Jump to
S1C2
Energy calculated at HF/CEP-31G
| | hartrees |
| Energy at 0K | -22.191953 |
| Energy at 298.15K | -22.193369 |
| HF Energy | -22.191953 |
| Nuclear repulsion energy | 17.623884 |
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-31G
| 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' |
4079 |
3677 |
101.59 |
|
|
|
| 2 |
A' |
3175 |
2862 |
154.43 |
|
|
|
| 3 |
A' |
1582 |
1426 |
69.99 |
|
|
|
| 4 |
A' |
1316 |
1186 |
226.69 |
|
|
|
| 5 |
A' |
1263 |
1138 |
135.64 |
|
|
|
| 6 |
A" |
1087 |
980 |
226.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6251.2 cm
-1
Scaled (by 0.9014) Zero Point Vibrational Energy (zpe) 5634.8 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-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.764 |
0.000 |
| O2 |
0.012 |
-0.580 |
0.000 |
| H3 |
-1.061 |
1.019 |
0.000 |
| H4 |
0.888 |
-0.965 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3434 | 1.1029 | 1.9382 |
O2 | 1.3434 | | 1.9253 | 0.9565 | H3 | 1.1029 | 1.9253 | | 2.7809 | H4 | 1.9382 | 0.9565 | 2.7809 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
113.793 |
|
O2 |
C1 |
H3 |
103.377 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/CEP-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.066 |
|
|
|
| 2 |
O |
-0.445 |
|
|
|
| 3 |
H |
0.089 |
|
|
|
| 4 |
H |
0.422 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.186 |
-1.105 |
0.000 |
1.120 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.218 |
-4.723 |
0.000 |
| y |
-4.723 |
-14.020 |
0.000 |
| z |
0.000 |
0.000 |
-11.975 |
|
| Traceless |
| | x | y | z |
| x |
1.779 |
-4.723 |
0.000 |
| y |
-4.723 |
-2.424 |
0.000 |
| z |
0.000 |
0.000 |
0.645 |
|
| Polar |
| 3z2-r2 | 1.289 |
| x2-y2 | 2.802 |
| xy | -4.723 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.994 |
-0.597 |
0.000 |
| y |
-0.597 |
2.323 |
0.000 |
| z |
0.000 |
0.000 |
1.554 |
<r2> (average value of r
2) Å
2
| <r2> |
15.982 |
| (<r2>)1/2 |
3.998 |
Jump to
S1C1
Energy calculated at HF/CEP-31G
| | hartrees |
| Energy at 0K | -22.178061 |
| Energy at 298.15K | -22.179458 |
| HF Energy | -22.178061 |
| Nuclear repulsion energy | 17.535134 |
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-31G
| 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' |
3966 |
3575 |
19.35 |
|
|
|
| 2 |
A' |
3019 |
2721 |
281.91 |
|
|
|
| 3 |
A' |
1550 |
1397 |
99.66 |
|
|
|
| 4 |
A' |
1305 |
1176 |
182.51 |
|
|
|
| 5 |
A' |
1259 |
1135 |
81.93 |
|
|
|
| 6 |
A" |
981 |
884 |
68.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6039.6 cm
-1
Scaled (by 0.9014) Zero Point Vibrational Energy (zpe) 5444.1 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 HF/CEP-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.118 |
0.767 |
0.000 |
| O2 |
0.118 |
-0.577 |
0.000 |
| H3 |
-0.950 |
1.094 |
0.000 |
| H4 |
-0.705 |
-1.075 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3444 | 1.1172 | 2.0175 |
O2 | 1.3444 | | 1.9834 | 0.9618 | H3 | 1.1172 | 1.9834 | | 2.1825 | H4 | 2.0175 | 0.9618 | 2.1825 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
121.158 |
|
O2 |
C1 |
H3 |
107.001 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/CEP-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.026 |
|
|
|
| 2 |
O |
-0.452 |
|
|
|
| 3 |
H |
0.038 |
|
|
|
| 4 |
H |
0.388 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.930 |
-1.246 |
0.000 |
4.123 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.699 |
-0.048 |
0.000 |
| y |
-0.048 |
-13.575 |
0.000 |
| z |
0.000 |
0.000 |
-11.906 |
|
| Traceless |
| | x | y | z |
| x |
0.042 |
-0.048 |
0.000 |
| y |
-0.048 |
-1.273 |
0.000 |
| z |
0.000 |
0.000 |
1.231 |
|
| Polar |
| 3z2-r2 | 2.463 |
| x2-y2 | 0.876 |
| 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 |
1.911 |
-0.033 |
0.000 |
| y |
-0.033 |
2.624 |
0.000 |
| z |
0.000 |
0.000 |
1.594 |
<r2> (average value of r
2) Å
2
| <r2> |
16.193 |
| (<r2>)1/2 |
4.024 |