Jump to
S1C2
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -130.451812 |
| Energy at 298.15K | |
| HF Energy | -130.451812 |
| Nuclear repulsion energy | 35.698091 |
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 HF/aug-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 |
A1 |
3734 |
3399 |
22.19 |
|
|
|
| 2 |
A1 |
1806 |
1644 |
40.54 |
|
|
|
| 3 |
A1 |
1479 |
1346 |
9.16 |
|
|
|
| 4 |
B1 |
414i |
377i |
234.65 |
|
|
|
| 5 |
B2 |
3900 |
3551 |
34.26 |
|
|
|
| 6 |
B2 |
1384 |
1260 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5943.8 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 5411.2 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 HF/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.534 |
| O2 |
0.000 |
0.000 |
0.722 |
| H3 |
0.000 |
0.867 |
-1.020 |
| H4 |
0.000 |
-0.867 |
-1.020 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.2565 | 0.9935 | 0.9935 |
O2 | 1.2565 | | 1.9460 | 1.9460 | H3 | 0.9935 | 1.9460 | | 1.7331 | H4 | 0.9935 | 1.9460 | 1.7331 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
119.284 |
|
O2 |
N1 |
H4 |
119.284 |
| H3 |
N1 |
H4 |
121.433 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.140 |
|
|
|
| 2 |
O |
-0.358 |
|
|
|
| 3 |
H |
0.249 |
|
|
|
| 4 |
H |
0.249 |
|
|
|
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 |
-2.808 |
2.808 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.618 |
0.000 |
0.000 |
| y |
0.000 |
-9.907 |
0.000 |
| z |
0.000 |
0.000 |
-11.083 |
|
| Traceless |
| | x | y | z |
| x |
-2.123 |
0.000 |
0.000 |
| y |
0.000 |
1.943 |
0.000 |
| z |
0.000 |
0.000 |
0.180 |
|
| Polar |
| 3z2-r2 | 0.360 |
| x2-y2 | -2.711 |
| 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 |
1.812 |
0.000 |
0.000 |
| y |
0.000 |
1.991 |
0.000 |
| z |
0.000 |
0.000 |
3.363 |
<r2> (average value of r
2) Å
2
| <r2> |
16.751 |
| (<r2>)1/2 |
4.093 |
Jump to
S1C1
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -130.452312 |
| Energy at 298.15K | -130.454809 |
| HF Energy | -130.452312 |
| Nuclear repulsion energy | 35.581756 |
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 HF/aug-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' |
3706 |
3374 |
11.69 |
|
|
|
| 2 |
A' |
1811 |
1649 |
36.37 |
|
|
|
| 3 |
A' |
1439 |
1310 |
8.23 |
|
|
|
| 4 |
A' |
540 |
492 |
251.11 |
|
|
|
| 5 |
A" |
3855 |
3510 |
22.86 |
|
|
|
| 6 |
A" |
1415 |
1288 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6383.0 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 5811.1 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 HF/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.028 |
0.541 |
0.000 |
| O2 |
-0.028 |
-0.722 |
0.000 |
| H3 |
0.211 |
0.994 |
0.855 |
| H4 |
0.211 |
0.994 |
-0.855 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.2636 | 0.9961 | 0.9961 |
O2 | 1.2636 | | 1.9318 | 1.9318 | H3 | 0.9961 | 1.9318 | | 1.7096 | H4 | 0.9961 | 1.9318 | 1.7096 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
116.998 |
|
O2 |
N1 |
H4 |
116.998 |
| H3 |
N1 |
H4 |
118.222 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.136 |
|
|
|
| 2 |
O |
-0.347 |
|
|
|
| 3 |
H |
0.242 |
|
|
|
| 4 |
H |
0.242 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.787 |
2.604 |
0.000 |
2.720 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.434 |
0.776 |
0.000 |
| y |
0.776 |
-11.316 |
0.000 |
| z |
0.000 |
0.000 |
-10.038 |
|
| Traceless |
| | x | y | z |
| x |
-1.757 |
0.776 |
0.000 |
| y |
0.776 |
-0.080 |
0.000 |
| z |
0.000 |
0.000 |
1.837 |
|
| Polar |
| 3z2-r2 | 3.673 |
| x2-y2 | -1.118 |
| xy | 0.776 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.825 |
0.018 |
0.000 |
| y |
0.018 |
3.305 |
0.000 |
| z |
0.000 |
0.000 |
2.000 |
<r2> (average value of r
2) Å
2
| <r2> |
16.795 |
| (<r2>)1/2 |
4.098 |