Jump to
S1C2
S2C1
S2C2
Energy calculated at B2PLYP/STO-3G
| | hartrees |
| Energy at 0K | -129.539743 |
| Energy at 298.15K | -129.538946 |
| HF Energy | -129.488047 |
| Nuclear repulsion energy | 46.097416 |
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 B2PLYP/STO-3G
| 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' |
3539 |
3539 |
38.16 |
|
|
|
| 2 |
A' |
1636 |
1636 |
84.18 |
|
|
|
| 3 |
A' |
1138 |
1138 |
26.35 |
|
|
|
| 4 |
A' |
606 |
606 |
1.54 |
|
|
|
| 5 |
A' |
353 |
353 |
0.94 |
|
|
|
| 6 |
A" |
427 |
427 |
1.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3849.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3849.7 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 B2PLYP/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.077 |
-1.264 |
0.000 |
| C2 |
0.000 |
0.085 |
0.000 |
| N3 |
-0.186 |
1.303 |
0.000 |
| H4 |
0.840 |
-2.048 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3503 | 2.5801 | 1.0941 |
C2 | 1.3503 | | 1.2327 | 2.2917 | N3 | 2.5801 | 1.2327 | | 3.5043 | H4 | 1.0941 | 2.2917 | 3.5043 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
174.590 |
|
C2 |
C1 |
H4 |
139.042 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B2PLYP/STO-3G
| | hartrees |
| Energy at 0K | -129.539775 |
| Energy at 298.15K | -129.538807 |
| HF Energy | -129.490748 |
| Nuclear repulsion energy | 46.069338 |
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 B2PLYP/STO-3G
| 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 |
3663 |
3663 |
117.52 |
|
|
|
| 2 |
Σ |
1506 |
1506 |
74.05 |
|
|
|
| 3 |
Σ |
969 |
969 |
117.39 |
|
|
|
| 4 |
Π |
429 |
429 |
3.48 |
|
|
|
| 4 |
Π |
429 |
429 |
3.48 |
|
|
|
| 5 |
Π |
335 |
335 |
14.51 |
|
|
|
| 5 |
Π |
335 |
335 |
14.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3832.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3832.8 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 B2PLYP/STO-3G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.222 |
| C2 |
0.000 |
0.000 |
0.036 |
| N3 |
0.000 |
0.000 |
1.346 |
| H4 |
0.000 |
0.000 |
-2.304 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2588 | 2.5681 | 1.0818 |
C2 | 1.2588 | | 1.3093 | 2.3406 | N3 | 2.5681 | 1.3093 | | 3.6499 | H4 | 1.0818 | 2.3406 | 3.6499 | |
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 B2PLYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.058 |
|
|
|
| 2 |
C |
0.013 |
|
|
|
| 3 |
N |
-0.090 |
|
|
|
| 4 |
H |
0.136 |
|
|
|
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 |
-2.368 |
2.368 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.362 |
0.000 |
0.000 |
| y |
0.000 |
-15.362 |
0.000 |
| z |
0.000 |
0.000 |
-14.462 |
|
| Traceless |
| | x | y | z |
| x |
-0.450 |
0.000 |
0.000 |
| y |
0.000 |
-0.450 |
0.000 |
| z |
0.000 |
0.000 |
0.900 |
|
| Polar |
| 3z2-r2 | 1.800 |
| 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 |
0.598 |
0.000 |
0.000 |
| y |
0.000 |
0.598 |
0.000 |
| z |
0.000 |
0.000 |
4.043 |
<r2> (average value of r
2) Å
2
| <r2> |
36.367 |
| (<r2>)1/2 |
6.030 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B2PLYP/STO-3G
| | hartrees |
| Energy at 0K | -129.509739 |
| Energy at 298.15K | -129.509012 |
| HF Energy | -129.435196 |
| Nuclear repulsion energy | 45.130149 |
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 B2PLYP/STO-3G
| 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' |
3200 |
3200 |
10.36 |
|
|
|
| 2 |
A' |
2058 |
2058 |
99.80 |
|
|
|
| 3 |
A' |
1164 |
1164 |
34.72 |
|
|
|
| 4 |
A' |
920 |
920 |
8.30 |
|
|
|
| 5 |
A' |
392 |
392 |
11.34 |
|
|
|
| 6 |
A" |
315 |
315 |
2.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4023.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4023.8 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 B2PLYP/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.373 |
-1.294 |
0.000 |
| C2 |
0.000 |
0.103 |
0.000 |
| N3 |
-0.536 |
1.206 |
0.000 |
| H4 |
1.513 |
-1.298 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.4460 | 2.6598 | 1.1398 |
C2 | 1.4460 | | 1.2259 | 2.0620 | N3 | 2.6598 | 1.2259 | | 3.2351 | H4 | 1.1398 | 2.0620 | 3.2351 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.021 |
|
|
|
| 2 |
C |
0.020 |
|
|
|
| 3 |
N |
-0.115 |
|
|
|
| 4 |
H |
0.074 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.655 |
-0.720 |
0.000 |
1.805 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.864 |
-0.461 |
0.000 |
| y |
-0.461 |
-20.122 |
0.000 |
| z |
0.000 |
0.000 |
-14.269 |
|
| Traceless |
| | x | y | z |
| x |
2.332 |
-0.461 |
0.000 |
| y |
-0.461 |
-5.556 |
0.000 |
| z |
0.000 |
0.000 |
3.224 |
|
| Polar |
| 3z2-r2 | 6.448 |
| x2-y2 | 5.259 |
| xy | -0.461 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.612 |
-1.209 |
0.000 |
| y |
-1.209 |
3.296 |
0.000 |
| z |
0.000 |
0.000 |
1.169 |
<r2> (average value of r
2) Å
2
| <r2> |
37.360 |
| (<r2>)1/2 |
6.112 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B2PLYP/STO-3G
| | hartrees |
| Energy at 0K | -129.509739 |
| Energy at 298.15K | -129.509012 |
| HF Energy | -129.435196 |
| Nuclear repulsion energy | 45.130149 |
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 B2PLYP/STO-3G
Geometric Data calculated at B2PLYP/STO-3G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability