Jump to
S1C2
Energy calculated at HF/6-311G*
| hartrees |
Energy at 0K | -113.814950 |
Energy at 298.15K | -113.816389 |
HF Energy | -113.814950 |
Nuclear repulsion energy | 31.193968 |
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 HF/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' |
4122 |
3728 |
91.49 |
|
|
|
2 |
A' |
3104 |
2807 |
149.10 |
|
|
|
3 |
A' |
1655 |
1496 |
57.43 |
|
|
|
4 |
A' |
1444 |
1306 |
143.72 |
|
|
|
5 |
A' |
1348 |
1219 |
130.29 |
|
|
|
6 |
A" |
1154 |
1043 |
156.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6413.3 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 5800.2 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 HF/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
0.732 |
0.000 |
O2 |
0.012 |
-0.561 |
0.000 |
H3 |
-1.057 |
0.985 |
0.000 |
H4 |
0.895 |
-0.888 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
H3 |
H4 |
C1 | | 1.2934 | 1.0977 | 1.8456 |
O2 | 1.2934 | | 1.8792 | 0.9421 | H3 | 1.0977 | 1.8792 | | 2.7051 | H4 | 1.8456 | 0.9421 | 2.7051 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
110.310 |
|
O2 |
C1 |
H3 |
103.307 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.109 |
|
|
|
2 |
O |
-0.503 |
|
|
|
3 |
H |
0.166 |
|
|
|
4 |
H |
0.447 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.239 |
-1.341 |
0.000 |
1.362 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-11.012 |
-3.987 |
0.000 |
y |
-3.987 |
-13.633 |
0.000 |
z |
0.000 |
0.000 |
-11.772 |
|
Traceless |
| x | y | z |
x |
1.690 |
-3.987 |
0.000 |
y |
-3.987 |
-2.241 |
0.000 |
z |
0.000 |
0.000 |
0.551 |
|
Polar |
3z2-r2 | 1.102 |
x2-y2 | 2.621 |
xy | -3.987 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.240 |
-0.518 |
0.000 |
y |
-0.518 |
2.249 |
0.000 |
z |
0.000 |
0.000 |
1.485 |
<r2> (average value of r
2) Å
2
<r2> |
16.996 |
(<r2>)1/2 |
4.123 |
Jump to
S1C1
Energy calculated at HF/6-311G*
| hartrees |
Energy at 0K | -113.805107 |
Energy at 298.15K | -113.806535 |
HF Energy | -113.805107 |
Nuclear repulsion energy | 31.087922 |
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 HF/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' |
4041 |
3655 |
25.99 |
|
|
|
2 |
A' |
2989 |
2703 |
230.95 |
|
|
|
3 |
A' |
1619 |
1464 |
67.16 |
|
|
|
4 |
A' |
1449 |
1311 |
207.19 |
|
|
|
5 |
A' |
1379 |
1247 |
1.16 |
|
|
|
6 |
A" |
1060 |
958 |
55.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6268.1 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 5668.9 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 HF/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.119 |
0.733 |
0.000 |
O2 |
0.119 |
-0.560 |
0.000 |
H3 |
-0.938 |
1.062 |
0.000 |
H4 |
-0.728 |
-0.980 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
H3 |
H4 |
C1 | | 1.2935 | 1.1068 | 1.9116 |
O2 | 1.2935 | | 1.9363 | 0.9456 | H3 | 1.1068 | 1.9363 | | 2.0535 | H4 | 1.9116 | 0.9456 | 2.0535 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
116.380 |
|
O2 |
C1 |
H3 |
107.299 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.056 |
|
|
|
2 |
O |
-0.507 |
|
|
|
3 |
H |
0.133 |
|
|
|
4 |
H |
0.430 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-3.307 |
-1.448 |
0.000 |
3.610 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-12.282 |
-0.048 |
0.000 |
y |
-0.048 |
-13.245 |
0.000 |
z |
0.000 |
0.000 |
-11.727 |
|
Traceless |
| x | y | z |
x |
0.204 |
-0.048 |
0.000 |
y |
-0.048 |
-1.241 |
0.000 |
z |
0.000 |
0.000 |
1.037 |
|
Polar |
3z2-r2 | 2.074 |
x2-y2 | 0.963 |
xy | -0.048 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.201 |
-0.129 |
0.000 |
y |
-0.129 |
2.469 |
0.000 |
z |
0.000 |
0.000 |
1.483 |
<r2> (average value of r
2) Å
2
<r2> |
17.190 |
(<r2>)1/2 |
4.146 |