Jump to
S1C2
Energy calculated at B3PW91/6-31G(2df,p)
| hartrees |
Energy at 0K | -151.497496 |
Energy at 298.15K | -151.499817 |
HF Energy | -151.497496 |
Nuclear repulsion energy | 37.169009 |
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 B3PW91/6-31G(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 |
3793 |
3647 |
10.26 |
78.46 |
0.15 |
0.27 |
2 |
A |
1461 |
1405 |
0.40 |
6.97 |
0.54 |
0.70 |
3 |
A |
992 |
954 |
1.03 |
9.64 |
0.24 |
0.39 |
4 |
A |
393 |
378 |
157.23 |
4.79 |
0.75 |
0.86 |
5 |
B |
3794 |
3647 |
39.14 |
33.48 |
0.75 |
0.86 |
6 |
B |
1362 |
1309 |
105.59 |
2.06 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5897.3 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 5669.7 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 B3PW91/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.716 |
-0.060 |
O2 |
0.000 |
-0.716 |
-0.060 |
H3 |
0.781 |
0.895 |
0.478 |
H4 |
-0.781 |
-0.895 |
0.478 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4322 | 0.9654 | 1.8695 |
O2 | 1.4322 | | 1.8695 | 0.9654 | H3 | 0.9654 | 1.8695 | | 2.3760 | H4 | 1.8695 | 0.9654 | 2.3760 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
100.667 |
|
O2 |
O1 |
H3 |
100.667 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.333 |
|
|
|
2 |
O |
-0.333 |
|
|
|
3 |
H |
0.333 |
|
|
|
4 |
H |
0.333 |
|
|
|
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 |
1.794 |
1.794 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-9.395 |
2.770 |
0.000 |
y |
2.770 |
-10.850 |
0.000 |
z |
0.000 |
0.000 |
-11.208 |
|
Traceless |
| x | y | z |
x |
1.634 |
2.770 |
0.000 |
y |
2.770 |
-0.549 |
0.000 |
z |
0.000 |
0.000 |
-1.085 |
|
Polar |
3z2-r2 | -2.170 |
x2-y2 | 1.455 |
xy | 2.770 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.517 |
0.296 |
0.000 |
y |
0.296 |
2.157 |
0.000 |
z |
0.000 |
0.000 |
1.237 |
<r2> (average value of r
2) Å
2
<r2> |
18.090 |
(<r2>)1/2 |
4.253 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G(2df,p)
| hartrees |
Energy at 0K | -151.495666 |
Energy at 298.15K | |
HF Energy | -151.495666 |
Nuclear repulsion energy | 36.995467 |
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 B3PW91/6-31G(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 |
3833 |
3685 |
0.00 |
|
|
|
2 |
Ag |
1568 |
1507 |
0.00 |
|
|
|
3 |
Ag |
997 |
959 |
0.00 |
|
|
|
4 |
Au |
302i |
290i |
253.87 |
|
|
|
5 |
Bu |
3843 |
3695 |
87.10 |
|
|
|
6 |
Bu |
1272 |
1223 |
137.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5605.2 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 5388.8 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 B3PW91/6-31G(2df,p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.722 |
0.000 |
O2 |
0.000 |
-0.722 |
0.000 |
H3 |
0.952 |
0.871 |
0.000 |
H4 |
-0.952 |
-0.871 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4446 | 0.9638 | 1.8564 |
O2 | 1.4446 | | 1.8564 | 0.9638 | H3 | 0.9638 | 1.8564 | | 2.5814 | H4 | 1.8564 | 0.9638 | 2.5814 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
98.899 |
|
O2 |
O1 |
H3 |
98.899 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.337 |
|
|
|
2 |
O |
-0.337 |
|
|
|
3 |
H |
0.337 |
|
|
|
4 |
H |
0.337 |
|
|
|
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 |
-7.878 |
3.330 |
0.000 |
y |
3.330 |
-10.985 |
0.000 |
z |
0.000 |
0.000 |
-12.425 |
|
Traceless |
| x | y | z |
x |
3.827 |
3.330 |
0.000 |
y |
3.330 |
-0.834 |
0.000 |
z |
0.000 |
0.000 |
-2.993 |
|
Polar |
3z2-r2 | -5.986 |
x2-y2 | 3.107 |
xy | 3.330 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.733 |
0.323 |
0.000 |
y |
0.323 |
2.159 |
0.000 |
z |
0.000 |
0.000 |
1.021 |
<r2> (average value of r
2) Å
2
<r2> |
18.193 |
(<r2>)1/2 |
4.265 |