Jump to
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -114.401825 |
| Energy at 298.15K | -114.403246 |
| HF Energy | -114.401825 |
| Nuclear repulsion energy | 30.862758 |
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 B1B95/6-311G**
| 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' |
3777 |
3626 |
76.69 |
|
|
|
| 2 |
A' |
2853 |
2739 |
158.48 |
|
|
|
| 3 |
A' |
1525 |
1464 |
22.99 |
|
|
|
| 4 |
A' |
1369 |
1315 |
79.05 |
|
|
|
| 5 |
A' |
1226 |
1177 |
123.96 |
|
|
|
| 6 |
A" |
1121 |
1076 |
121.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5935.1 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 5698.3 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 B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.739 |
0.000 |
| O2 |
0.011 |
-0.566 |
0.000 |
| H3 |
-1.081 |
0.967 |
0.000 |
| H4 |
0.926 |
-0.870 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3047 | 1.1160 | 1.8507 |
O2 | 1.3047 | | 1.8822 | 0.9643 | H3 | 1.1160 | 1.8822 | | 2.7209 | H4 | 1.8507 | 0.9643 | 2.7209 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.367 |
|
O2 |
C1 |
H3 |
101.783 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.146 |
|
|
|
| 2 |
O |
-0.224 |
|
|
|
| 3 |
H |
0.089 |
|
|
|
| 4 |
H |
0.281 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.268 |
-1.630 |
0.000 |
1.651 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.927 |
-3.651 |
0.000 |
| y |
-3.651 |
-13.593 |
0.000 |
| z |
0.000 |
0.000 |
-11.824 |
|
| Traceless |
| | x | y | z |
| x |
1.782 |
-3.651 |
0.000 |
| y |
-3.651 |
-2.218 |
0.000 |
| z |
0.000 |
0.000 |
0.436 |
|
| Polar |
| 3z2-r2 | 0.872 |
| x2-y2 | 2.667 |
| xy | -3.651 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.530 |
-0.537 |
0.000 |
| y |
-0.537 |
2.531 |
0.000 |
| z |
0.000 |
0.000 |
1.581 |
<r2> (average value of r
2) Å
2
| <r2> |
17.124 |
| (<r2>)1/2 |
4.138 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -114.393066 |
| Energy at 298.15K | -114.394473 |
| HF Energy | -114.393066 |
| Nuclear repulsion energy | 30.790334 |
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 B1B95/6-311G**
| 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' |
3614 |
3470 |
21.38 |
|
|
|
| 2 |
A' |
2749 |
2639 |
240.13 |
|
|
|
| 3 |
A' |
1484 |
1425 |
52.20 |
|
|
|
| 4 |
A' |
1370 |
1315 |
76.52 |
|
|
|
| 5 |
A' |
1217 |
1168 |
23.22 |
|
|
|
| 6 |
A" |
1032 |
991 |
36.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5732.8 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 5504.1 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 B1B95/6-311G**
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 |
-0.954 |
1.061 |
0.000 |
| H4 |
-0.753 |
-0.985 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3005 | 1.1239 | 1.9319 |
O2 | 1.3005 | | 1.9483 | 0.9710 | H3 | 1.1239 | 1.9483 | | 2.0561 | H4 | 1.9319 | 0.9710 | 2.0561 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
115.771 |
|
O2 |
C1 |
H3 |
106.729 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.099 |
|
|
|
| 2 |
O |
-0.219 |
|
|
|
| 3 |
H |
0.063 |
|
|
|
| 4 |
H |
0.255 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.018 |
-1.700 |
0.000 |
3.464 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.225 |
-0.072 |
0.000 |
| y |
-0.072 |
-13.124 |
0.000 |
| z |
0.000 |
0.000 |
-11.769 |
|
| Traceless |
| | x | y | z |
| x |
0.222 |
-0.072 |
0.000 |
| y |
-0.072 |
-1.127 |
0.000 |
| z |
0.000 |
0.000 |
0.905 |
|
| Polar |
| 3z2-r2 | 1.810 |
| x2-y2 | 0.899 |
| xy | -0.072 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.484 |
-0.058 |
0.000 |
| y |
-0.058 |
2.939 |
0.000 |
| z |
0.000 |
0.000 |
1.573 |
<r2> (average value of r
2) Å
2
| <r2> |
17.308 |
| (<r2>)1/2 |
4.160 |