Jump to
S1C2
Energy calculated at M06-2X/STO-3G
| | hartrees |
| Energy at 0K | -112.863060 |
| Energy at 298.15K | -112.864452 |
| HF Energy | -112.863060 |
| Nuclear repulsion energy | 29.822026 |
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 M06-2X/STO-3G
| 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' |
3791 |
3791 |
7.04 |
|
|
|
| 2 |
A' |
3096 |
3096 |
79.38 |
|
|
|
| 3 |
A' |
1659 |
1659 |
31.35 |
|
|
|
| 4 |
A' |
1457 |
1457 |
24.52 |
|
|
|
| 5 |
A' |
1292 |
1292 |
80.38 |
|
|
|
| 6 |
A" |
1109 |
1109 |
60.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6201.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6201.7 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 M06-2X/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.010 |
0.767 |
0.000 |
| O2 |
0.010 |
-0.583 |
0.000 |
| H3 |
-1.129 |
0.931 |
0.000 |
| H4 |
0.988 |
-0.873 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3495 | 1.1507 | 1.9088 |
O2 | 1.3495 | | 1.8942 | 1.0196 | H3 | 1.1507 | 1.8942 | | 2.7807 | H4 | 1.9088 | 1.0196 | 2.7807 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
106.522 |
|
O2 |
C1 |
H3 |
98.198 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.034 |
|
|
|
| 2 |
O |
-0.204 |
|
|
|
| 3 |
H |
0.005 |
|
|
|
| 4 |
H |
0.232 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.538 |
-1.498 |
0.000 |
1.592 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.834 |
-2.435 |
0.000 |
| y |
-2.435 |
-12.717 |
0.000 |
| z |
0.000 |
0.000 |
-10.255 |
|
| Traceless |
| | x | y | z |
| x |
1.652 |
-2.435 |
0.000 |
| y |
-2.435 |
-2.673 |
0.000 |
| z |
0.000 |
0.000 |
1.020 |
|
| Polar |
| 3z2-r2 | 2.041 |
| x2-y2 | 2.883 |
| xy | -2.435 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.388 |
-0.675 |
0.000 |
| y |
-0.675 |
1.452 |
0.000 |
| z |
0.000 |
0.000 |
0.634 |
<r2> (average value of r
2) Å
2
| <r2> |
16.954 |
| (<r2>)1/2 |
4.117 |
Jump to
S1C1
Energy calculated at M06-2X/STO-3G
| | hartrees |
| Energy at 0K | -112.854169 |
| Energy at 298.15K | -112.855559 |
| HF Energy | -112.854169 |
| Nuclear repulsion energy | 29.834205 |
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 M06-2X/STO-3G
| 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' |
3659 |
3659 |
39.96 |
|
|
|
| 2 |
A' |
3032 |
3032 |
102.79 |
|
|
|
| 3 |
A' |
1630 |
1630 |
27.21 |
|
|
|
| 4 |
A' |
1468 |
1468 |
28.62 |
|
|
|
| 5 |
A' |
1335 |
1335 |
33.14 |
|
|
|
| 6 |
A" |
1074 |
1074 |
22.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6099.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6099.0 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 M06-2X/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.128 |
0.762 |
0.000 |
| O2 |
0.128 |
-0.578 |
0.000 |
| H3 |
-0.986 |
1.055 |
0.000 |
| H4 |
-0.807 |
-1.003 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3391 | 1.1519 | 1.9972 |
O2 | 1.3391 | | 1.9761 | 1.0273 | H3 | 1.1519 | 1.9761 | | 2.0658 | H4 | 1.9972 | 1.0273 | 2.0658 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
114.486 |
|
O2 |
C1 |
H3 |
104.742 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.009 |
|
|
|
| 2 |
O |
-0.193 |
|
|
|
| 3 |
H |
-0.010 |
|
|
|
| 4 |
H |
0.212 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.475 |
-1.529 |
0.000 |
2.909 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.805 |
0.175 |
0.000 |
| y |
0.175 |
-12.243 |
0.000 |
| z |
0.000 |
0.000 |
-10.256 |
|
| Traceless |
| | x | y | z |
| x |
0.445 |
0.175 |
0.000 |
| y |
0.175 |
-1.713 |
0.000 |
| z |
0.000 |
0.000 |
1.268 |
|
| Polar |
| 3z2-r2 | 2.535 |
| x2-y2 | 1.438 |
| xy | 0.175 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.091 |
0.109 |
0.000 |
| y |
0.109 |
1.770 |
0.000 |
| z |
0.000 |
0.000 |
0.687 |
<r2> (average value of r
2) Å
2
| <r2> |
17.053 |
| (<r2>)1/2 |
4.130 |