Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -114.318904 |
| Energy at 298.15K | -114.320328 |
| HF Energy | -114.318904 |
| Nuclear repulsion energy | 30.836309 |
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' |
3735 |
3584 |
48.70 |
|
|
|
| 2 |
A' |
2873 |
2757 |
164.03 |
|
|
|
| 3 |
A' |
1549 |
1486 |
30.03 |
|
|
|
| 4 |
A' |
1367 |
1312 |
74.40 |
|
|
|
| 5 |
A' |
1252 |
1201 |
125.45 |
|
|
|
| 6 |
A" |
1137 |
1091 |
134.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5956.0 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 5715.4 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) |
| C1 |
0.011 |
0.740 |
0.000 |
| O2 |
0.011 |
-0.565 |
0.000 |
| H3 |
-1.082 |
0.966 |
0.000 |
| H4 |
0.924 |
-0.882 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3053 | 1.1169 | 1.8606 |
O2 | 1.3053 | | 1.8818 | 0.9656 | H3 | 1.1169 | 1.8818 | | 2.7273 | H4 | 1.8606 | 0.9656 | 2.7273 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.113 |
|
O2 |
C1 |
H3 |
101.674 |
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 |
-0.203 |
|
|
|
| 2 |
O |
-0.394 |
|
|
|
| 3 |
H |
0.173 |
|
|
|
| 4 |
H |
0.424 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.307 |
-1.675 |
0.000 |
1.703 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.959 |
-3.818 |
0.000 |
| y |
-3.818 |
-13.681 |
0.000 |
| z |
0.000 |
0.000 |
-11.929 |
|
| Traceless |
| | x | y | z |
| x |
1.845 |
-3.818 |
0.000 |
| y |
-3.818 |
-2.236 |
0.000 |
| z |
0.000 |
0.000 |
0.391 |
|
| Polar |
| 3z2-r2 | 0.782 |
| x2-y2 | 2.721 |
| xy | -3.818 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.487 |
-0.551 |
0.000 |
| y |
-0.551 |
2.488 |
0.000 |
| z |
0.000 |
0.000 |
1.527 |
<r2> (average value of r
2) Å
2
| <r2> |
17.193 |
| (<r2>)1/2 |
4.146 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -114.309724 |
| Energy at 298.15K | -114.311137 |
| HF Energy | -114.309724 |
| Nuclear repulsion energy | 30.759055 |
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' |
3524 |
3381 |
30.83 |
|
|
|
| 2 |
A' |
2760 |
2648 |
253.67 |
|
|
|
| 3 |
A' |
1503 |
1442 |
66.50 |
|
|
|
| 4 |
A' |
1372 |
1316 |
64.92 |
|
|
|
| 5 |
A' |
1269 |
1218 |
21.64 |
|
|
|
| 6 |
A" |
1047 |
1005 |
43.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5737.1 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 5505.4 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) |
| C1 |
0.122 |
0.738 |
0.000 |
| O2 |
0.122 |
-0.562 |
0.000 |
| H3 |
-0.955 |
1.067 |
0.000 |
| H4 |
-0.747 |
-1.004 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.2998 | 1.1253 | 1.9467 |
O2 | 1.2998 | | 1.9518 | 0.9751 | H3 | 1.1253 | 1.9518 | | 2.0808 | H4 | 1.9467 | 0.9751 | 2.0808 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
116.970 |
|
O2 |
C1 |
H3 |
106.968 |
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 |
-0.149 |
|
|
|
| 2 |
O |
-0.390 |
|
|
|
| 3 |
H |
0.143 |
|
|
|
| 4 |
H |
0.396 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.153 |
-1.742 |
0.000 |
3.602 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.321 |
-0.032 |
0.000 |
| y |
-0.032 |
-13.170 |
0.000 |
| z |
0.000 |
0.000 |
-11.878 |
|
| Traceless |
| | x | y | z |
| x |
0.203 |
-0.032 |
0.000 |
| y |
-0.032 |
-1.070 |
0.000 |
| z |
0.000 |
0.000 |
0.867 |
|
| Polar |
| 3z2-r2 | 1.734 |
| x2-y2 | 0.849 |
| xy | -0.032 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.453 |
-0.032 |
0.000 |
| y |
-0.032 |
2.977 |
0.000 |
| z |
0.000 |
0.000 |
1.525 |
<r2> (average value of r
2) Å
2
| <r2> |
17.395 |
| (<r2>)1/2 |
4.171 |