Jump to
S1C2
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -79.723741 |
| Energy at 298.15K | -79.729604 |
| HF Energy | -79.723741 |
| Nuclear repulsion energy | 41.993442 |
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 PBEPBE/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 |
2969 |
2942 |
0.00 |
266.96 |
0.01 |
0.01 |
| 2 |
A1g |
1375 |
1362 |
0.00 |
4.15 |
0.75 |
0.86 |
| 3 |
A1g |
992 |
983 |
0.00 |
8.33 |
0.27 |
0.42 |
| 4 |
A1u |
303 |
300 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
2971 |
2943 |
61.64 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1358 |
1345 |
2.04 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3023 |
2995 |
0.00 |
149.87 |
0.75 |
0.86 |
| 7 |
Eg |
3023 |
2995 |
0.00 |
149.87 |
0.75 |
0.86 |
| 8 |
Eg |
1457 |
1443 |
0.00 |
25.78 |
0.75 |
0.86 |
| 8 |
Eg |
1457 |
1443 |
0.00 |
25.78 |
0.75 |
0.86 |
| 9 |
Eg |
1176 |
1166 |
0.00 |
0.58 |
0.75 |
0.86 |
| 9 |
Eg |
1176 |
1166 |
0.00 |
0.58 |
0.75 |
0.86 |
| 10 |
Eu |
3048 |
3020 |
66.37 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3048 |
3020 |
66.37 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1458 |
1445 |
11.17 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1458 |
1445 |
11.17 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
802 |
794 |
5.62 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
802 |
794 |
5.62 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 15946.1 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 15801.0 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 PBEPBE/6-311G**
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.765 |
| C2 |
0.000 |
0.000 |
-0.765 |
| H3 |
0.000 |
1.025 |
1.168 |
| H4 |
-0.887 |
-0.512 |
1.168 |
| H5 |
0.887 |
-0.512 |
1.168 |
| H6 |
0.000 |
-1.025 |
-1.168 |
| H7 |
-0.887 |
0.512 |
-1.168 |
| H8 |
0.887 |
0.512 |
-1.168 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5309 | 1.1011 | 1.1011 | 1.1011 | 2.1886 | 2.1886 | 2.1886 |
C2 | 1.5309 | | 2.1886 | 2.1886 | 2.1886 | 1.1011 | 1.1011 | 1.1011 | H3 | 1.1011 | 2.1886 | | 1.7749 | 1.7749 | 3.1082 | 2.5516 | 2.5516 | H4 | 1.1011 | 2.1886 | 1.7749 | | 1.7749 | 2.5516 | 2.5516 | 3.1082 | H5 | 1.1011 | 2.1886 | 1.7749 | 1.7749 | | 2.5516 | 3.1082 | 2.5516 | H6 | 2.1886 | 1.1011 | 3.1082 | 2.5516 | 2.5516 | | 1.7749 | 1.7749 | H7 | 2.1886 | 1.1011 | 2.5516 | 2.5516 | 3.1082 | 1.7749 | | 1.7749 | H8 | 2.1886 | 1.1011 | 2.5516 | 3.1082 | 2.5516 | 1.7749 | 1.7749 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.465 |
|
C1 |
C2 |
H7 |
111.465 |
| C1 |
C2 |
H8 |
111.465 |
|
C2 |
C1 |
H3 |
111.465 |
| C2 |
C1 |
H4 |
111.465 |
|
C2 |
C1 |
H5 |
111.465 |
| H3 |
C1 |
H4 |
107.406 |
|
H3 |
C1 |
H5 |
107.406 |
| H4 |
C1 |
H5 |
107.406 |
|
H6 |
C2 |
H7 |
107.406 |
| H6 |
C2 |
H8 |
107.406 |
|
H7 |
C2 |
H8 |
107.406 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.365 |
|
|
|
| 2 |
C |
-0.365 |
|
|
|
| 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 |
-15.022 |
0.000 |
0.000 |
| y |
0.000 |
-15.022 |
0.000 |
| z |
0.000 |
0.000 |
-15.605 |
|
| Traceless |
| | x | y | z |
| x |
0.292 |
0.000 |
0.000 |
| y |
0.000 |
0.292 |
0.000 |
| z |
0.000 |
0.000 |
-0.583 |
|
| Polar |
| 3z2-r2 | -1.167 |
| 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 |
3.729 |
0.000 |
