Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -79.741132 |
| Energy at 298.15K | -79.747047 |
| HF Energy | -79.741132 |
| Nuclear repulsion energy | 42.277167 |
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 HSEh1PBE/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 |
3051 |
2928 |
0.00 |
242.96 |
0.01 |
0.02 |
| 2 |
A1g |
1438 |
1380 |
0.00 |
3.75 |
0.72 |
0.83 |
| 3 |
A1g |
1029 |
987 |
0.00 |
9.27 |
0.28 |
0.44 |
| 4 |
A1u |
313 |
300 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3051 |
2927 |
67.37 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1414 |
1357 |
4.28 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3106 |
2981 |
0.00 |
149.66 |
0.75 |
0.86 |
| 7 |
Eg |
3106 |
2981 |
0.00 |
149.65 |
0.75 |
0.86 |
| 8 |
Eg |
1521 |
1459 |
0.00 |
26.65 |
0.75 |
0.86 |
| 8 |
Eg |
1521 |
1459 |
0.00 |
26.65 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1176 |
0.00 |
0.80 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1176 |
0.00 |
0.80 |
0.75 |
0.86 |
| 10 |
Eu |
3132 |
3006 |
76.65 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3132 |
3006 |
76.65 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1521 |
1460 |
14.25 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1521 |
1460 |
14.25 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
828 |
795 |
5.63 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
828 |
795 |
5.63 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16481.4 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 15815.6 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 HSEh1PBE/6-311G*
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.760 |
| C2 |
0.000 |
0.000 |
-0.760 |
| H3 |
0.000 |
1.017 |
1.162 |
| H4 |
-0.881 |
-0.509 |
1.162 |
| H5 |
0.881 |
-0.509 |
1.162 |
| H6 |
0.000 |
-1.017 |
-1.162 |
| H7 |
-0.881 |
0.509 |
-1.162 |
| H8 |
0.881 |
0.509 |
-1.162 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5205 | 1.0936 | 1.0936 | 1.0936 | 2.1745 | 2.1745 | 2.1745 |
C2 | 1.5205 | | 2.1745 | 2.1745 | 2.1745 | 1.0936 | 1.0936 | 1.0936 | H3 | 1.0936 | 2.1745 | | 1.7621 | 1.7621 | 3.0881 | 2.5361 | 2.5361 | H4 | 1.0936 | 2.1745 | 1.7621 | | 1.7621 | 2.5361 | 2.5361 | 3.0881 | H5 | 1.0936 | 2.1745 | 1.7621 | 1.7621 | | 2.5361 | 3.0881 | 2.5361 | H6 | 2.1745 | 1.0936 | 3.0881 | 2.5361 | 2.5361 | | 1.7621 | 1.7621 | H7 | 2.1745 | 1.0936 | 2.5361 | 2.5361 | 3.0881 | 1.7621 | | 1.7621 | H8 | 2.1745 | 1.0936 | 2.5361 | 3.0881 | 2.5361 | 1.7621 | 1.7621 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.526 |
|
C1 |
C2 |
H7 |
111.526 |
| C1 |
C2 |
H8 |
111.526 |
|
C2 |
C1 |
H3 |
111.526 |
| C2 |
C1 |
H4 |
111.526 |
|
C2 |
C1 |
H5 |
111.526 |
| H3 |
C1 |
H4 |
107.341 |
|
H3 |
C1 |
H5 |
107.341 |
| H4 |
C1 |
H5 |
107.341 |
|
H6 |
C2 |
H7 |
107.341 |
| H6 |
C2 |
H8 |
107.341 |
|
H7 |
C2 |
H8 |
107.341 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.662 |
|
|
|
| 2 |
C |
-0.662 |
|
|
|
| 3 |
H |
0.221 |
|
|
|
| 4 |
H |
0.221 |
|
|
|
| 5 |
H |
0.221 |
|
|
|
| 6 |
H |
0.221 |
|
|
|
| 7 |
H |
0.221 |
|
|
|
| 8 |
H |
0.221 |
|
|
|
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 |
-14.890 |
0.000 |
0.000 |
| y |
0.000 |
-14.890 |
0.000 |
| z |
0.000 |
0.000 |
-15.597 |
|
| Traceless |
| | x | y | z |
| x |
0.354 |
0.000 |
0.000 |
| y |
0.000 |
0.354 |
0.000 |
| z |
0.000 |
0.000 |
