Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G
| | hartrees |
| Energy at 0K | -79.708772 |
| Energy at 298.15K | -79.714709 |
| HF Energy | -79.708772 |
| Nuclear repulsion energy | 42.168808 |
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/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1g |
3065 |
2932 |
0.00 |
223.86 |
0.01 |
0.02 |
| 2 |
A1g |
1467 |
1403 |
0.00 |
8.93 |
0.72 |
0.84 |
| 3 |
A1g |
1042 |
997 |
0.00 |
8.94 |
0.28 |
0.44 |
| 4 |
A1u |
306 |
293 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3063 |
2930 |
60.04 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1465 |
1401 |
7.50 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3133 |
2997 |
0.00 |
135.68 |
0.75 |
0.86 |
| 7 |
Eg |
3133 |
2997 |
0.00 |
135.68 |
0.75 |
0.86 |
| 8 |
Eg |
1550 |
1483 |
0.00 |
45.69 |
0.75 |
0.86 |
| 8 |
Eg |
1550 |
1483 |
0.00 |
45.69 |
0.75 |
0.86 |
| 9 |
Eg |
1256 |
1201 |
0.00 |
3.67 |
0.75 |
0.86 |
| 9 |
Eg |
1256 |
1201 |
0.00 |
3.67 |
0.75 |
0.86 |
| 10 |
Eu |
3160 |
3023 |
69.53 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3160 |
3023 |
69.53 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1553 |
1486 |
14.56 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1553 |
1486 |
14.56 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
859 |
822 |
8.73 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
859 |
822 |
8.73 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16714.8 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 15989.3 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 HSEh1PBE/6-31G
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.763 |
| C2 |
0.000 |
0.000 |
-0.763 |
| H3 |
0.000 |
1.021 |
1.162 |
| H4 |
-0.884 |
-0.510 |
1.162 |
| H5 |
0.884 |
-0.510 |
1.162 |
| H6 |
0.000 |
-1.021 |
-1.162 |
| H7 |
-0.884 |
0.510 |
-1.162 |
| H8 |
0.884 |
0.510 |
-1.162 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5268 | 1.0956 | 1.0956 | 1.0956 | 2.1790 | 2.1790 | 2.1790 |
C2 | 1.5268 | | 2.1790 | 2.1790 | 2.1790 | 1.0956 | 1.0956 | 1.0956 | H3 | 1.0956 | 2.1790 | | 1.7677 | 1.7677 | 3.0928 | 2.5379 | 2.5379 | H4 | 1.0956 | 2.1790 | 1.7677 | | 1.7677 | 2.5379 | 2.5379 | 3.0928 | H5 | 1.0956 | 2.1790 | 1.7677 | 1.7677 | | 2.5379 | 3.0928 | 2.5379 | H6 | 2.1790 | 1.0956 | 3.0928 | 2.5379 | 2.5379 | | 1.7677 | 1.7677 | H7 | 2.1790 | 1.0956 | 2.5379 | 2.5379 | 3.0928 | 1.7677 | | 1.7677 | H8 | 2.1790 | 1.0956 | 2.5379 | 3.0928 | 2.5379 | 1.7677 | 1.7677 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.325 |
|
C1 |
C2 |
H7 |
111.325 |
| C1 |
C2 |
H8 |
111.325 |
|
C2 |
C1 |
H3 |
111.325 |
| C2 |
C1 |
H4 |
111.325 |
|
C2 |
C1 |
H5 |
111.325 |
| H3 |
C1 |
H4 |
107.556 |
|
H3 |
C1 |
H5 |
107.556 |
| H4 |
C1 |
H5 |
107.556 |
|
H6 |
C2 |
H7 |
107.556 |
| H6 |
C2 |
H8 |
107.556 |
|
H7 |
C2 |
H8 |
107.556 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.486 |
|
|
|
| 2 |
C |
-0.486 |
|
|
|
| 3 |
H |
0.162 |
|
|
|
| 4 |
H |
0.162 |
|
|
|
| 5 |
H |
0.162 |
|
|
|
| 6 |
H |
0.162 |
|
|
|
| 7 |
H |
0.162 |
|
|
|
| 8 |
H |
0.162 |
|
|
|
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 |
-14.735 |
0.000 |
0.000 |
| y |
0.000 |
-14.735 |
0.000 |
| z |
0.000 |
0.000 |
-15.130 |
|
| Traceless |
| | x | y | z |
| x |
0.197 |
0.000 |
0.000 |
| y |
0.000 |
0.197 |
0.000 |
| z |
0.000 |
0.000 |
-0.395 |
|
| Polar |
| 3z2-r2 | -0.790 |
| 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 |
