Jump to
S1C2
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -151.555922 |
| Energy at 298.15K | -151.558242 |
| HF Energy | -151.555922 |
| Nuclear repulsion energy | 37.261050 |
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/cc-pVTZ
| 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 |
3825 |
3661 |
14.22 |
77.58 |
0.14 |
0.25 |
| 2 |
A |
1458 |
1395 |
0.40 |
5.83 |
0.53 |
0.70 |
| 3 |
A |
1002 |
959 |
1.01 |
13.49 |
0.24 |
0.38 |
| 4 |
A |
388 |
371 |
169.88 |
5.37 |
0.75 |
0.86 |
| 5 |
B |
3824 |
3660 |
52.66 |
31.22 |
0.75 |
0.86 |
| 6 |
B |
1347 |
1290 |
102.95 |
1.82 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5921.7 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 5667.6 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/cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.715 |
-0.058 |
| O2 |
0.000 |
-0.715 |
-0.058 |
| H3 |
0.784 |
0.896 |
0.467 |
| H4 |
-0.784 |
-0.896 |
0.467 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4292 | 0.9614 | 1.8667 |
O2 | 1.4292 | | 1.8667 | 0.9614 | H3 | 0.9614 | 1.8667 | | 2.3812 | H4 | 1.8667 | 0.9614 | 2.3812 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
100.853 |
|
O2 |
O1 |
H3 |
100.853 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.241 |
|
|
|
| 2 |
O |
-0.241 |
|
|
|
| 3 |
H |
0.241 |
|
|
|
| 4 |
H |
0.241 |
|
|
|
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 |
1.809 |
1.809 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.526 |
2.863 |
0.000 |
| y |
2.863 |
-11.167 |
0.000 |
| z |
0.000 |
0.000 |
-11.490 |
|
| Traceless |
| | x | y | z |
| x |
1.802 |
2.863 |
0.000 |
| y |
2.863 |
-0.658 |
0.000 |
| z |
0.000 |
0.000 |
-1.144 |
|
| Polar |
| 3z2-r2 | -2.288 |
| x2-y2 | 1.640 |
| xy | 2.863 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.590 |
0.278 |
0.000 |
| y |
0.278 |
2.302 |
0.000 |
| z |
0.000 |
0.000 |
1.303 |
<r2> (average value of r
2) Å
2
| <r2> |
18.197 |
| (<r2>)1/2 |
4.266 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -151.554189 |
| Energy at 298.15K | |
| HF Energy | -151.554189 |
| Nuclear repulsion energy | 37.109274 |
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/cc-pVTZ
| 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 |
3861 |
3696 |
0.00 |
|
|
|
| 2 |
Ag |
1553 |
1486 |
0.00 |
|
|
|
| 3 |
Ag |
1004 |
961 |
0.00 |
|
|
|
| 4 |
Au |
302i |
289i |
270.61 |
|
|
|
| 5 |
Bu |
3868 |
3702 |
106.17 |
|
|
|
| 6 |
Bu |
1257 |
1203 |
133.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5620.2 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 5379.1 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/cc-pVTZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.720 |
0.000 |
| O2 |
0.000 |
-0.720 |
0.000 |
| H3 |
0.948 |
0.872 |
0.000 |
| H4 |
-0.948 |
-0.872 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4403 | 0.9599 | 1.8530 |
O2 | 1.4403 | | 1.8530 | 0.9599 | H3 | 0.9599 | 1.8530 | | 2.5759 | H4 | 1.8530 | 0.9599 | 2.5759 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
99.107 |
|
O2 |
O1 |
H3 |
99.107 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.237 |
|
|
|
| 2 |
O |
-0.237 |
|
|
|
| 3 |
H |
0.237 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
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 |
-8.050 |
3.403 |
0.000 |
| y |
3.403 |
-11.301 |
0.000 |
| z |
0.000 |
0.000 |
-12.667 |
|
| Traceless |
| | x | y | z |
| x |
3.934 |
3.403 |
0.000 |
| y |
3.403 |
-0.943 |
0.000 |
| z |
0.000 |
0.000 |
-2.991 |
|
| Polar |
| 3z2-r2 | -5.983 |
| x2-y2 | 3.251 |
| xy | 3.403 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.798 |
0.293 |
0.000 |
| y |
0.293 |
2.292 |
0.000 |
| z |
0.000 |
0.000 |
1.074 |
<r2> (average value of r
2) Å
2
| <r2> |
18.281 |
| (<r2>)1/2 |
4.276 |