Jump to
S1C2
Energy calculated at B2PLYP/cc-pVDZ
| hartrees |
Energy at 0K | -151.421320 |
Energy at 298.15K | -151.423563 |
HF Energy | -151.294695 |
Nuclear repulsion energy | 36.729832 |
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 B2PLYP/cc-pVDZ
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 |
3763 |
3604 |
11.25 |
81.59 |
0.19 |
0.32 |
2 |
A |
1443 |
1382 |
0.19 |
7.03 |
0.66 |
0.80 |
3 |
A |
929 |
889 |
1.33 |
11.78 |
0.24 |
0.39 |
4 |
A |
334 |
320 |
187.84 |
6.75 |
0.75 |
0.86 |
5 |
B |
3761 |
3602 |
51.58 |
34.43 |
0.75 |
0.86 |
6 |
B |
1301 |
1246 |
101.84 |
2.08 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5765.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5521.9 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 B2PLYP/cc-pVDZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.727 |
-0.055 |
O2 |
0.000 |
-0.727 |
-0.055 |
H3 |
0.822 |
0.886 |
0.436 |
H4 |
-0.822 |
-0.886 |
0.436 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4550 | 0.9707 | 1.8767 |
O2 | 1.4550 | | 1.8767 | 0.9707 | H3 | 0.9707 | 1.8767 | | 2.4184 | H4 | 1.8767 | 0.9707 | 2.4184 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
99.428 |
|
O2 |
O1 |
H3 |
99.428 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.183 |
|
|
|
2 |
O |
-0.183 |
|
|
|
3 |
H |
0.183 |
|
|
|
4 |
H |
0.183 |
|
|
|
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 |
1.724 |
1.724 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-9.129 |
2.900 |
0.000 |
y |
2.900 |
-11.088 |
0.000 |
z |
0.000 |
0.000 |
-11.448 |
|
Traceless |
| x | y | z |
x |
2.139 |
2.900 |
0.000 |
y |
2.900 |
-0.800 |
0.000 |
z |
0.000 |
0.000 |
-1.339 |
|
Polar |
3z2-r2 | -2.679 |
x2-y2 | 1.959 |
xy | 2.900 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.335 |
0.331 |
0.000 |
y |
0.331 |
2.044 |
0.000 |
z |
0.000 |
0.000 |
0.889 |
<r2> (average value of r
2) Å
2
<r2> |
18.413 |
(<r2>)1/2 |
4.291 |
Jump to
S1C1
Energy calculated at B2PLYP/cc-pVDZ
| hartrees |
Energy at 0K | -151.420306 |
Energy at 298.15K | |
HF Energy | -151.293457 |
Nuclear repulsion energy | 36.590205 |
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 B2PLYP/cc-pVDZ
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 |
3790 |
3630 |
0.00 |
|
|
|
2 |
Ag |
1527 |
1462 |
0.00 |
|
|
|
3 |
Ag |
931 |
892 |
0.00 |
|
|
|
4 |
Au |
247i |
237i |
283.13 |
|
|
|
5 |
Bu |
3797 |
3637 |
93.71 |
|
|
|
6 |
Bu |
1230 |
1178 |
127.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5513.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5280.5 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 B2PLYP/cc-pVDZ
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.733 |
0.000 |
O2 |
0.000 |
-0.733 |
0.000 |
H3 |
0.960 |
0.865 |
0.000 |
H4 |
-0.960 |
-0.865 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
O2 |
H3 |
H4 |
O1 | | 1.4655 | 0.9695 | 1.8639 |
O2 | 1.4655 | | 1.8639 | 0.9695 | H3 | 0.9695 | 1.8639 | | 2.5847 | H4 | 1.8639 | 0.9695 | 2.5847 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
O2 |
H4 |
97.818 |
|
O2 |
O1 |
H3 |
97.818 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.185 |
|
|
|
2 |
O |
-0.185 |
|
|
|
3 |
H |
0.185 |
|
|
|
4 |
H |
0.185 |
|
|
|
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 |
-7.898 |
3.339 |
0.000 |
y |
3.339 |
-11.198 |
0.000 |
z |
0.000 |
0.000 |
-12.423 |
|
Traceless |
| x | y | z |
x |
3.912 |
3.339 |
0.000 |
y |
3.339 |
-1.038 |
0.000 |
z |
0.000 |
0.000 |
-2.875 |
|
Polar |
3z2-r2 | -5.750 |
x2-y2 | 3.300 |
xy | 3.339 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.553 |
0.352 |
0.000 |
y |
0.352 |
2.051 |
0.000 |
z |
0.000 |
0.000 |
0.656 |
<r2> (average value of r
2) Å
2
<r2> |
18.493 |
(<r2>)1/2 |
4.300 |