Jump to
S1C2
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -150.624834 |
| Energy at 298.15K | -150.626688 |
| HF Energy | -150.624834 |
| Nuclear repulsion energy | 34.894897 |
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 B97D3/3-21G*
| 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 |
3346 |
3346 |
0.00 |
133.53 |
0.36 |
0.53 |
| 2 |
A |
1459 |
1459 |
0.00 |
13.89 |
0.70 |
0.82 |
| 3 |
A |
942 |
942 |
0.00 |
9.97 |
0.26 |
0.41 |
| 4 |
A |
78 |
78 |
326.93 |
0.00 |
0.74 |
0.85 |
| 5 |
B |
3374 |
3374 |
9.66 |
0.00 |
0.75 |
0.86 |
| 6 |
B |
1146 |
1146 |
143.53 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5172.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5172.6 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 B97D3/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.774 |
-0.000 |
| O2 |
0.000 |
-0.774 |
-0.000 |
| H3 |
1.002 |
0.872 |
0.000 |
| H4 |
-1.002 |
-0.872 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.5471 | 1.0066 | 1.9269 |
O2 | 1.5471 | | 1.9269 | 1.0066 | H3 | 1.0066 | 1.9269 | | 2.6568 | H4 | 1.9269 | 1.0066 | 2.6568 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
95.637 |
|
O2 |
O1 |
H3 |
95.637 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.365 |
|
|
|
| 2 |
O |
-0.365 |
|
|
|
| 3 |
H |
0.365 |
|
|
|
| 4 |
H |
0.365 |
|
|
|
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 |
0.001 |
0.001 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.598 |
3.480 |
0.000 |
| y |
3.480 |
-10.950 |
0.000 |
| z |
0.000 |
0.000 |
-12.111 |
|
| Traceless |
| | x | y | z |
| x |
3.932 |
3.480 |
0.000 |
| y |
3.480 |
-1.096 |
0.000 |
| z |
0.000 |
0.000 |
-2.837 |
|
| Polar |
| 3z2-r2 | -5.673 |
| x2-y2 | 3.352 |
| xy | 3.480 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.621 |
0.439 |
0.000 |
| y |
0.439 |
1.924 |
0.000 |
| z |
0.000 |
0.000 |
0.189 |
<r2> (average value of r
2) Å
2
| <r2> |
19.487 |
| (<r2>)1/2 |
4.414 |
Jump to
S1C1
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -150.624841 |
| Energy at 298.15K | -150.626618 |
| HF Energy | -150.624841 |
| Nuclear repulsion energy | 34.890027 |
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 B97D3/3-21G*
| 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 |
3349 |
3349 |
0.00 |
|
|
|
| 2 |
Ag |
1459 |
1459 |
0.00 |
|
|
|
| 3 |
Ag |
943 |
943 |
0.00 |
|
|
|
| 4 |
Au |
37 |
37 |
327.17 |
|
|
|
| 5 |
Bu |
3376 |
3376 |
9.72 |
|
|
|
| 6 |
Bu |
1146 |
1146 |
143.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5155.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5155.1 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 B97D3/3-21G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.774 |
0.000 |
| O2 |
0.000 |
-0.774 |
0.000 |
| H3 |
1.002 |
0.872 |
0.000 |
| H4 |
-1.002 |
-0.872 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
O2 |
H3 |
H4 |
| O1 | | 1.5476 | 1.0064 | 1.9269 |
O2 | 1.5476 | | 1.9269 | 1.0064 | H3 | 1.0064 | 1.9269 | | 2.6564 | H4 | 1.9269 | 1.0064 | 2.6564 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
O2 |
H4 |
95.619 |
|
O2 |
O1 |
H3 |
95.619 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.365 |
|
|
|
| 2 |
O |
-0.365 |
|
|
|
| 3 |
H |
0.365 |
|
|
|
| 4 |
H |
0.365 |
|
|
|
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 |
-7.599 |
3.480 |
0.000 |
| y |
3.480 |
-10.950 |
0.000 |
| z |
0.000 |
0.000 |
-12.111 |
|
| Traceless |
| | x | y | z |
| x |
3.932 |
3.480 |
0.000 |
| y |
3.480 |
-1.095 |
0.000 |
| z |
0.000 |
0.000 |
-2.836 |
|
| Polar |
| 3z2-r2 | -5.673 |
| x2-y2 | 3.351 |
| xy | 3.480 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.621 |
0.438 |
0.000 |
| y |
0.438 |
1.926 |
0.000 |
| z |
0.000 |
0.000 |
0.189 |
<r2> (average value of r
2) Å
2
| <r2> |
19.491 |
| (<r2>)1/2 |
4.415 |