Jump to
S1C2
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -130.470118 |
| Energy at 298.15K | -130.472234 |
| HF Energy | -130.470118 |
| Nuclear repulsion energy | 35.234739 |
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 LSDA/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3286 |
3246 |
2.93 |
|
|
|
| 2 |
A1 |
1628 |
1608 |
7.01 |
|
|
|
| 3 |
A1 |
1429 |
1412 |
20.28 |
|
|
|
| 4 |
B1 |
195 |
193 |
188.43 |
|
|
|
| 5 |
B2 |
3383 |
3342 |
0.07 |
|
|
|
| 6 |
B2 |
1245 |
1230 |
3.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5583.3 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 5514.7 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 LSDA/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.532 |
| O2 |
0.000 |
0.000 |
0.730 |
| H3 |
0.000 |
0.885 |
-1.058 |
| H4 |
0.000 |
-0.885 |
-1.058 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.2614 | 1.0293 | 1.0293 |
O2 | 1.2614 | | 1.9944 | 1.9944 | H3 | 1.0293 | 1.9944 | | 1.7693 | H4 | 1.0293 | 1.9944 | 1.7693 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
120.738 |
|
O2 |
N1 |
H4 |
120.738 |
| H3 |
N1 |
H4 |
118.525 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.177 |
|
|
|
| 2 |
O |
-0.287 |
|
|
|
| 3 |
H |
0.232 |
|
|
|
| 4 |
H |
0.232 |
|
|
|
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 |
-3.105 |
3.105 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.375 |
0.000 |
0.000 |
| y |
0.000 |
-9.946 |
0.000 |
| z |
0.000 |
0.000 |
-10.950 |
|
| Traceless |
| | x | y | z |
| x |
-1.926 |
0.000 |
0.000 |
| y |
0.000 |
1.716 |
0.000 |
| z |
0.000 |
0.000 |
0.210 |
|
| Polar |
| 3z2-r2 | 0.420 |
| x2-y2 | -2.428 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.017 |
0.000 |
0.000 |
| y |
0.000 |
1.626 |
0.000 |
| z |
0.000 |
0.000 |
2.731 |
<r2> (average value of r
2) Å
2
| <r2> |
16.969 |
| (<r2>)1/2 |
4.119 |
Jump to
S1C1
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -130.470118 |
| Energy at 298.15K | -130.472232 |
| HF Energy | -130.470118 |
| Nuclear repulsion energy | 35.233872 |
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 LSDA/6-311G**
| 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' |
3288 |
3247 |
2.91 |
|
|
|
| 2 |
A' |
1628 |
1608 |
7.00 |
|
|
|
| 3 |
A' |
1429 |
1411 |
20.25 |
|
|
|
| 4 |
A' |
194 |
191 |
188.45 |
|
|
|
| 5 |
A" |
3385 |
3343 |
0.07 |
|
|
|
| 6 |
A" |
1245 |
1229 |
3.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5583.5 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 5514.8 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 LSDA/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.000 |
0.532 |
0.000 |
| O2 |
-0.000 |
-0.730 |
0.000 |
| H3 |
0.001 |
1.058 |
0.884 |
| H4 |
0.001 |
1.058 |
-0.884 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.2615 | 1.0291 | 1.0291 |
O2 | 1.2615 | | 1.9946 | 1.9946 | H3 | 1.0291 | 1.9946 | | 1.7687 | H4 | 1.0291 | 1.9946 | 1.7687 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
120.761 |
|
O2 |
N1 |
H4 |
120.761 |
| H3 |
N1 |
H4 |
118.478 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.177 |
|
|
|
| 2 |
O |
-0.287 |
|
|
|
| 3 |
H |
0.232 |
|
|
|
| 4 |
H |
0.232 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.005 |
3.106 |
0.000 |
3.106 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.374 |
0.005 |
0.000 |
| y |
0.005 |
-10.948 |
0.000 |
| z |
0.000 |
0.000 |
-9.948 |
|
| Traceless |
| | x | y | z |
| x |
-1.926 |
0.005 |
0.000 |
| y |
0.005 |
0.214 |
0.000 |
| z |
0.000 |
0.000 |
1.713 |
|
| Polar |
| 3z2-r2 | 3.425 |
| x2-y2 | -1.427 |
| xy | 0.005 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.017 |
0.001 |
0.000 |
| y |
0.001 |
2.731 |
0.000 |
| z |
0.000 |
0.000 |
1.626 |
<r2> (average value of r
2) Å
2
| <r2> |
16.970 |
| (<r2>)1/2 |
4.119 |