Jump to
S1C2
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -168.530312 |
| Energy at 298.15K | |
| HF Energy | -168.530312 |
| Nuclear repulsion energy | 60.628688 |
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/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3548 |
3411 |
272.76 |
24.67 |
0.27 |
0.42 |
| 2 |
Σ |
2388 |
2296 |
362.28 |
26.36 |
0.14 |
0.24 |
| 3 |
Σ |
1353 |
1300 |
116.32 |
18.63 |
0.29 |
0.45 |
| 4 |
Π |
586 |
563 |
0.23 |
0.66 |
0.75 |
0.86 |
| 4 |
Π |
586 |
563 |
0.23 |
0.66 |
0.75 |
0.86 |
| 5 |
Π |
169 |
162 |
86.07 |
2.29 |
0.75 |
0.86 |
| 5 |
Π |
169 |
162 |
86.07 |
2.29 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4399.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 4228.8 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 B1B95/cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.177 |
| N2 |
0.000 |
0.000 |
-0.015 |
| C3 |
0.000 |
0.000 |
-1.178 |
| H4 |
0.000 |
0.000 |
-2.245 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1918 | 2.3551 | 3.4224 |
N2 | 1.1918 | | 1.1632 | 2.2306 | C3 | 2.3551 | 1.1632 | | 1.0673 | H4 | 3.4224 | 2.2306 | 1.0673 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
180.000 |
|
N2 |
C3 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.292 |
|
|
|
| 2 |
N |
0.213 |
|
|
|
| 3 |
C |
-0.032 |
|
|
|
| 4 |
H |
0.110 |
|
|
|
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 |
-2.955 |
2.955 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.423 |
0.000 |
0.000 |
| y |
0.000 |
-16.423 |
0.000 |
| z |
0.000 |
0.000 |
-13.729 |
|
| Traceless |
| | x | y | z |
| x |
-1.347 |
0.000 |
0.000 |
| y |
0.000 |
-1.347 |
0.000 |
| z |
0.000 |
0.000 |
2.694 |
|
| Polar |
| 3z2-r2 | 5.388 |
| x2-y2 | 0.000 |
| 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 |
1.392 |
0.000 |
0.000 |
| y |
0.000 |
1.392 |
0.000 |
| z |
0.000 |
0.000 |
5.521 |
<r2> (average value of r
2) Å
2
| <r2> |
34.150 |
| (<r2>)1/2 |
5.844 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -168.530316 |
| Energy at 298.15K | -168.530811 |
| HF Energy | -168.530316 |
| Nuclear repulsion energy | 60.634556 |
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/cc-pVDZ
| 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' |
3551 |
3414 |
272.38 |
|
|
|
| 2 |
A' |
2391 |
2298 |
362.51 |
|
|
|
| 3 |
A' |
1354 |
1302 |
116.34 |
|
|
|
| 4 |
A' |
586 |
563 |
0.25 |
|
|
|
| 5 |
A' |
176 |
169 |
86.07 |
|
|
|
| 6 |
A" |
586 |
563 |
0.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4322.2 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 4154.5 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/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.018 |
-1.177 |
0.000 |
| N2 |
0.000 |
0.015 |
0.000 |
| C3 |
0.019 |
1.178 |
0.000 |
| H4 |
0.030 |
2.245 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1916 | 2.3548 | 3.4223 |
N2 | 1.1916 | | 1.1632 | 2.2307 | C3 | 2.3548 | 1.1632 | | 1.0675 | H4 | 3.4223 | 2.2307 | 1.0675 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.937 |
|
N2 |
C3 |
H4 |
179.718 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.292 |
|
|
|
| 2 |
N |
0.214 |
|
|
|
| 3 |
C |
-0.033 |
|
|
|
| 4 |
H |
0.110 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.039 |
2.953 |
0.000 |
2.954 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.423 |
0.028 |
0.000 |
| y |
0.028 |
-13.729 |
0.000 |
| z |
0.000 |
0.000 |
-16.423 |
|
| Traceless |
| | x | y | z |
| x |
-1.346 |
0.028 |
0.000 |
| y |
0.028 |
2.693 |
0.000 |
| z |
0.000 |
0.000 |
-1.347 |
|
| Polar |
| 3z2-r2 | -2.693 |
| x2-y2 | -2.693 |
| xy | 0.028 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.393 |
0.064 |
0.000 |
| y |
0.064 |
5.520 |
0.000 |
| z |
0.000 |
0.000 |
1.392 |
<r2> (average value of r
2) Å
2
| <r2> |
34.145 |
| (<r2>)1/2 |
5.843 |