Jump to
S1C2
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -114.425062 |
| Energy at 298.15K | -114.426466 |
| HF Energy | -114.425062 |
| Nuclear repulsion energy | 30.336280 |
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 BLYP/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' |
3556 |
3542 |
47.47 |
|
|
|
| 2 |
A' |
2712 |
2701 |
180.08 |
|
|
|
| 3 |
A' |
1484 |
1479 |
19.41 |
|
|
|
| 4 |
A' |
1254 |
1250 |
20.83 |
|
|
|
| 5 |
A' |
1174 |
1170 |
148.92 |
|
|
|
| 6 |
A" |
1087 |
1083 |
114.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5633.9 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 5612.0 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.754 |
0.000 |
| O2 |
0.011 |
-0.577 |
0.000 |
| H3 |
-1.096 |
0.970 |
0.000 |
| H4 |
0.944 |
-0.875 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3306 | 1.1279 | 1.8771 |
O2 | 1.3306 | | 1.9025 | 0.9794 | H3 | 1.1279 | 1.9025 | | 2.7509 | H4 | 1.8771 | 0.9794 | 2.7509 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.731 |
|
O2 |
C1 |
H3 |
101.083 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.151 |
|
|
|
| 2 |
O |
-0.198 |
|
|
|
| 3 |
H |
0.082 |
|
|
|
| 4 |
H |
0.267 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.291 |
-1.662 |
0.000 |
1.687 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.110 |
-3.564 |
0.000 |
| y |
-3.564 |
-13.796 |
0.000 |
| z |
0.000 |
0.000 |
-11.977 |
|
| Traceless |
| | x | y | z |
| x |
1.777 |
-3.564 |
0.000 |
| y |
-3.564 |
-2.253 |
0.000 |
| z |
0.000 |
0.000 |
0.476 |
|
| Polar |
| 3z2-r2 | 0.952 |
| x2-y2 | 2.687 |
| xy | -3.564 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.690 |
-0.583 |
0.000 |
| y |
-0.583 |
2.678 |
0.000 |
| z |
0.000 |
0.000 |
1.606 |
<r2> (average value of r
2) Å
2
| <r2> |
17.551 |
| (<r2>)1/2 |
4.189 |
Jump to
S1C1
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -114.417283 |
| Energy at 298.15K | -114.418670 |
| HF Energy | -114.417283 |
| Nuclear repulsion energy | 30.313457 |
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 BLYP/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' |
3256 |
3244 |
88.38 |
|
|
|
| 2 |
A' |
2606 |
2596 |
273.24 |
|
|
|
| 3 |
A' |
1435 |
1430 |
53.06 |
|
|
|
| 4 |
A' |
1270 |
1265 |
28.83 |
|
|
|
| 5 |
A' |
1142 |
1137 |
17.57 |
|
|
|
| 6 |
A" |
1005 |
1001 |
29.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5357.1 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 5336.2 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.123 |
0.749 |
0.000 |
| O2 |
0.123 |
-0.571 |
0.000 |
| H3 |
-0.962 |
1.082 |
0.000 |
| H4 |
-0.766 |
-1.012 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3194 | 1.1352 | 1.9727 |
O2 | 1.3194 | | 1.9772 | 0.9931 | H3 | 1.1352 | 1.9772 | | 2.1032 | H4 | 1.9727 | 0.9931 | 2.1032 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
116.378 |
|
O2 |
C1 |
H3 |
107.084 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.105 |
|
|
|
| 2 |
O |
-0.189 |
|
|
|
| 3 |
H |
0.061 |
|
|
|
| 4 |
H |
0.233 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.902 |
-1.673 |
0.000 |
3.349 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.460 |
-0.102 |
0.000 |
| y |
-0.102 |
-13.268 |
0.000 |
| z |
0.000 |
0.000 |
-11.926 |
|
| Traceless |
| | x | y | z |
| x |
0.137 |
-0.102 |
0.000 |
| y |
-0.102 |
-1.075 |
0.000 |
| z |
0.000 |
0.000 |
0.938 |
|
| Polar |
| 3z2-r2 | 1.876 |
| x2-y2 | 0.808 |
| xy | -0.102 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.647 |
0.063 |
0.000 |
| y |
0.063 |
3.381 |
0.000 |
| z |
0.000 |
0.000 |
1.591 |
<r2> (average value of r
2) Å
2
| <r2> |
17.729 |
| (<r2>)1/2 |
4.211 |