Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -151.503042 |
| Energy at 298.15K | -151.505358 |
| HF Energy | -151.503042 |
| Nuclear repulsion energy | 37.129310 |
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 B1B95/6-31+G**
| 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 |
3836 |
3669 |
14.72 |
87.33 |
0.15 |
0.26 |
| 2 |
A |
1467 |
1404 |
0.07 |
6.85 |
0.58 |
0.73 |
| 3 |
A |
994 |
951 |
1.13 |
17.58 |
0.24 |
0.39 |
| 4 |
A |
390 |
373 |
223.23 |
0.86 |
0.67 |
0.80 |
| 5 |
B |
3835 |
3669 |
71.07 |
28.51 |
0.75 |
0.86 |
| 6 |
B |
1329 |
1271 |
99.69 |
1.49 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5925.4 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 5668.3 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 B1B95/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.717 |
-0.054 |
| O2 |
0.000 |
-0.717 |
-0.054 |
| H3 |
0.813 |
0.897 |
0.435 |
| H4 |
-0.813 |
-0.897 |
0.435 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4338 | 0.9658 | 1.8720 |
O2 | 1.4338 | | 1.8720 | 0.9658 | H3 | 0.9658 | 1.8720 | | 2.4204 | H4 | 1.8720 | 0.9658 | 2.4204 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
100.737 |
|
O2 |
O1 |
H3 |
100.737 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.367 |
|
|
|
| 2 |
O |
-0.367 |
|
|
|
| 3 |
H |
0.367 |
|
|
|
| 4 |
H |
0.367 |
|
|
|
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 |
1.837 |
1.837 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.526 |
3.234 |
0.000 |
| y |
3.234 |
-11.570 |
0.000 |
| z |
0.000 |
0.000 |
-12.070 |
|
| Traceless |
| | x | y | z |
| x |
2.294 |
3.234 |
0.000 |
| y |
3.234 |
-0.771 |
0.000 |
| z |
0.000 |
0.000 |
-1.522 |
|
| Polar |
| 3z2-r2 | -3.045 |
| x2-y2 | 2.043 |
| xy | 3.234 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.616 |
0.225 |
0.000 |
| y |
0.225 |
2.347 |
0.000 |
| z |
0.000 |
0.000 |
1.464 |
<r2> (average value of r
2) Å
2
| <r2> |
18.484 |
| (<r2>)1/2 |
4.299 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -151.501560 |
| Energy at 298.15K | |
| HF Energy | -151.501560 |
| Nuclear repulsion energy | 36.985895 |
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 B1B95/6-31+G**
| 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 |
3867 |
3699 |
0.00 |
|
|
|
| 2 |
Ag |
1549 |
1482 |
0.00 |
|
|
|
| 3 |
Ag |
992 |
949 |
0.00 |
|
|
|
| 4 |
Au |
300i |
287i |
321.03 |
|
|
|
| 5 |
Bu |
3873 |
3705 |
122.03 |
|
|
|
| 6 |
Bu |
1253 |
1199 |
134.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5617.2 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 5373.4 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 B1B95/6-31+G**
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 |
0.877 |
0.000 |
| H4 |
-0.952 |
-0.877 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.4439 | 0.9646 | 1.8611 |
O2 | 1.4439 | | 1.8611 | 0.9646 | H3 | 0.9646 | 1.8611 | | 2.5892 | H4 | 1.8611 | 0.9646 | 2.5892 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
99.262 |
|
O2 |
O1 |
H3 |
99.262 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.373 |
|
|
|
| 2 |
O |
-0.373 |
|
|
|
| 3 |
H |
0.373 |
|
|
|
| 4 |
H |
0.373 |
|
|
|
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 |
-8.134 |
3.748 |
0.000 |
| y |
3.748 |
-11.693 |
0.000 |
| z |
0.000 |
0.000 |
-13.188 |
|
| Traceless |
| | x | y | z |
| x |
4.306 |
3.748 |
0.000 |
| y |
3.748 |
-1.032 |
0.000 |
| z |
0.000 |
0.000 |
-3.274 |
|
| Polar |
| 3z2-r2 | -6.549 |
| x2-y2 | 3.558 |
| xy | 3.748 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.695 |
0.243 |
0.000 |
| y |
0.243 |
2.370 |
0.000 |
| z |
0.000 |
0.000 |
1.370 |
<r2> (average value of r
2) Å
2
| <r2> |
18.565 |
| (<r2>)1/2 |
4.309 |