Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -154.226922 |
| Energy at 298.15K | |
| HF Energy | -154.226922 |
| Nuclear repulsion energy | 74.935345 |
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 |
A' |
3818 |
3664 |
4.09 |
|
|
|
| 2 |
A' |
3163 |
3035 |
12.26 |
|
|
|
| 3 |
A' |
2997 |
2876 |
75.44 |
|
|
|
| 4 |
A' |
1535 |
1473 |
0.39 |
|
|
|
| 5 |
A' |
1494 |
1434 |
7.12 |
|
|
|
| 6 |
A' |
1447 |
1389 |
2.38 |
|
|
|
| 7 |
A' |
1253 |
1202 |
67.43 |
|
|
|
| 8 |
A' |
1075 |
1032 |
92.60 |
|
|
|
| 9 |
A' |
1015 |
974 |
32.89 |
|
|
|
| 10 |
A' |
626 |
600 |
20.72 |
|
|
|
| 11 |
A' |
375 |
360 |
36.61 |
|
|
|
| 12 |
A" |
3270 |
3138 |
16.77 |
|
|
|
| 13 |
A" |
3030 |
2907 |
68.09 |
|
|
|
| 14 |
A" |
1302 |
1250 |
0.32 |
|
|
|
| 15 |
A" |
1179 |
1131 |
1.18 |
|
|
|
| 16 |
A" |
815 |
782 |
0.26 |
|
|
|
| 17 |
A" |
270 |
259 |
147.54 |
|
|
|
| 18 |
A" |
158i |
152i |
0.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14252.2 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 13676.4 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 Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-1.108 |
-0.365 |
0.000 |
| C2 |
0.000 |
0.534 |
0.000 |
| C3 |
1.255 |
-0.252 |
0.000 |
| H4 |
-1.912 |
0.162 |
0.000 |
| H5 |
-0.033 |
1.182 |
0.888 |
| H6 |
-0.033 |
1.182 |
-0.888 |
| H7 |
1.655 |
-0.645 |
-0.928 |
| H8 |
1.655 |
-0.645 |
0.928 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| O1 | | 1.4270 | 2.3664 | 0.9613 | 2.0830 | 2.0830 | 2.9285 | 2.9285 |
C2 | 1.4270 | | 1.4812 | 1.9475 | 1.0999 | 1.0999 | 2.2338 | 2.2338 | C3 | 2.3664 | 1.4812 | | 3.1943 | 2.1229 | 2.1229 | 1.0838 | 1.0838 | H4 | 0.9613 | 1.9475 | 3.1943 | | 2.3146 | 2.3146 | 3.7732 | 3.7732 | H5 | 2.0830 | 1.0999 | 2.1229 | 2.3146 | | 1.7754 | 3.0799 | 2.4884 | H6 | 2.0830 | 1.0999 | 2.1229 | 2.3146 | 1.7754 | | 2.4884 | 3.0799 | H7 | 2.9285 | 2.2338 | 1.0838 | 3.7732 | 3.0799 | 2.4884 | | 1.8552 | H8 | 2.9285 | 2.2338 | 1.0838 | 3.7732 | 2.4884 | 3.0799 | 1.8552 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C2 |
C3 |
108.900 |
|
O1 |
C2 |
H5 |
110.370 |
| O1 |
C2 |
H6 |
110.370 |
|
C2 |
O1 |
H4 |
107.663 |
| C2 |
C3 |
H7 |
120.332 |
|
C2 |
C3 |
H8 |
120.332 |
| C3 |
C2 |
H5 |
109.786 |
|
C3 |
C2 |
H6 |
109.786 |
| H5 |
C2 |
H6 |
107.618 |
|
H7 |
C3 |
H8 |
117.721 |
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 |
O |
-0.568 |
|
|
|
| 2 |
C |
-0.240 |
|
|
|
| 3 |
C |
-0.427 |
|
|
|
| 4 |
H |
0.386 |
|
|
|
| 5 |
H |
0.197 |
|
|
|
| 6 |
H |
0.197 |
|
|
|
| 7 |
H |
0.227 |
|
|
|
| 8 |
H |
0.227 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.279 |
1.587 |
0.000 |
1.611 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.671 |
-2.957 |
0.000 |
| y |
-2.957 |
-20.198 |
0.000 |
| z |
0.000 |
0.000 |
-18.777 |
|
| Traceless |
| | x | y | z |
| x |
2.817 |
-2.957 |
0.000 |
| y |
-2.957 |
-2.474 |
0.000 |
| z |
0.000 |
0.000 |
-0.342 |
|
| Polar |
| 3z2-r2 | -0.685 |
| x2-y2 | 3.527 |
| xy | -2.957 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.528 |
-0.474 |
0.000 |
| y |
-0.474 |
3.492 |
0.000 |
| z |
0.000 |
0.000 |
3.524 |
<r2> (average value of r
2) Å
2
| <r2> |
50.115 |
| (<r2>)1/2 |
