Jump to
S1C2
Energy calculated at HF/CEP-121G
| | hartrees |
| Energy at 0K | -22.194344 |
| Energy at 298.15K | -22.195765 |
| HF Energy | -22.194344 |
| Nuclear repulsion energy | 17.657855 |
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/CEP-121G
| 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' |
4034 |
3681 |
92.67 |
|
|
|
| 2 |
A' |
3079 |
2810 |
129.29 |
|
|
|
| 3 |
A' |
1583 |
1444 |
59.13 |
|
|
|
| 4 |
A' |
1306 |
1192 |
216.83 |
|
|
|
| 5 |
A' |
1261 |
1151 |
126.17 |
|
|
|
| 6 |
A" |
1093 |
998 |
215.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6178.4 cm
-1
Scaled (by 0.9125) Zero Point Vibrational Energy (zpe) 5637.8 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 HF/CEP-121G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.763 |
0.000 |
| O2 |
0.013 |
-0.578 |
0.000 |
| H3 |
-1.061 |
1.017 |
0.000 |
| H4 |
0.883 |
-0.965 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3411 | 1.1034 | 1.9348 |
O2 | 1.3411 | | 1.9231 | 0.9524 | H3 | 1.1034 | 1.9231 | | 2.7765 | H4 | 1.9348 | 0.9524 | 2.7765 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
113.977 |
|
O2 |
C1 |
H3 |
103.330 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/CEP-121G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.010 |
|
|
|
| 2 |
O |
-0.499 |
|
|
|
| 3 |
H |
0.071 |
|
|
|
| 4 |
H |
0.418 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.215 |
-1.100 |
0.000 |
1.121 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.302 |
-4.643 |
0.000 |
| y |
-4.643 |
-13.949 |
0.000 |
| z |
0.000 |
0.000 |
-11.958 |
|
| Traceless |
| | x | y | z |
| x |
1.652 |
-4.643 |
0.000 |
| y |
-4.643 |
-2.319 |
0.000 |
| z |
0.000 |
0.000 |
0.668 |
|
| Polar |
| 3z2-r2 | 1.335 |
| x2-y2 | 2.648 |
| xy | -4.643 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.342 |
-0.559 |
0.000 |
| y |
-0.559 |
2.465 |
0.000 |
| z |
0.000 |
0.000 |
1.600 |
<r2> (average value of r
2) Å
2
| <r2> |
15.954 |
| (<r2>)1/2 |
3.994 |
Jump to
S1C1
Energy calculated at HF/CEP-121G
| | hartrees |
| Energy at 0K | -22.181688 |
| Energy at 298.15K | -22.183091 |
| HF Energy | -22.181688 |
| Nuclear repulsion energy | 17.557311 |
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/CEP-121G
| 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' |
3922 |
3579 |
18.34 |
|
|
|
| 2 |
A' |
2921 |
2665 |
244.35 |
|
|
|
| 3 |
A' |
1541 |
1406 |
87.51 |
|
|
|
| 4 |
A' |
1292 |
1179 |
150.00 |
|
|
|
| 5 |
A' |
1278 |
1166 |
116.73 |
|
|
|
| 6 |
A" |
989 |
902 |
76.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5971.1 cm
-1
Scaled (by 0.9125) Zero Point Vibrational Energy (zpe) 5448.7 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/CEP-121G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.118 |
0.766 |
0.000 |
| O2 |
0.118 |
-0.577 |
0.000 |
| H3 |
-0.952 |
1.092 |
0.000 |
| H4 |
-0.700 |
-1.075 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3432 | 1.1183 | 2.0149 |
O2 | 1.3432 | | 1.9820 | 0.9579 | H3 | 1.1183 | 1.9820 | | 2.1809 | H4 | 2.0149 | 0.9579 | 2.1809 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
121.324 |
|
O2 |
C1 |
H3 |
106.902 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/CEP-121G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.094 |
|
|
|
| 2 |
O |
-0.507 |
|
|
|
| 3 |
H |
0.027 |
|
|
|
| 4 |
H |
0.385 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.745 |
-1.232 |
0.000 |
3.943 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.792 |
0.095 |
0.000 |
| y |
0.095 |
-13.469 |
0.000 |
| z |
0.000 |
0.000 |
-11.883 |
|
| Traceless |
| | x | y | z |
| x |
-0.116 |
0.095 |
0.000 |
| y |
0.095 |
-1.131 |
0.000 |
| z |
0.000 |
0.000 |
1.247 |
|
| Polar |
| 3z2-r2 | 2.495 |
| x2-y2 | 0.677 |
| xy | 0.095 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.324 |
-0.083 |
0.000 |
| y |
-0.083 |
2.747 |
0.000 |
| z |
0.000 |
0.000 |
1.604 |
<r2> (average value of r
2) Å
2
| <r2> |
16.170 |
| (<r2>)1/2 |
4.021 |