Jump to
S1C2
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -130.724945 |
| Energy at 298.15K | -130.724325 |
| HF Energy | -130.724945 |
| Nuclear repulsion energy | 47.489747 |
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/daug-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' |
3469 |
3138 |
19.74 |
|
|
|
| 2 |
A' |
1653 |
1495 |
147.24 |
|
|
|
| 3 |
A' |
1202 |
1087 |
5.18 |
|
|
|
| 4 |
A' |
621 |
561 |
18.38 |
|
|
|
| 5 |
A' |
388 |
351 |
0.46 |
|
|
|
| 6 |
A" |
417 |
377 |
0.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3874.5 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 3504.9 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 HF/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.199 |
-1.211 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.305 |
1.241 |
0.000 |
| H4 |
0.939 |
-1.973 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3184 | 2.5034 | 1.0620 |
C2 | 1.3184 | | 1.1886 | 2.2687 | N3 | 2.5034 | 1.1886 | | 3.4465 | H4 | 1.0620 | 2.2687 | 3.4465 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
173.827 |
|
C2 |
C1 |
H4 |
144.548 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.420 |
|
|
|
| 2 |
C |
-0.155 |
|
|
|
| 3 |
N |
-0.403 |
|
|
|
| 4 |
H |
0.978 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.134 |
-2.820 |
0.000 |
3.039 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.541 |
-1.061 |
0.000 |
| y |
-1.061 |
-17.398 |
0.000 |
| z |
0.000 |
0.000 |
-17.472 |
|
| Traceless |
| | x | y | z |
| x |
0.893 |
-1.061 |
0.000 |
| y |
-1.061 |
-0.391 |
0.000 |
| z |
0.000 |
0.000 |
-0.502 |
|
| Polar |
| 3z2-r2 | -1.004 |
| x2-y2 | 0.856 |
| xy | -1.061 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.129 |
-0.690 |
0.000 |
| y |
-0.690 |
6.019 |
0.000 |
| z |
0.000 |
0.000 |
2.955 |
<r2> (average value of r
2) Å
2
| <r2> |
36.000 |
| (<r2>)1/2 |
6.000 |
Jump to
S1C1
Energy calculated at HF/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -130.722952 |
| Energy at 298.15K | |
| HF Energy | -130.722952 |
| Nuclear repulsion energy | 47.579248 |
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/daug-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 |
Σ |
3540 |
3202 |
58.48 |
|
|
|
| 2 |
Σ |
1563 |
1414 |
135.94 |
|
|
|
| 3 |
Σ |
1255 |
1135 |
0.00 |
|
|
|
| 4 |
Π |
414 |
375 |
0.21 |
|
|
|
| 4 |
Π |
414 |
375 |
0.21 |
|
|
|
| 5 |
Π |
418i |
378i |
43.25 |
|
|
|
| 5 |
Π |
418i |
378i |
43.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3175.2 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 2872.3 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/daug-cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.204 |
| C2 |
0.000 |
0.000 |
0.079 |
| N3 |
0.000 |
0.000 |
1.287 |
| H4 |
0.000 |
0.000 |
-2.260 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2836 | 2.4911 | 1.0558 |
C2 | 1.2836 | | 1.2074 | 2.3395 | N3 | 2.4911 | 1.2074 | | 3.5469 | H4 | 1.0558 | 2.3395 | 3.5469 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
180.000 |
|
C2 |
C1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.096 |
|
|
|
| 2 |
C |
-0.203 |
|
|
|
| 3 |
N |
-0.509 |
|
|
|
| 4 |
H |
0.808 |
|
|
|
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 |
-3.209 |
3.209 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.449 |
0.000 |
0.000 |
| y |
0.000 |
-17.449 |
0.000 |
| z |
0.000 |
0.000 |
-15.699 |
|
| Traceless |
| | x | y | z |
| x |
-0.875 |
0.000 |
0.000 |
| y |
0.000 |
-0.875 |
0.000 |
| z |
0.000 |
0.000 |
1.751 |
|
| Polar |
| 3z2-r2 | 3.502 |
| 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 |
2.979 |
0.000 |
0.000 |
| y |
0.000 |
2.979 |
0.000 |
| z |
0.000 |
0.000 |
6.296 |
<r2> (average value of r
2) Å
2
| <r2> |
35.972 |
| (<r2>)1/2 |
5.998 |