Jump to
S1C2
Energy calculated at B1B95/6-31G(2df,p)
| hartrees |
Energy at 0K | -151.502055 |
Energy at 298.15K | -151.504382 |
HF Energy | -151.502055 |
Nuclear repulsion energy | 37.337737 |
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(2df,p)
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 |
3826 |
3664 |
11.38 |
78.40 |
0.15 |
0.27 |
2 |
A |
1470 |
1408 |
0.36 |
6.76 |
0.55 |
0.71 |
3 |
A |
1011 |
968 |
1.02 |
10.13 |
0.24 |
0.39 |
4 |
A |
396 |
379 |
158.41 |
4.75 |
0.75 |
0.86 |
5 |
B |
3826 |
3664 |
42.78 |
33.33 |
0.75 |
0.86 |
6 |
B |
1370 |
1312 |
106.26 |
2.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5948.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5697.2 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 B1B95/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.712 |
-0.060 |
O2 |
0.000 |
-0.712 |
-0.060 |
H3 |
0.778 |
0.893 |
0.477 |
H4 |
-0.778 |
-0.893 |
0.477 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4247 | 0.9624 | 1.8630 |
O2 | 1.4247 | | 1.8630 | 0.9624 | H3 | 0.9624 | 1.8630 | | 2.3689 | H4 | 1.8630 | 0.9624 | 2.3689 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
100.822 |
|
O2 |
O1 |
H3 |
100.822 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.330 |
|
|
|
2 |
O |
-0.330 |
|
|
|
3 |
H |
0.330 |
|
|
|
4 |
H |
0.330 |
|
|
|
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 |
1.798 |
1.798 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-9.388 |
2.765 |
0.000 |
y |
2.765 |
-10.837 |
0.000 |
z |
0.000 |
0.000 |
-11.182 |
|
Traceless |
| x | y | z |
x |
1.622 |
2.765 |
0.000 |
y |
2.765 |
-0.552 |
0.000 |
z |
0.000 |
0.000 |
-1.070 |
|
Polar |
3z2-r2 | -2.140 |
x2-y2 | 1.449 |
xy | 2.765 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.503 |
0.297 |
0.000 |
y |
0.297 |
2.142 |
0.000 |
z |
0.000 |
0.000 |
1.226 |
<r2> (average value of r
2) Å
2
<r2> |
17.976 |
(<r2>)1/2 |
4.240 |
Jump to
S1C1
Energy calculated at B1B95/6-31G(2df,p)
| hartrees |
Energy at 0K | -151.500204 |
Energy at 298.15K | |
HF Energy | -151.500204 |
Nuclear repulsion energy | 37.165914 |
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(2df,p)
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 |
3865 |
3701 |
0.00 |
|
|
|
2 |
Ag |
1576 |
1509 |
0.00 |
|
|
|
3 |
Ag |
1015 |
972 |
0.00 |
|
|
|
4 |
Au |
301i |
288i |
256.07 |
|
|
|
5 |
Bu |
3875 |
3711 |
93.22 |
|
|
|
6 |
Bu |
1277 |
1223 |
137.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5653.1 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5414.0 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(2df,p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.718 |
0.000 |
O2 |
0.000 |
-0.718 |
0.000 |
H3 |
0.949 |
0.869 |
0.000 |
H4 |
-0.949 |
-0.869 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4368 | 0.9608 | 1.8497 |
O2 | 1.4368 | | 1.8497 | 0.9608 | H3 | 0.9608 | 1.8497 | | 2.5738 | H4 | 1.8497 | 0.9608 | 2.5738 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
99.034 |
|
O2 |
O1 |
H3 |
99.034 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.334 |
|
|
|
2 |
O |
-0.334 |
|
|
|
3 |
H |
0.334 |
|
|
|
4 |
H |
0.334 |
|
|
|
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 |
-7.875 |
3.326 |
0.000 |
y |
3.326 |
-10.975 |
0.000 |
z |
0.000 |
0.000 |
-12.394 |
|
Traceless |
| x | y | z |
x |
3.809 |
3.326 |
0.000 |
y |
3.326 |
-0.841 |
0.000 |
z |
0.000 |
0.000 |
-2.969 |
|
Polar |
3z2-r2 | -5.937 |
x2-y2 | 3.100 |
xy | 3.326 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.717 |
0.325 |
0.000 |
y |
0.325 |
2.145 |
0.000 |
z |
0.000 |
0.000 |
1.012 |
<r2> (average value of r
2) Å
2
<r2> |
18.075 |
(<r2>)1/2 |
4.251 |