0.000 |
| y |
0.000 |
3.729 |
0.000 |
| z |
0.000 |
0.000 |
4.146 |
<r2> (average value of r
2) Å
2
| <r2> |
31.026 |
| (<r2>)1/2 |
5.570 |
Jump to
S1C1
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -79.719519 |
| Energy at 298.15K | |
| HF Energy | -79.719519 |
| Nuclear repulsion energy | 41.835568 |
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 PBEPBE/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' |
2984 |
2957 |
0.00 |
|
|
|
| 2 |
A1' |
1391 |
1379 |
0.00 |
|
|
|
| 3 |
A1' |
988 |
979 |
0.00 |
|
|
|
| 4 |
A1" |
295i |
293i |
0.00 |
|
|
|
| 5 |
A2" |
2979 |
2951 |
63.51 |
|
|
|
| 6 |
A2" |
1355 |
1343 |
2.10 |
|
|
|
| 7 |
E' |
3055 |
3027 |
54.74 |
|
|
|
| 7 |
E' |
3055 |
3027 |
54.74 |
|
|
|
| 8 |
E' |
1463 |
1450 |
13.12 |
|
|
|
| 8 |
E' |
1463 |
1450 |
13.12 |
|
|
|
| 9 |
E' |
871 |
863 |
5.13 |
|
|
|
| 9 |
E' |
871 |
863 |
5.13 |
|
|
|
| 10 |
E" |
3033 |
3006 |
0.00 |
|
|
|
| 10 |
E" |
3033 |
3006 |
0.00 |
|
|
|
| 11 |
E" |
1455 |
1442 |
0.00 |
|
|
|
| 11 |
E" |
1455 |
1442 |
0.00 |
|
|
|
| 12 |
E" |
1126 |
1116 |
0.00 |
|
|
|
| 12 |
E" |
1126 |
1116 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15704.8 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 15561.9 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 PBEPBE/6-311G**
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.772 |
| C2 |
0.000 |
0.000 |
-0.772 |
| H3 |
0.000 |
1.020 |
1.183 |
| H4 |
-0.884 |
-0.510 |
1.183 |
| H5 |
0.884 |
-0.510 |
1.183 |
| H6 |
0.000 |
1.020 |
-1.183 |
| H7 |
0.884 |
-0.510 |
-1.183 |
| H8 |
-0.884 |
-0.510 |
-1.183 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5444 | 1.0999 | 1.0999 | 1.0999 | 2.2054 | 2.2054 | 2.2054 |
C2 | 1.5444 | | 2.2054 | 2.2054 | 2.2054 | 1.0999 | 1.0999 | 1.0999 | H3 | 1.0999 | 2.2054 | | 1.7674 | 1.7674 | 2.3658 | 2.9531 | 2.9531 | H4 | 1.0999 | 2.2054 | 1.7674 | | 1.7674 | 2.9531 | 2.9531 | 2.3658 | H5 | 1.0999 | 2.2054 | 1.7674 | 1.7674 | | 2.9531 | 2.3658 | 2.9531 | H6 | 2.2054 | 1.0999 | 2.3658 | 2.9531 | 2.9531 | | 1.7674 | 1.7674 | H7 | 2.2054 | 1.0999 | 2.9531 | 2.9531 | 2.3658 | 1.7674 | | 1.7674 | H8 | 2.2054 | 1.0999 | 2.9531 | 2.3658 | 2.9531 | 1.7674 | 1.7674 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.925 |
|
C1 |
C2 |
H7 |
111.925 |
| C1 |
C2 |
H8 |
111.925 |
|
C2 |
C1 |
H3 |
111.925 |
| C2 |
C1 |
H4 |
111.925 |
|
C2 |
C1 |
H5 |
111.925 |
| H3 |
C1 |
H4 |
106.910 |
|
H3 |
C1 |
H5 |
106.910 |
| H4 |
C1 |
H5 |
106.910 |
|
H6 |
C2 |
H7 |
106.910 |
| H6 |
C2 |
H8 |
106.910 |
|
H7 |
C2 |
H8 |
106.910 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.375 |
|
|
|
| 2 |
C |
-0.375 |
|
|
|
| 3 |
H |
0.125 |
|
|
|
| 4 |
H |
0.125 |
|
|
|
| 5 |
H |
0.125 |
|
|
|
| 6 |
H |
0.125 |
|
|
|
| 7 |
H |
0.125 |
|
|
|
| 8 |
H |
0.125 |
|
|
|
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 |
-15.013 |
0.000 |
0.000 |
| y |
0.000 |
-15.013 |
0.000 |
| z |
0.000 |
0.000 |
-15.586 |
|
| Traceless |
| | x | y | z |
| x |
0.286 |
0.000 |
0.000 |
| y |
0.000 |
0.286 |
0.000 |
| z |
0.000 |
0.000 |
-0.573 |
|
| Polar |
| 3z2-r2 | -1.145 |
| 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 |
3.660 |
0.000 |
0.000 |
| y |
0.000 |
3.660 |
0.000 |
| z |
0.000 |
0.000 |
4.057 |
<r2> (average value of r
2) Å
2
| <r2> |
31.294 |
| (<r2>)1/2 |
5.594 |