Jump to
S1C2
S2C1
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -130.710179 |
| Energy at 298.15K | -130.709574 |
| HF Energy | -130.710179 |
| Nuclear repulsion energy | 47.374760 |
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/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' |
3471 |
3153 |
19.82 |
|
|
|
| 2 |
A' |
1660 |
1508 |
128.71 |
|
|
|
| 3 |
A' |
1202 |
1092 |
4.24 |
|
|
|
| 4 |
A' |
621 |
564 |
21.03 |
|
|
|
| 5 |
A' |
393 |
357 |
0.68 |
|
|
|
| 6 |
A" |
421 |
383 |
0.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3883.6 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 3528.2 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 HF/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.200 |
-1.214 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.306 |
1.244 |
0.000 |
| H4 |
0.943 |
-1.976 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3208 | 2.5094 | 1.0641 |
C2 | 1.3208 | | 1.1923 | 2.2724 | N3 | 2.5094 | 1.1923 | | 3.4537 | H4 | 1.0641 | 2.2724 | 3.4537 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
173.832 |
|
C2 |
C1 |
H4 |
144.446 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -130.708221 |
| Energy at 298.15K | |
| HF Energy | -130.708221 |
| Nuclear repulsion energy | 47.469583 |
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/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 |
3547 |
3222 |
60.72 |
|
|
|
| 2 |
Σ |
1576 |
1432 |
116.88 |
|
|
|
| 3 |
Σ |
1252 |
1137 |
0.00 |
|
|
|
| 4 |
Π |
422 |
383 |
0.05 |
|
|
|
| 4 |
Π |
422 |
383 |
0.05 |
|
|
|
| 5 |
Π |
400i |
363i |
43.58 |
|
|
|
| 5 |
Π |
400i |
363i |
43.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3209.0 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 2915.4 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/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.207 |
| C2 |
0.000 |
0.000 |
0.079 |
| N3 |
0.000 |
0.000 |
1.290 |
| H4 |
0.000 |
0.000 |
-2.264 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2860 | 2.4969 | 1.0575 |
C2 | 1.2860 | | 1.2109 | 2.3435 | N3 | 2.4969 | 1.2109 | | 3.5544 | H4 | 1.0575 | 2.3435 | 3.5544 | |
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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.066 |
|
|
|
| 2 |
C |
0.045 |
|
|
|
| 3 |
N |
-0.282 |
|
|
|
| 4 |
H |
0.171 |
|
|
|
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 |
-3.169 |
3.169 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.358 |
0.000 |
0.000 |
| y |
0.000 |
-17.358 |
0.000 |
| z |
0.000 |
0.000 |
-15.687 |
|
| Traceless |
| | x | y | z |
| x |
-0.835 |
0.000 |
0.000 |
| y |
0.000 |
-0.835 |
0.000 |
| z |
0.000 |
0.000 |
1.671 |
|
| Polar |
| 3z2-r2 | 3.341 |
| 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 |
1.890 |
0.000 |
0.000 |
| y |
0.000 |
1.890 |
0.000 |
| z |
0.000 |
0.000 |
5.726 |
<r2> (average value of r
2) Å
2
| <r2> |
36.046 |
| (<r2>)1/2 |
6.004 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -130.650222 |
| Energy at 298.15K | -130.649773 |
| HF Energy | -130.650222 |
| Nuclear repulsion energy | 47.435496 |
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/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' |
3230 |
2935 |
7.95 |
|
|
|
| 2 |
A' |
2353 |
2137 |
35.99 |
|
|
|
| 3 |
A' |
1136 |
1032 |
68.71 |
|
|
|
| 4 |
A' |
1020 |
927 |
19.61 |
|
|
|
| 5 |
A' |
486 |
441 |
27.63 |
|
|
|
| 6 |
A" |
364 |
331 |
15.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4294.2 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 3901.3 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.251 |
-1.270 |
0.000 |
| C2 |
0.000 |
0.112 |
0.000 |
| N3 |
0.115 |
1.248 |
0.000 |
| H4 |
0.703 |
-1.795 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.4045 | 2.5444 | 1.0889 |
C2 | 1.4045 | | 1.1419 | 2.0327 | N3 | 2.5444 | 1.1419 | | 3.0998 | H4 | 1.0889 | 2.0327 | 3.0998 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.050 |
|
|
|
| 2 |
C |
0.090 |
|
|
|
| 3 |
N |
-0.289 |
|
|
|
| 4 |
H |
0.149 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.452 |
-2.113 |
0.000 |
2.564 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.546 |
-3.498 |
0.000 |
| y |
-3.498 |
-20.326 |
0.000 |
| z |
0.000 |
0.000 |
-15.969 |
|
| Traceless |
| | x | y | z |
| x |
-0.398 |
-3.498 |
0.000 |
| y |
-3.498 |
-3.069 |
0.000 |
| z |
0.000 |
0.000 |
3.467 |
|
| Polar |
| 3z2-r2 | 6.934 |
| x2-y2 | 1.781 |
| xy | -3.498 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.369 |
0.209 |
0.000 |
| y |
0.209 |
5.692 |
0.000 |
| z |
0.000 |
0.000 |
2.460 |
<r2> (average value of r
2) Å
2
| <r2> |
36.260 |
| (<r2>)1/2 |
6.022 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -130.650222 |
| Energy at 298.15K | -130.649773 |
| HF Energy | -130.650222 |
| Nuclear repulsion energy | 47.435496 |
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/6-311G**
Geometric Data calculated at HF/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability