Jump to
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -151.435444 |
| Energy at 298.15K | -151.437250 |
| HF Energy | -151.435444 |
| Nuclear repulsion energy | 35.687714 |
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 B1B95/6-31G
| 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 |
3669 |
3499 |
0.00 |
136.77 |
0.35 |
0.51 |
| 2 |
A |
1512 |
1442 |
0.00 |
10.61 |
0.74 |
0.85 |
| 3 |
A |
908 |
866 |
0.00 |
17.81 |
0.27 |
0.42 |
| 4 |
A |
54 |
51 |
441.83 |
0.00 |
0.74 |
0.85 |
| 5 |
B |
3686 |
3515 |
58.57 |
0.00 |
0.75 |
0.86 |
| 6 |
B |
1175 |
1120 |
152.12 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5501.6 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 5246.9 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 B1B95/6-31G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.756 |
0.000 |
| O2 |
0.000 |
-0.756 |
0.000 |
| H3 |
0.968 |
0.898 |
-0.001 |
| H4 |
-0.968 |
-0.898 |
-0.001 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.5112 | 0.9781 | 1.9159 |
O2 | 1.5112 | | 1.9159 | 0.9781 | H3 | 0.9781 | 1.9159 | | 2.6403 | H4 | 1.9159 | 0.9781 | 2.6403 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
98.372 |
|
O2 |
O1 |
H3 |
98.372 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.412 |
|
|
|
| 2 |
O |
-0.412 |
|
|
|
| 3 |
H |
0.412 |
|
|
|
| 4 |
H |
0.412 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-0.003 |
0.003 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.927 |
4.068 |
0.000 |
| y |
4.068 |
-11.438 |
0.000 |
| z |
0.000 |
0.000 |
-12.651 |
|
| Traceless |
| | x | y | z |
| x |
4.117 |
4.068 |
0.000 |
| y |
4.068 |
-1.149 |
0.000 |
| z |
0.000 |
0.000 |
-2.968 |
|
| Polar |
| 3z2-r2 | -5.936 |
| x2-y2 | 3.511 |
| xy | 4.068 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.555 |
0.399 |
0.000 |
| y |
0.399 |
2.207 |
0.000 |
| z |
0.000 |
0.000 |
0.326 |
<r2> (average value of r
2) Å
2
| <r2> |
19.285 |
| (<r2>)1/2 |
4.392 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -151.435440 |
| Energy at 298.15K | -151.437295 |
| HF Energy | -151.435440 |
| Nuclear repulsion energy | 35.687949 |
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 B1B95/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3673 |
3503 |
0.00 |
|
|
|
| 2 |
Ag |
1513 |
1443 |
0.00 |
|
|
|
| 3 |
Ag |
908 |
866 |
0.00 |
|
|
|
| 4 |
Au |
80 |
76 |
441.81 |
|
|
|
| 5 |
Bu |
3690 |
3519 |
58.48 |
|
|
|
| 6 |
Bu |
1176 |
1121 |
152.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5520.0 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 5264.4 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 B1B95/6-31G
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.756 |
0.000 |
| O2 |
0.000 |
-0.756 |
0.000 |
| H3 |
0.968 |
0.898 |
0.000 |
| H4 |
-0.968 |
-0.898 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.5111 | 0.9781 | 1.9159 |
O2 | 1.5111 | | 1.9159 | 0.9781 | H3 | 0.9781 | 1.9159 | | 2.6402 | H4 | 1.9159 | 0.9781 | 2.6402 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
98.369 |
|
O2 |
O1 |
H3 |
98.369 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.412 |
|
|
|
| 2 |
O |
-0.412 |
|
|
|
| 3 |
H |
0.412 |
|
|
|
| 4 |
H |
0.412 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.927 |
4.068 |
0.000 |
| y |
4.068 |
-11.439 |
0.000 |
| z |
0.000 |
0.000 |
-12.651 |
|
| Traceless |
| | x | y | z |
| x |
4.118 |
4.068 |
0.000 |
| y |
4.068 |
-1.150 |
0.000 |
| z |
0.000 |
0.000 |
-2.968 |
|
| Polar |
| 3z2-r2 | -5.935 |
| x2-y2 | 3.512 |
| xy | 4.068 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.555 |
0.399 |
0.000 |
| y |
0.399 |
2.207 |
0.000 |
| z |
0.000 |
0.000 |
0.326 |
<r2> (average value of r
2) Å
2
| <r2> |
19.285 |
| (<r2>)1/2 |
4.391 |