-0.707 |
|
| Polar |
| 3z2-r2 | -1.414 |
| 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 |
3.533 |
0.000 |
0.000 |
| y |
0.000 |
3.533 |
0.000 |
| z |
0.000 |
0.000 |
3.887 |
<r2> (average value of r
2) Å
2
| <r2> |
30.688 |
| (<r2>)1/2 |
5.540 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -79.736726 |
| Energy at 298.15K | |
| HF Energy | -79.736726 |
| Nuclear repulsion energy | 42.116851 |
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 HSEh1PBE/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' |
3068 |
2944 |
0.00 |
|
|
|
| 2 |
A1' |
1462 |
1403 |
0.00 |
|
|
|
| 3 |
A1' |
1028 |
987 |
0.00 |
|
|
|
| 4 |
A1" |
302i |
290i |
0.00 |
|
|
|
| 5 |
A2" |
3059 |
2936 |
69.56 |
|
|
|
| 6 |
A2" |
1415 |
1358 |
4.30 |
|
|
|
| 7 |
E' |
3140 |
3013 |
64.64 |
|
|
|
| 7 |
E' |
3140 |
3013 |
64.62 |
|
|
|
| 8 |
E' |
1530 |
1468 |
15.68 |
|
|
|
| 8 |
E' |
1530 |
1468 |
15.68 |
|
|
|
| 9 |
E' |
908 |
871 |
5.40 |
|
|
|
| 9 |
E' |
908 |
871 |
5.40 |
|
|
|
| 10 |
E" |
3117 |
2991 |
0.00 |
|
|
|
| 10 |
E" |
3117 |
2991 |
0.00 |
|
|
|
| 11 |
E" |
1520 |
1459 |
0.00 |
|
|
|
| 11 |
E" |
1520 |
1459 |
0.00 |
|
|
|
| 12 |
E" |
1178 |
1130 |
0.00 |
|
|
|
| 12 |
E" |
1178 |
1130 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16257.6 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 15600.8 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 HSEh1PBE/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 |
1.013 |
1.177 |
| H4 |
-0.877 |
-0.506 |
1.177 |
| H5 |
0.877 |
-0.506 |
1.177 |
| H6 |
0.000 |
1.013 |
-1.177 |
| H7 |
0.877 |
-0.506 |
-1.177 |
| H8 |
-0.877 |
-0.506 |
-1.177 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5338 | 1.0925 | 1.0925 | 1.0925 | 2.1917 | 2.1917 | 2.1917 |
C2 | 1.5338 | | 2.1917 | 2.1917 | 2.1917 | 1.0925 | 1.0925 | 1.0925 | H3 | 1.0925 | 2.1917 | | 1.7540 | 1.7540 | 2.3536 | 2.9353 | 2.9353 | H4 | 1.0925 | 2.1917 | 1.7540 | | 1.7540 | 2.9353 | 2.9353 | 2.3536 | H5 | 1.0925 | 2.1917 | 1.7540 | 1.7540 | | 2.9353 | 2.3536 | 2.9353 | H6 | 2.1917 | 1.0925 | 2.3536 | 2.9353 | 2.9353 | | 1.7540 | 1.7540 | H7 | 2.1917 | 1.0925 | 2.9353 | 2.9353 | 2.3536 | 1.7540 | | 1.7540 | H8 | 2.1917 | 1.0925 | 2.9353 | 2.3536 | 2.9353 | 1.7540 | 1.7540 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
112.038 |
|
C1 |
C2 |
H7 |
112.038 |
| C1 |
C2 |
H8 |
112.038 |
|
C2 |
C1 |
H3 |
112.038 |
| C2 |
C1 |
H4 |
112.038 |
|
C2 |
C1 |
H5 |
112.038 |
| H3 |
C1 |
H4 |
106.787 |
|
H3 |
C1 |
H5 |
106.787 |
| H4 |
C1 |
H5 |
106.787 |
|
H6 |
C2 |
H7 |
106.787 |
| H6 |
C2 |
H8 |
106.787 |
|
H7 |
C2 |
H8 |
106.787 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.676 |
|
|
|
| 2 |
C |
-0.676 |
|
|
|
| 3 |
H |
0.225 |
|
|
|
| 4 |
H |
0.225 |
|
|
|
| 5 |
H |
0.225 |
|
|
|
| 6 |
H |
0.225 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.225 |
|
|
|
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 |
-14.887 |
0.000 |
0.000 |
| y |
0.000 |
-14.887 |
0.000 |
| z |
0.000 |
0.000 |
-15.523 |
|
| Traceless |
| | x | y | z |
| x |
0.318 |
0.000 |
0.000 |
| y |
0.000 |
0.318 |
0.000 |
| z |
0.000 |
0.000 |
-0.635 |
|
| Polar |
| 3z2-r2 | -1.271 |
| 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 |
3.473 |
0.000 |
0.000 |
| y |
0.000 |
3.473 |
0.000 |
| z |
0.000 |
0.000 |
3.796 |
<r2> (average value of r
2) Å
2
| <r2> |
30.950 |
| (<r2>)1/2 |
5.563 |