7.079 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -154.228722 |
| Energy at 298.15K | -154.233404 |
| HF Energy | -154.228722 |
| Nuclear repulsion energy | 75.265054 |
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 |
A |
3852 |
3697 |
12.01 |
|
|
|
| 2 |
A |
3289 |
3157 |
9.08 |
|
|
|
| 3 |
A |
3175 |
3047 |
7.24 |
|
|
|
| 4 |
A |
2967 |
2847 |
74.61 |
|
|
|
| 5 |
A |
2904 |
2786 |
79.04 |
|
|
|
| 6 |
A |
1515 |
1453 |
6.91 |
|
|
|
| 7 |
A |
1482 |
1422 |
4.74 |
|
|
|
| 8 |
A |
1429 |
1371 |
0.60 |
|
|
|
| 9 |
A |
1292 |
1240 |
79.92 |
|
|
|
| 10 |
A |
1239 |
1189 |
9.61 |
|
|
|
| 11 |
A |
1143 |
1097 |
51.06 |
|
|
|
| 12 |
A |
1083 |
1040 |
25.00 |
|
|
|
| 13 |
A |
975 |
936 |
12.31 |
|
|
|
| 14 |
A |
875 |
839 |
15.00 |
|
|
|
| 15 |
A |
455 |
437 |
27.62 |
|
|
|
| 16 |
A |
402 |
386 |
49.61 |
|
|
|
| 17 |
A |
302 |
290 |
116.12 |
|
|
|
| 18 |
A |
146 |
140 |
22.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14262.1 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 13685.9 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 HSEh1PBE/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-1.101 |
-0.379 |
-0.058 |
| C2 |
-0.011 |
0.521 |
0.035 |
| C3 |
1.243 |
-0.253 |
-0.018 |
| H4 |
-1.905 |
0.119 |
0.106 |
| H5 |
-0.067 |
1.095 |
0.979 |
| H6 |
-0.034 |
1.262 |
-0.781 |
| H7 |
2.184 |
0.242 |
-0.221 |
| H8 |
1.238 |
-1.294 |
0.277 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| O1 | | 1.4166 | 2.3479 | 0.9595 | 2.0781 | 2.0861 | 3.3477 | 2.5343 |
C2 | 1.4166 | | 1.4741 | 1.9372 | 1.1068 | 1.1023 | 2.2275 | 2.2163 | C3 | 2.3479 | 1.4741 | | 3.1720 | 2.1276 | 2.1232 | 1.0828 | 1.0822 | H4 | 0.9595 | 1.9372 | 3.1720 | | 2.2566 | 2.3641 | 4.1039 | 3.4503 | H5 | 2.0781 | 1.1068 | 2.1276 | 2.2566 | | 1.7682 | 2.6900 | 2.8116 | H6 | 2.0861 | 1.1023 | 2.1232 | 2.3641 | 1.7682 | | 2.5052 | 3.0448 | H7 | 3.3477 | 2.2275 | 1.0828 | 4.1039 | 2.6900 | 2.5052 | | 1.8717 | H8 | 2.5343 | 2.2163 | 1.0822 | 3.4503 | 2.8116 | 3.0448 | 1.8717 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C2 |
C3 |
108.612 |
|
O1 |
C2 |
H5 |
110.276 |
| O1 |
C2 |
H6 |
111.212 |
|
C2 |
O1 |
H4 |
107.676 |
| C2 |
C3 |
H7 |
120.418 |
|
C2 |
C3 |
H8 |
119.432 |
| C3 |
C2 |
H5 |
110.237 |
|
C3 |
C2 |
H6 |
110.157 |
| H5 |
C2 |
H6 |
106.342 |
|
H7 |
C3 |
H8 |
119.653 |
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 |
O |
-0.574 |
|
|
|
| 2 |
C |
-0.219 |
|
|
|
| 3 |
C |
-0.460 |
|
|
|
| 4 |
H |
0.391 |
|
|
|
| 5 |
H |
0.200 |
|
|
|
| 6 |
H |
0.204 |
|
|
|
| 7 |
H |
0.219 |
|
|
|
| 8 |
H |
0.238 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.377 |
1.779 |
0.474 |
1.879 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.786 |
-1.865 |
-0.609 |
| y |
-1.865 |
-19.326 |
-0.483 |
| z |
-0.609 |
-0.483 |
-20.388 |
|
| Traceless |
| | x | y | z |
| x |
4.072 |
-1.865 |
-0.609 |
| y |
-1.865 |
-1.239 |
-0.483 |
| z |
-0.609 |
-0.483 |
-2.832 |
|
| Polar |
| 3z2-r2 | -5.665 |
| x2-y2 | 3.541 |
| xy | -1.865 |
| xz | -0.609 |
| yz | -0.483 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.579 |
-0.255 |
-0.145 |
| y |
-0.255 |
3.936 |
-0.083 |
| z |
-0.145 |
-0.083 |
2.996 |
<r2> (average value of r
2) Å
2
| <r2> |
49.988 |
| (<r2>)1/2 |
7.070 |