Jump to
S1C2
S2C1
S2C2
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -129.956451 |
| Energy at 298.15K | -129.955571 |
| HF Energy | -129.956451 |
| Nuclear repulsion energy | 47.233945 |
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/3-21G*
| 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' |
3525 |
3182 |
28.22 |
|
|
|
| 2 |
A' |
1679 |
1516 |
67.33 |
|
|
|
| 3 |
A' |
1220 |
1101 |
0.00 |
|
|
|
| 4 |
A' |
478 |
431 |
0.22 |
|
|
|
| 5 |
A' |
195 |
176 |
30.12 |
|
|
|
| 6 |
A" |
505 |
456 |
0.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3801.2 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 3431.0 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/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.055 |
-1.220 |
0.000 |
| C2 |
0.000 |
0.076 |
0.000 |
| N3 |
-0.006 |
1.293 |
0.000 |
| H4 |
0.372 |
-2.188 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2969 | 2.5133 | 1.0585 |
C2 | 1.2969 | | 1.2171 | 2.2947 | N3 | 2.5133 | 1.2171 | | 3.5019 | H4 | 1.0585 | 2.2947 | 3.5019 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
177.287 |
|
C2 |
C1 |
H4 |
153.794 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -129.956783 |
| Energy at 298.15K | -129.956230 |
| HF Energy | -129.956783 |
| Nuclear repulsion energy | 47.266132 |
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/3-21G*
| 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 |
3567 |
3219 |
50.27 |
|
|
|
| 2 |
Σ |
1652 |
1491 |
62.23 |
|
|
|
| 3 |
Σ |
1235 |
1114 |
0.72 |
|
|
|
| 4 |
Π |
557 |
503 |
8.34 |
|
|
|
| 4 |
Π |
557 |
503 |
8.34 |
|
|
|
| 5 |
Π |
333 |
300 |
46.23 |
|
|
|
| 5 |
Π |
333 |
300 |
46.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4116.6 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 3715.6 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/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.208 |
| C2 |
0.000 |
0.000 |
0.070 |
| N3 |
0.000 |
0.000 |
1.299 |
| H4 |
0.000 |
0.000 |
-2.263 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2785 | 2.5071 | 1.0549 |
C2 | 1.2785 | | 1.2286 | 2.3334 | N3 | 2.5071 | 1.2286 | | 3.5620 | H4 | 1.0549 | 2.3334 | 3.5620 | |
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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.021 |
|
|
|
| 2 |
C |
0.086 |
|
|
|
| 3 |
N |
-0.470 |
|
|
|
| 4 |
H |
0.362 |
|
|
|
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 |
-3.041 |
3.041 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.340 |
0.000 |
0.000 |
| y |
0.000 |
-17.340 |
0.000 |
| z |
0.000 |
0.000 |
-16.122 |
|
| Traceless |
| | x | y | z |
| x |
-0.609 |
0.000 |
0.000 |
| y |
0.000 |
-0.609 |
0.000 |
| z |
0.000 |
0.000 |
1.218 |
|
| Polar |
| 3z2-r2 | 2.436 |
| 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 |
1.261 |
0.000 |
0.000 |
| y |
0.000 |
1.261 |
0.000 |
| z |
0.000 |
0.000 |
4.826 |
<r2> (average value of r
2) Å
2
| <r2> |
36.297 |
| (<r2>)1/2 |
6.025 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -129.881329 |
| Energy at 298.15K | -129.881021 |
| HF Energy | -129.881329 |
| Nuclear repulsion energy | 47.361352 |
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/3-21G*
| 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' |
3208 |
2896 |
10.79 |
|
|
|
| 2 |
A' |
2318 |
2092 |
32.16 |
|
|
|
| 3 |
A' |
1159 |
1047 |
110.18 |
|
|
|
| 4 |
A' |
967 |
873 |
0.97 |
|
|
|
| 5 |
A' |
533 |
481 |
31.62 |
|
|
|
| 6 |
A" |
496 |
448 |
9.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4340.7 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 3917.9 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/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.219 |
-1.265 |
0.000 |
| C2 |
0.000 |
0.106 |
0.000 |
| N3 |
0.087 |
1.256 |
0.000 |
| H4 |
0.706 |
-1.839 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3888 | 2.5400 | 1.0885 |
C2 | 1.3888 | | 1.1534 | 2.0695 | N3 | 2.5400 | 1.1534 | | 3.1568 | H4 | 1.0885 | 2.0695 | 3.1568 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.044 |
|
|
|
| 2 |
C |
0.159 |
|
|
|
| 3 |
N |
-0.444 |
|
|
|
| 4 |
H |
0.241 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.690 |
-1.901 |
0.000 |
2.543 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.566 |
-3.683 |
0.000 |
| y |
-3.683 |
-20.486 |
0.000 |
| z |
0.000 |
0.000 |
-15.941 |
|
| Traceless |
| | x | y | z |
| x |
-0.353 |
-3.683 |
0.000 |
| y |
-3.683 |
-3.232 |
0.000 |
| z |
0.000 |
0.000 |
3.585 |
|
| Polar |
| 3z2-r2 | 7.169 |
| x2-y2 | 1.920 |
| xy | -3.683 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.729 |
-0.001 |
0.000 |
| y |
-0.001 |
5.235 |
0.000 |
| z |
0.000 |
0.000 |
2.146 |
<r2> (average value of r
2) Å
2
| <r2> |
36.391 |
| (<r2>)1/2 |
6.033 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -129.881329 |
| Energy at 298.15K | -129.881021 |
| HF Energy | -129.881329 |
| Nuclear repulsion energy | 47.361352 |
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/3-21G*
Geometric Data calculated at HF/3-21G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability