Jump to
S1C2
Energy calculated at B3LYPultrafine/6-311G*
| | hartrees |
| Energy at 0K | -168.619398 |
| Energy at 298.15K | |
| HF Energy | -168.619398 |
| Nuclear repulsion energy | 60.535720 |
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 B3LYPultrafine/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 |
Σ |
3503 |
3385 |
233.04 |
23.51 |
0.27 |
0.43 |
| 2 |
Σ |
2335 |
2256 |
353.08 |
27.46 |
0.12 |
0.22 |
| 3 |
Σ |
1300 |
1256 |
120.96 |
18.40 |
0.30 |
0.46 |
| 4 |
Π |
572 |
553 |
0.53 |
0.49 |
0.75 |
0.86 |
| 4 |
Π |
572 |
553 |
0.53 |
0.49 |
0.75 |
0.86 |
| 5 |
Π |
170 |
165 |
94.98 |
5.15 |
0.75 |
0.86 |
| 5 |
Π |
170 |
165 |
94.98 |
5.15 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4311.1 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4165.8 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 B3LYPultrafine/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.181 |
| N2 |
0.000 |
0.000 |
-0.019 |
| C3 |
0.000 |
0.000 |
-1.179 |
| H4 |
0.000 |
0.000 |
-2.240 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1995 | 2.3591 | 3.4207 |
N2 | 1.1995 | | 1.1596 | 2.2212 | C3 | 2.3591 | 1.1596 | | 1.0616 | H4 | 3.4207 | 2.2212 | 1.0616 | |
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 B3LYPultrafine/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.335 |
|
|
|
| 2 |
N |
0.100 |
|
|
|
| 3 |
C |
-0.082 |
|
|
|
| 4 |
H |
0.317 |
|
|
|
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 |
-3.132 |
3.132 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.699 |
0.000 |
0.000 |
| y |
0.000 |
-16.699 |
0.000 |
| z |
0.000 |
0.000 |
-13.933 |
|
| Traceless |
| | x | y | z |
| x |
-1.383 |
0.000 |
0.000 |
| y |
0.000 |
-1.383 |
0.000 |
| z |
0.000 |
0.000 |
2.765 |
|
| Polar |
| 3z2-r2 | 5.531 |
| 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 |
1.459 |
0.000 |
0.000 |
| y |
0.000 |
1.459 |
0.000 |
| z |
0.000 |
0.000 |
5.629 |
<r2> (average value of r
2) Å
2
| <r2> |
34.358 |
| (<r2>)1/2 |
5.862 |
Jump to
S1C1
Energy calculated at B3LYPultrafine/6-311G*
| | hartrees |
| Energy at 0K | -168.619398 |
| Energy at 298.15K | -168.619856 |
| HF Energy | -168.619398 |
| Nuclear repulsion energy | 60.535488 |
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 B3LYPultrafine/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' |
3503 |
3385 |
233.04 |
|
|
|
| 2 |
A' |
2335 |
2256 |
353.07 |
|
|
|
| 3 |
A' |
1300 |
1256 |
120.96 |
|
|
|
| 4 |
A' |
572 |
553 |
0.52 |
|
|
|
| 5 |
A' |
170 |
165 |
94.98 |
|
|
|
| 6 |
A" |
567 |
548 |
0.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4223.5 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4081.2 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 B3LYPultrafine/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.000 |
-1.181 |
0.000 |
| N2 |
0.000 |
0.019 |
0.000 |
| C3 |
0.000 |
1.179 |
0.000 |
| H4 |
0.000 |
2.240 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1995 | 2.3591 | 3.4207 |
N2 | 1.1995 | | 1.1596 | 2.2212 | C3 | 2.3591 | 1.1596 | | 1.0616 | H4 | 3.4207 | 2.2212 | 1.0616 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.997 |
|
N2 |
C3 |
H4 |
179.982 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.335 |
|
|
|
| 2 |
N |
0.100 |
|
|
|
| 3 |
C |
-0.082 |
|
|
|
| 4 |
H |
0.317 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
3.132 |
0.000 |
3.132 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.699 |
-0.000 |
0.000 |
| y |
-0.000 |
-13.933 |
0.000 |
| z |
0.000 |
0.000 |
-16.699 |
|
| Traceless |
| | x | y | z |
| x |
-1.383 |
-0.000 |
0.000 |
| y |
-0.000 |
2.765 |
0.000 |
| z |
0.000 |
0.000 |
-1.383 |
|
| Polar |
| 3z2-r2 | -2.765 |
| x2-y2 | -2.765 |
| 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 |
1.459 |
0.001 |
0.000 |
| y |
0.001 |
5.629 |
0.000 |
| z |
0.000 |
0.000 |
1.459 |
<r2> (average value of r
2) Å
2
| <r2> |
34.358 |
| (<r2>)1/2 |
5.862 |