Jump to
S1C2
S2C1
S2C2
Energy calculated at BLYP/6-311G*
| | hartrees |
| Energy at 0K | -131.423804 |
| Energy at 298.15K | -131.423054 |
| HF Energy | -131.423804 |
| Nuclear repulsion energy | 47.131868 |
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 BLYP/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' |
3312 |
3304 |
31.60 |
|
|
|
| 2 |
A' |
1766 |
1762 |
21.01 |
|
|
|
| 3 |
A' |
1216 |
1213 |
3.19 |
|
|
|
| 4 |
A' |
451 |
450 |
11.76 |
|
|
|
| 5 |
A' |
352 |
351 |
47.30 |
|
|
|
| 6 |
A" |
443 |
442 |
1.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3770.1 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 3760.7 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.058 |
-1.221 |
0.000 |
| C2 |
0.000 |
0.082 |
0.000 |
| N3 |
-0.129 |
1.288 |
0.000 |
| H4 |
0.551 |
-2.176 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3045 | 2.5161 | 1.0748 |
C2 | 1.3045 | | 1.2128 | 2.3246 | N3 | 2.5161 | 1.2128 | | 3.5303 | H4 | 1.0748 | 2.3246 | 3.5303 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.468 |
|
C2 |
C1 |
H4 |
155.265 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at BLYP/6-311G*
| | hartrees |
| Energy at 0K | -131.423455 |
| Energy at 298.15K | |
| HF Energy | -131.423455 |
| Nuclear repulsion energy | 47.177227 |
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 BLYP/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 |
3365 |
3357 |
55.05 |
|
|
|
| 2 |
Σ |
1742 |
1737 |
20.14 |
|
|
|
| 3 |
Σ |
1239 |
1236 |
2.57 |
|
|
|
| 4 |
Π |
445 |
443 |
0.56 |
|
|
|
| 4 |
Π |
445 |
443 |
0.56 |
|
|
|
| 5 |
Π |
248i |
248i |
52.52 |
|
|
|
| 5 |
Π |
248i |
248i |
52.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3368.9 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 3360.5 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 BLYP/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.213 |
| C2 |
0.000 |
0.000 |
0.079 |
| N3 |
0.000 |
0.000 |
1.298 |
| H4 |
0.000 |
0.000 |
-2.284 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2924 | 2.5108 | 1.0706 |
C2 | 1.2924 | | 1.2184 | 2.3630 | N3 | 2.5108 | 1.2184 | | 3.5814 | H4 | 1.0706 | 2.3630 | 3.5814 | |
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 BLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.080 |
|
|
|
| 2 |
C |
-0.007 |
|
|
|
| 3 |
N |
-0.179 |
|
|
|
| 4 |
H |
0.266 |
|
|
|
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 |
-17.308 |
0.000 |
0.000 |
| y |
0.000 |
-17.308 |
0.000 |
| z |
0.000 |
0.000 |
-15.569 |
|
| Traceless |
| | x | y | z |
| x |
-0.869 |
0.000 |
0.000 |
| y |
0.000 |
-0.869 |
0.000 |
| z |
0.000 |
0.000 |
1.738 |
|
| Polar |
| 3z2-r2 | 3.477 |
| 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 |
1.930 |
0.000 |
0.000 |
| y |
0.000 |
1.930 |
0.000 |
| z |
0.000 |
0.000 |
6.498 |
<r2> (average value of r
2) Å
2
| <r2> |
36.319 |
| (<r2>)1/2 |
6.027 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at BLYP/6-311G*
| | hartrees |
| Energy at 0K | -131.402445 |
| Energy at 298.15K | -131.401873 |
| HF Energy | -131.402445 |
| Nuclear repulsion energy | 46.750611 |
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 BLYP/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' |
2979 |
2972 |
15.52 |
|
|
|
| 2 |
A' |
2001 |
1996 |
15.96 |
|
|
|
| 3 |
A' |
1076 |
1073 |
27.41 |
|
|
|
| 4 |
A' |
913 |
911 |
57.67 |
|
|
|
| 5 |
A' |
451 |
449 |
20.96 |
|
|
|
| 6 |
A" |
312 |
311 |
8.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3865.6 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 3855.9 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.243 |
-1.260 |
0.000 |
| C2 |
0.000 |
0.091 |
0.000 |
| N3 |
-0.398 |
1.216 |
0.000 |
| H4 |
1.325 |
-1.493 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3730 | 2.5579 | 1.1066 |
C2 | 1.3730 | | 1.1932 | 2.0652 | N3 | 2.5579 | 1.1932 | | 3.2105 | H4 | 1.1066 | 2.0652 | 3.2105 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.152 |
|
|
|
| 2 |
C |
0.080 |
|
|
|
| 3 |
N |
-0.161 |
|
|
|
| 4 |
H |
0.232 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.878 |
-1.069 |
0.000 |
2.161 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.544 |
-1.771 |
0.000 |
| y |
-1.771 |
-21.566 |
0.000 |
| z |
0.000 |
0.000 |
-15.900 |
|
| Traceless |
| | x | y | z |
| x |
2.189 |
-1.771 |
0.000 |
| y |
-1.771 |
-5.344 |
0.000 |
| z |
0.000 |
0.000 |
3.155 |
|
| Polar |
| 3z2-r2 | 6.310 |
| x2-y2 | 5.023 |
| xy | -1.771 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.921 |
-1.198 |
0.000 |
| y |
-1.198 |
6.262 |
0.000 |
| z |
0.000 |
0.000 |
2.385 |
<r2> (average value of r
2) Å
2
| <r2> |
36.622 |
| (<r2>)1/2 |
6.052 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at BLYP/6-311G*
| | hartrees |
| Energy at 0K | -131.402445 |
| Energy at 298.15K | -131.401873 |
| HF Energy | -131.402445 |
| Nuclear repulsion energy | 46.750611 |
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 BLYP/6-311G*
Geometric Data calculated at BLYP/6-311G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability