Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -114.326639 |
| Energy at 298.15K | -114.328061 |
| HF Energy | -114.326639 |
| Nuclear repulsion energy | 30.825738 |
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' |
3769 |
3620 |
76.83 |
|
|
|
| 2 |
A' |
2853 |
2740 |
155.12 |
|
|
|
| 3 |
A' |
1523 |
1462 |
22.34 |
|
|
|
| 4 |
A' |
1368 |
1313 |
74.83 |
|
|
|
| 5 |
A' |
1228 |
1179 |
125.59 |
|
|
|
| 6 |
A" |
1119 |
1075 |
123.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5929.6 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 5694.8 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 Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.739 |
0.000 |
| O2 |
0.011 |
-0.567 |
0.000 |
| H3 |
-1.083 |
0.970 |
0.000 |
| H4 |
0.928 |
-0.870 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3060 | 1.1181 | 1.8519 |
O2 | 1.3060 | | 1.8865 | 0.9656 | H3 | 1.1181 | 1.8865 | | 2.7256 | H4 | 1.8519 | 0.9656 | 2.7256 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.288 |
|
O2 |
C1 |
H3 |
101.921 |
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 |
-0.151 |
|
|
|
| 2 |
O |
-0.219 |
|
|
|
| 3 |
H |
0.092 |
|
|
|
| 4 |
H |
0.278 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.242 |
-1.644 |
0.000 |
1.662 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.953 |
-3.696 |
0.000 |
| y |
-3.696 |
-13.660 |
0.000 |
| z |
0.000 |
0.000 |
-11.862 |
|
| Traceless |
| | x | y | z |
| x |
1.808 |
-3.696 |
0.000 |
| y |
-3.696 |
-2.252 |
0.000 |
| z |
0.000 |
0.000 |
0.445 |
|
| Polar |
| 3z2-r2 | 0.889 |
| x2-y2 | 2.707 |
| xy | -3.696 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.538 |
-0.538 |
0.000 |
| y |
-0.538 |
2.544 |
0.000 |
| z |
0.000 |
0.000 |
1.597 |
<r2> (average value of r
2) Å
2
| <r2> |
17.176 |
| (<r2>)1/2 |
4.144 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -114.317827 |
| Energy at 298.15K | -114.319234 |
| HF Energy | -114.317827 |
| Nuclear repulsion energy | 30.756750 |
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' |
3597 |
3454 |
23.20 |
|
|
|
| 2 |
A' |
2750 |
2641 |
236.47 |
|
|
|
| 3 |
A' |
1481 |
1423 |
53.32 |
|
|
|
| 4 |
A' |
1370 |
1315 |
72.26 |
|
|
|
| 5 |
A' |
1219 |
1170 |
21.15 |
|
|
|
| 6 |
A" |
1032 |
991 |
35.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5723.6 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 5496.9 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 Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.122 |
0.738 |
0.000 |
| O2 |
0.122 |
-0.563 |
0.000 |
| H3 |
-0.955 |
1.066 |
0.000 |
| H4 |
-0.755 |
-0.985 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3014 | 1.1258 | 1.9334 |
O2 | 1.3014 | | 1.9531 | 0.9729 | H3 | 1.1258 | 1.9531 | | 2.0609 | H4 | 1.9334 | 0.9729 | 2.0609 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
115.699 |
|
O2 |
C1 |
H3 |
106.934 |
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 |
-0.104 |
|
|
|
| 2 |
O |
-0.214 |
|
|
|
| 3 |
H |
0.067 |
|
|
|
| 4 |
H |
0.250 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.051 |
-1.708 |
0.000 |
3.496 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.266 |
-0.113 |
0.000 |
| y |
-0.113 |
-13.184 |
0.000 |
| z |
0.000 |
0.000 |
-11.806 |
|
| Traceless |
| | x | y | z |
| x |
0.229 |
-0.113 |
0.000 |
| y |
-0.113 |
-1.147 |
0.000 |
| z |
0.000 |
0.000 |
0.919 |
|
| Polar |
| 3z2-r2 | 1.837 |
| x2-y2 | 0.917 |
| xy | -0.113 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.497 |
-0.054 |
0.000 |
| y |
-0.054 |
2.971 |
0.000 |
| z |
0.000 |
0.000 |
1.589 |
<r2> (average value of r
2) Å
2
| <r2> |
17.360 |
| (<r2>)1/2 |
4.167 |