Jump to
S2C1
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -147.458735 |
| Energy at 298.15K | -147.458482 |
| HF Energy | -147.458735 |
| Nuclear repulsion energy | 46.691793 |
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/aug-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 |
Σg |
1286 |
1232 |
0.00 |
|
|
|
| 2 |
Σu |
1556 |
1491 |
240.69 |
|
|
|
| 3 |
Πu |
436 |
417 |
17.63 |
|
|
|
| 3 |
Πu |
436 |
417 |
17.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1857.0 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 1778.8 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/aug-cc-pVDZ
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.000 |
| N2 |
0.000 |
0.000 |
1.230 |
| N3 |
0.000 |
0.000 |
-1.230 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
N3 |
| C1 | | 1.2297 | 1.2297 |
N2 | 1.2297 | | 2.4594 | N3 | 1.2297 | 2.4594 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N2 |
C1 |
N3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.444 |
|
|
|
| 2 |
N |
-0.222 |
|
|
|
| 3 |
N |
-0.222 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.686 |
0.000 |
0.000 |
| y |
0.000 |
-15.686 |
0.000 |
| z |
0.000 |
0.000 |
-20.447 |
|
| Traceless |
| | x | y | z |
| x |
2.381 |
0.000 |
0.000 |
| y |
0.000 |
2.381 |
0.000 |
| z |
0.000 |
0.000 |
-4.762 |
|
| Polar |
| 3z2-r2 | -9.523 |
| 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 |
2.513 |
0.000 |
0.000 |
| y |
0.000 |
2.513 |
0.000 |
| z |
0.000 |
0.000 |
5.710 |
<r2> (average value of r
2) Å
2
| <r2> |
31.958 |
| (<r2>)1/2 |
5.653 |
Jump to
S1C1
Energy calculated at B1B95/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -147.404328 |
| Energy at 298.15K | -147.404053 |
| HF Energy | -147.404328 |
| Nuclear repulsion energy | 46.803332 |
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/aug-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 |
Σg |
1313 |
1258 |
0.00 |
|
|
|
| 2 |
Σu |
1864 |
1785 |
71.61 |
|
|
|
| 3 |
Πu |
564 |
540 |
7.95 |
|
|
|
| 3 |
Πu |
313 |
300 |
30.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2027.0 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 1941.7 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 B1B95/aug-cc-pVDZ
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.000 |
| N2 |
0.000 |
0.000 |
1.227 |
| N3 |
0.000 |
0.000 |
-1.227 |
Atom - Atom Distances (Å)
| |
C1 |
N2 |
N3 |
| C1 | | 1.2267 | 1.2267 |
N2 | 1.2267 | | 2.4535 | N3 | 1.2267 | 2.4535 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N2 |
C1 |
N3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.412 |
|
|
|
| 2 |
N |
-0.206 |
|
|
|
| 3 |
N |
-0.206 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.156 |
0.000 |
0.000 |
| y |
0.000 |
-14.456 |
0.000 |
| z |
0.000 |
0.000 |
-20.525 |
|
| Traceless |
| | x | y | z |
| x |
0.335 |
0.000 |
0.000 |
| y |
0.000 |
4.384 |
0.000 |
| z |
0.000 |
0.000 |
-4.719 |
|
| Polar |
| 3z2-r2 | -9.439 |
| x2-y2 | -2.699 |
| 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 |
2.467 |
0.000 |
0.000 |
| y |
0.000 |
2.498 |
0.000 |
| z |
0.000 |
0.000 |
5.864 |
<r2> (average value of r
2) Å
2
| <r2> |
31.923 |
| (<r2>)1/2 |
5.650 |