Jump to
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -151.480560 |
| Energy at 298.15K | -151.482859 |
| HF Energy | -151.480560 |
| Nuclear repulsion energy | 37.117114 |
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 |
3773 |
3582 |
8.27 |
91.32 |
0.19 |
0.32 |
| 2 |
A |
1492 |
1417 |
0.45 |
9.18 |
0.64 |
0.78 |
| 3 |
A |
1003 |
953 |
1.79 |
12.04 |
0.27 |
0.42 |
| 4 |
A |
374 |
355 |
204.80 |
6.87 |
0.75 |
0.86 |
| 5 |
B |
3776 |
3584 |
38.81 |
38.59 |
0.75 |
0.86 |
| 6 |
B |
1360 |
1291 |
109.75 |
2.63 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5889.2 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 5590.7 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 B1B95/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.717 |
-0.056 |
| O2 |
0.000 |
-0.717 |
-0.056 |
| H3 |
0.812 |
0.888 |
0.444 |
| H4 |
-0.812 |
-0.888 |
0.444 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4339 | 0.9686 | 1.8666 |
O2 | 1.4339 | | 1.8666 | 0.9686 | H3 | 0.9686 | 1.8666 | | 2.4063 | H4 | 1.8666 | 0.9686 | 2.4063 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
100.161 |
|
O2 |
O1 |
H3 |
100.161 |
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 |
-0.428 |
|
|
|
| 2 |
O |
-0.428 |
|
|
|
| 3 |
H |
0.428 |
|
|
|
| 4 |
H |
0.428 |
|
|
|
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 |
1.847 |
1.847 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.170 |
3.008 |
0.000 |
| y |
3.008 |
-11.048 |
0.000 |
| z |
0.000 |
0.000 |
-11.454 |
|
| Traceless |
| | x | y | z |
| x |
2.081 |
3.008 |
0.000 |
| y |
3.008 |
-0.736 |
0.000 |
| z |
0.000 |
0.000 |
-1.345 |
|
| Polar |
| 3z2-r2 | -2.690 |
| x2-y2 | 1.878 |
| xy | 3.008 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.351 |
0.326 |
0.000 |
| y |
0.326 |
1.990 |
0.000 |
| z |
0.000 |
0.000 |
0.924 |
<r2> (average value of r
2) Å
2
| <r2> |
18.156 |
| (<r2>)1/2 |
4.261 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -151.479199 |
| Energy at 298.15K | |
| HF Energy | -151.479199 |
| Nuclear repulsion energy | 36.955620 |
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 |
3810 |
3617 |
0.00 |
|
|
|
| 2 |
Ag |
1586 |
1505 |
0.00 |
|
|
|
| 3 |
Ag |
1006 |
955 |
0.00 |
|
|
|
| 4 |
Au |
277i |
263i |
312.98 |
|
|
|
| 5 |
Bu |
3823 |
3629 |
81.81 |
|
|
|
| 6 |
Bu |
1281 |
1216 |
144.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5614.0 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 5329.3 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 B1B95/6-31G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.723 |
0.000 |
| O2 |
0.000 |
-0.723 |
0.000 |
| H3 |
0.957 |
0.865 |
0.000 |
| H4 |
-0.957 |
-0.865 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4454 | 0.9674 | 1.8538 |
O2 | 1.4454 | | 1.8538 | 0.9674 | H3 | 0.9674 | 1.8538 | | 2.5798 | H4 | 1.8538 | 0.9674 | 2.5798 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
98.458 |
|
O2 |
O1 |
H3 |
98.458 |
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 |
-0.433 |
|
|
|
| 2 |
O |
-0.433 |
|
|
|
| 3 |
H |
0.433 |
|
|
|
| 4 |
H |
0.433 |
|
|
|
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 |
-7.813 |
3.507 |
0.000 |
| y |
3.507 |
-11.178 |
0.000 |
| z |
0.000 |
0.000 |
-12.520 |
|
| Traceless |
| | x | y | z |
| x |
4.036 |
3.507 |
0.000 |
| y |
3.507 |
-1.012 |
0.000 |
| z |
0.000 |
0.000 |
-3.024 |
|
| Polar |
| 3z2-r2 | -6.048 |
| x2-y2 | 3.365 |
| xy | 3.507 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.575 |
0.342 |
0.000 |
| y |
0.342 |
1.998 |
0.000 |
| z |
0.000 |
0.000 |
0.684 |
<r2> (average value of r
2) Å
2
| <r2> |
18.245 |
| (<r2>)1/2 |
4.271 |