3.295 |
0.000 |
0.000 |
| y |
0.000 |
3.295 |
0.000 |
| z |
0.000 |
0.000 |
3.466 |
<r2> (average value of r
2) Å
2
| <r2> |
30.627 |
| (<r2>)1/2 |
5.534 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G
| | hartrees |
| Energy at 0K | -79.704474 |
| Energy at 298.15K | |
| HF Energy | -79.704474 |
| Nuclear repulsion energy | 42.028805 |
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/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1' |
3081 |
2947 |
0.00 |
|
|
|
| 2 |
A1' |
1491 |
1426 |
0.00 |
|
|
|
| 3 |
A1' |
1037 |
992 |
0.00 |
|
|
|
| 4 |
A1" |
298i |
285i |
0.00 |
|
|
|
| 5 |
A2" |
3071 |
2937 |
63.40 |
|
|
|
| 6 |
A2" |
1463 |
1400 |
7.89 |
|
|
|
| 7 |
E' |
3166 |
3029 |
57.65 |
|
|
|
| 7 |
E' |
3166 |
3029 |
57.63 |
|
|
|
| 8 |
E' |
1561 |
1493 |
16.44 |
|
|
|
| 8 |
E' |
1561 |
1493 |
16.44 |
|
|
|
| 9 |
E' |
939 |
898 |
8.90 |
|
|
|
| 9 |
E' |
939 |
898 |
8.89 |
|
|
|
| 10 |
E" |
3144 |
3008 |
0.00 |
|
|
|
| 10 |
E" |
3144 |
3008 |
0.00 |
|
|
|
| 11 |
E" |
1549 |
1482 |
0.00 |
|
|
|
| 11 |
E" |
1549 |
1482 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1158 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1158 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16491.8 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 15776.1 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/6-31G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.769 |
| C2 |
0.000 |
0.000 |
-0.769 |
| H3 |
0.000 |
1.017 |
1.175 |
| H4 |
-0.880 |
-0.508 |
1.175 |
| H5 |
0.880 |
-0.508 |
1.175 |
| H6 |
0.000 |
1.017 |
-1.175 |
| H7 |
0.880 |
-0.508 |
-1.175 |
| H8 |
-0.880 |
-0.508 |
-1.175 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5384 | 1.0947 | 1.0947 | 1.0947 | 2.1941 | 2.1941 | 2.1941 |
C2 | 1.5384 | | 2.1941 | 2.1941 | 2.1941 | 1.0947 | 1.0947 | 1.0947 | H3 | 1.0947 | 2.1941 | | 1.7608 | 1.7608 | 2.3504 | 2.9368 | 2.9368 | H4 | 1.0947 | 2.1941 | 1.7608 | | 1.7608 | 2.9368 | 2.9368 | 2.3504 | H5 | 1.0947 | 2.1941 | 1.7608 | 1.7608 | | 2.9368 | 2.3504 | 2.9368 | H6 | 2.1941 | 1.0947 | 2.3504 | 2.9368 | 2.9368 | | 1.7608 | 1.7608 | H7 | 2.1941 | 1.0947 | 2.9368 | 2.9368 | 2.3504 | 1.7608 | | 1.7608 | H8 | 2.1941 | 1.0947 | 2.9368 | 2.3504 | 2.9368 | 1.7608 | 1.7608 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.772 |
|
C1 |
C2 |
H7 |
111.772 |
| C1 |
C2 |
H8 |
111.772 |
|
C2 |
C1 |
H3 |
111.772 |
| C2 |
C1 |
H4 |
111.772 |
|
C2 |
C1 |
H5 |
111.772 |
| H3 |
C1 |
H4 |
107.075 |
|
H3 |
C1 |
H5 |
107.075 |
| H4 |
C1 |
H5 |
107.075 |
|
H6 |
C2 |
H7 |
107.075 |
| H6 |
C2 |
H8 |
107.075 |
|
H7 |
C2 |
H8 |
107.075 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.495 |
|
|
|
| 2 |
C |
-0.495 |
|
|
|
| 3 |
H |
0.165 |
|
|
|
| 4 |
H |
0.165 |
|
|
|
| 5 |
H |
0.165 |
|
|
|
| 6 |
H |
0.165 |
|
|
|
| 7 |
H |
0.165 |
|
|
|
| 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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.715 |
0.000 |
0.000 |
| y |
0.000 |
-14.715 |
0.000 |
| z |
0.000 |
0.000 |
-15.053 |
|
| Traceless |
| | x | y | z |
| x |
0.169 |
0.000 |
0.000 |
| y |
0.000 |
0.169 |
0.000 |
| z |
0.000 |
0.000 |
-0.339 |
|
| Polar |
| 3z2-r2 | -0.677 |
| 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 |
3.220 |
0.000 |
0.000 |
| y |
0.000 |
3.220 |
0.000 |
| z |
0.000 |
0.000 |
3.374 |
<r2> (average value of r
2) Å
2
| <r2> |
30.848 |
| (<r2>)1/2 |
5.554 |