | H8 | 2.1743 | 1.0938 | 2.5342 | 3.0875 | 2.5342 | 1.7636 | 1.7636 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.423 |
|
C1 |
C2 |
H7 |
111.423 |
| C1 |
C2 |
H8 |
111.423 |
|
C2 |
C1 |
H3 |
111.423 |
| C2 |
C1 |
H4 |
111.423 |
|
C2 |
C1 |
H5 |
111.423 |
| H3 |
C1 |
H4 |
107.451 |
|
H3 |
C1 |
H5 |
107.451 |
| H4 |
C1 |
H5 |
107.451 |
|
H6 |
C2 |
H7 |
107.451 |
| H6 |
C2 |
H8 |
107.451 |
|
H7 |
C2 |
H8 |
107.451 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.367 |
|
|
|
| 2 |
C |
-0.367 |
|
|
|
| 3 |
H |
0.122 |
|
|
|
| 4 |
H |
0.122 |
|
|
|
| 5 |
H |
0.122 |
|
|
|
| 6 |
H |
0.122 |
|
|
|
| 7 |
H |
0.122 |
|
|
|
| 8 |
H |
0.122 |
|
|
|
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 |
-14.855 |
0.000 |
0.000 |
| y |
0.000 |
-14.855 |
0.000 |
| z |
0.000 |
0.000 |
-15.467 |
|
| Traceless |
| | x | y | z |
| x |
0.306 |
0.000 |
0.000 |
| y |
0.000 |
0.306 |
0.000 |
| z |
0.000 |
0.000 |
-0.612 |
|
| Polar |
| 3z2-r2 | -1.224 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.609 |
0.000 |
0.000 |
| y |
0.000 |
3.609 |
0.000 |
| z |
0.000 |
0.000 |
3.988 |
<r2> (average value of r
2) Å
2
| <r2> |
30.651 |
| (<r2>)1/2 |
5.536 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-311G**
| | hartrees |
| Energy at 0K | -79.738431 |
| Energy at 298.15K | |
| HF Energy | -79.738431 |
| Nuclear repulsion energy | 42.111181 |
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 PBE1PBE/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1' |
3065 |
2940 |
0.00 |
|
|
|
| 2 |
A1' |
1439 |
1380 |
0.00 |
|
|
|
| 3 |
A1' |
1025 |
984 |
0.00 |
|
|
|
| 4 |
A1" |
303i |
291i |
0.00 |
|
|
|
| 5 |
A2" |
3057 |
2933 |
61.35 |
|
|
|
| 6 |
A2" |
1397 |
1340 |
2.94 |
|
|
|
| 7 |
E' |
3140 |
3012 |
53.12 |
|
|
|
| 7 |
E' |
3140 |
3012 |
53.12 |
|
|
|
| 8 |
E' |
1507 |
1446 |
14.09 |
|
|
|
| 8 |
E' |
1507 |
1446 |
14.09 |
|
|
|
| 9 |
E' |
896 |
860 |
5.02 |
|
|
|
| 9 |
E' |
896 |
860 |
5.02 |
|
|
|
| 10 |
E" |
3118 |
2991 |
0.00 |
|
|
|
| 10 |
E" |
3118 |
2991 |
0.00 |
|
|
|
| 11 |
E" |
1498 |
1437 |
0.00 |
|
|
|
| 11 |
E" |
1498 |
1437 |
0.00 |
|
|
|
| 12 |
E" |
1165 |
1118 |
0.00 |
|
|
|
| 12 |
E" |
1165 |
1118 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16163.5 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 15507.3 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 PBE1PBE/6-311G**
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.767 |
| C2 |
0.000 |
0.000 |
-0.767 |
| H3 |
0.000 |
1.014 |
1.175 |
| H4 |
-0.878 |
-0.507 |
1.175 |
| H5 |
0.878 |
-0.507 |
1.175 |
| H6 |
0.000 |
1.014 |
-1.175 |
| H7 |
0.878 |
-0.507 |
-1.175 |
| H8 |
-0.878 |
-0.507 |
-1.175 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5345 | 1.0927 | 1.0927 | 1.0927 | 2.1907 | 2.1907 | 2.1907 |
C2 | 1.5345 | | 2.1907 | 2.1907 | 2.1907 | 1.0927 | 1.0927 | 1.0927 | H3 | 1.0927 | 2.1907 | | 1.7561 | 1.7561 | 2.3494 | 2.9332 | 2.9332 | H4 | 1.0927 | 2.1907 | 1.7561 | | 1.7561 | 2.9332 | 2.9332 | 2.3494 | H5 | 1.0927 | 2.1907 | 1.7561 | 1.7561 | | 2.9332 | 2.3494 | 2.9332 | H6 | 2.1907 | 1.0927 | 2.3494 | 2.9332 | 2.9332 | | 1.7561 | 1.7561 | H7 | 2.1907 | 1.0927 | 2.9332 | 2.9332 | 2.3494 | 1.7561 | | 1.7561 | H8 | 2.1907 | 1.0927 | 2.9332 | 2.3494 | 2.9332 | 1.7561 | 1.7561 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.893 |
|
C1 |
C2 |
H7 |
111.893 |
| C1 |
C2 |
H8 |
111.893 |
|
C2 |
C1 |
H3 |
111.893 |
| C2 |
C1 |
H4 |
111.893 |
|
C2 |
C1 |
H5 |
111.893 |
| H3 |
C1 |
H4 |
106.945 |
|
H3 |
C1 |
H5 |
106.945 |
| H4 |
C1 |
H5 |
106.945 |
|
H6 |
C2 |
H7 |
106.945 |
| H6 |
C2 |
H8 |
106.945 |
|
H7 |
C2 |
H8 |
106.945 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.379 |
|
|
|
| 2 |
C |
-0.379 |
|
|
|
| 3 |
H |
0.126 |
|
|
|
| 4 |
H |
0.126 |
|
|
|
| 5 |
H |
0.126 |
|
|
|
| 6 |
H |
0.126 |
|
|
|
| 7 |
H |
0.126 |
|
|
|
| 8 |
H |
0.126 |
|
|
|
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 |
-14.847 |
0.000 |
0.000 |
| y |
0.000 |
-14.847 |
0.000 |
| z |
0.000 |
0.000 |
-15.444 |
|
| Traceless |
| | x | y | z |
| x |
0.299 |
0.000 |
0.000 |
| y |
0.000 |
0.299 |
0.000 |
| z |
0.000 |
0.000 |
-0.597 |
|
| Polar |
| 3z2-r2 | -1.194 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.544 |
0.000 |
0.000 |
| y |
0.000 |
3.544 |
0.000 |
| z |
0.000 |
0.000 |
3.905 |
<r2> (average value of r
2) Å
2
| <r2> |
30.909 |
| (<r2>)1/2 |
5.560 |