Jump to
S1C2
Energy calculated at PBE1PBE/3-21G
| | hartrees |
| Energy at 0K | -113.637363 |
| Energy at 298.15K | -113.638770 |
| HF Energy | -113.637363 |
| Nuclear repulsion energy | 29.910386 |
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 PBE1PBE/3-21G
| 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' |
3482 |
3344 |
29.14 |
|
|
|
| 2 |
A' |
2755 |
2646 |
164.98 |
|
|
|
| 3 |
A' |
1512 |
1452 |
32.06 |
|
|
|
| 4 |
A' |
1264 |
1214 |
2.08 |
|
|
|
| 5 |
A' |
1188 |
1141 |
189.29 |
|
|
|
| 6 |
A" |
1094 |
1051 |
151.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5646.8 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 5423.2 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 PBE1PBE/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.768 |
0.000 |
| O2 |
0.011 |
-0.583 |
0.000 |
| H3 |
-1.099 |
0.980 |
0.000 |
| H4 |
0.947 |
-0.919 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3511 | 1.1299 | 1.9293 |
O2 | 1.3511 | | 1.9175 | 0.9943 | H3 | 1.1299 | 1.9175 | | 2.7916 | H4 | 1.9293 | 0.9943 | 2.7916 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.750 |
|
O2 |
C1 |
H3 |
100.848 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.045 |
|
|
|
| 2 |
O |
-0.528 |
|
|
|
| 3 |
H |
0.168 |
|
|
|
| 4 |
H |
0.405 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.440 |
-1.569 |
0.000 |
1.630 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.733 |
-3.888 |
0.000 |
| y |
-3.888 |
-13.643 |
0.000 |
| z |
0.000 |
0.000 |
-11.668 |
|
| Traceless |
| | x | y | z |
| x |
1.922 |
-3.888 |
0.000 |
| y |
-3.888 |
-2.442 |
0.000 |
| z |
0.000 |
0.000 |
0.520 |
|
| Polar |
| 3z2-r2 | 1.041 |
| x2-y2 | 2.910 |
| xy | -3.888 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.256 |
-0.717 |
0.000 |
| y |
-0.717 |
2.226 |
0.000 |
| z |
0.000 |
0.000 |
1.142 |
<r2> (average value of r
2) Å
2
| <r2> |
17.675 |
| (<r2>)1/2 |
4.204 |
Jump to
S1C1
Energy calculated at PBE1PBE/3-21G
| | hartrees |
| Energy at 0K | -113.628381 |
| Energy at 298.15K | -113.629776 |
| HF Energy | -113.628381 |
| Nuclear repulsion energy | 29.941026 |
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 PBE1PBE/3-21G
| 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' |
3213 |
3086 |
47.62 |
|
|
|
| 2 |
A' |
2604 |
2501 |
250.22 |
|
|
|
| 3 |
A' |
1459 |
1402 |
81.23 |
|
|
|
| 4 |
A' |
1300 |
1248 |
20.82 |
|
|
|
| 5 |
A' |
1181 |
1134 |
46.56 |
|
|
|
| 6 |
A" |
1020 |
980 |
46.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5388.6 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 5175.2 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 PBE1PBE/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.123 |
0.760 |
0.000 |
| O2 |
0.123 |
-0.574 |
0.000 |
| H3 |
-0.967 |
1.100 |
0.000 |
| H4 |
-0.755 |
-1.067 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3348 | 1.1417 | 2.0278 |
O2 | 1.3348 | | 1.9979 | 1.0071 | H3 | 1.1417 | 1.9979 | | 2.1775 | H4 | 2.0278 | 1.0071 | 2.1775 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
119.302 |
|
O2 |
C1 |
H3 |
107.298 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.024 |
|
|
|
| 2 |
O |
-0.521 |
|
|
|
| 3 |
H |
0.123 |
|
|
|
| 4 |
H |
0.374 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.280 |
-1.676 |
0.000 |
3.683 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.259 |
0.097 |
0.000 |
| y |
0.097 |
-13.012 |
0.000 |
| z |
0.000 |
0.000 |
-11.662 |
|
| Traceless |
| | x | y | z |
| x |
0.078 |
0.097 |
0.000 |
| y |
0.097 |
-1.052 |
0.000 |
| z |
0.000 |
0.000 |
0.974 |
|
| Polar |
| 3z2-r2 | 1.948 |
| x2-y2 | 0.753 |
| xy | 0.097 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.069 |
-0.011 |
0.000 |
| y |
-0.011 |
2.842 |
0.000 |
| z |
0.000 |
0.000 |
1.197 |
<r2> (average value of r
2) Å
2
| <r2> |
17.865 |
| (<r2>)1/2 |
4.227 |