Jump to
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -130.302364 |
| Energy at 298.15K | -130.304483 |
| HF Energy | -130.302364 |
| Nuclear repulsion energy | 33.935731 |
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 B1B95/3-21G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3438 |
3289 |
5.49 |
|
|
|
| 2 |
A1 |
1688 |
1615 |
17.49 |
|
|
|
| 3 |
A1 |
1242 |
1188 |
0.60 |
|
|
|
| 4 |
B1 |
207 |
198 |
321.71 |
|
|
|
| 5 |
B2 |
3581 |
3426 |
0.94 |
|
|
|
| 6 |
B2 |
1211 |
1158 |
5.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5682.7 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 5436.6 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 B1B95/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.569 |
| O2 |
0.000 |
0.000 |
0.767 |
| H3 |
0.000 |
0.879 |
-1.076 |
| H4 |
0.000 |
-0.879 |
-1.076 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.3357 | 1.0147 | 1.0147 |
O2 | 1.3357 | | 2.0418 | 2.0418 | H3 | 1.0147 | 2.0418 | | 1.7575 | H4 | 1.0147 | 2.0418 | 1.7575 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
120.001 |
|
O2 |
N1 |
H4 |
120.001 |
| H3 |
N1 |
H4 |
119.997 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.378 |
|
|
|
| 2 |
O |
-0.281 |
|
|
|
| 3 |
H |
0.330 |
|
|
|
| 4 |
H |
0.330 |
|
|
|
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 |
-3.005 |
3.005 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.988 |
0.000 |
0.000 |
| y |
0.000 |
-9.532 |
0.000 |
| z |
0.000 |
0.000 |
-10.240 |
|
| Traceless |
| | x | y | z |
| x |
-2.102 |
0.000 |
0.000 |
| y |
0.000 |
1.582 |
0.000 |
| z |
0.000 |
0.000 |
0.520 |
|
| Polar |
| 3z2-r2 | 1.040 |
| x2-y2 | -2.456 |
| 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 |
0.458 |
0.000 |
0.000 |
| y |
0.000 |
1.214 |
0.000 |
| z |
0.000 |
0.000 |
2.395 |
<r2> (average value of r
2) Å
2
| <r2> |
17.442 |
| (<r2>)1/2 |
4.176 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -130.302364 |
| Energy at 298.15K | -130.304483 |
| HF Energy | -130.302364 |
| Nuclear repulsion energy | 33.938546 |
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 B1B95/3-21G
| 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' |
3438 |
3289 |
5.48 |
|
|
|
| 2 |
A' |
1688 |
1615 |
17.48 |
|
|
|
| 3 |
A' |
1242 |
1189 |
0.60 |
|
|
|
| 4 |
A' |
206 |
197 |
321.66 |
|
|
|
| 5 |
A" |
3581 |
3426 |
0.93 |
|
|
|
| 6 |
A" |
1211 |
1158 |
5.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5683.0 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 5436.9 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 B1B95/3-21G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.378 |
|
|
|
| 2 |
O |
-0.281 |
|
|
|
| 3 |
H |
0.330 |
|
|
|
| 4 |
H |
0.330 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
3.005 |
0.000 |
3.005 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.988 |
0.000 |
0.000 |
| y |
0.000 |
-10.241 |
0.000 |
| z |
0.000 |
0.000 |
-9.532 |
|
| Traceless |
| | x | y | z |
| x |
-2.102 |
0.000 |
0.000 |
| y |
0.000 |
0.519 |
0.000 |
| z |
0.000 |
0.000 |
1.582 |
|
| Polar |
| 3z2-r2 | 3.165 |
| x2-y2 | -1.747 |
| 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 |
0.458 |
0.000 |
0.000 |
| y |
0.000 |
2.394 |
0.000 |
| z |
0.000 |
0.000 |
1.214 |
<r2> (average value of r
2) Å
2
| <r2> |
17.441 |
| (<r2>)1/2 |
4.176 |