Jump to
S1C2
S2C1
S2C2
Energy calculated at B2PLYP/3-21G
| | hartrees |
| Energy at 0K | -130.524422 |
| Energy at 298.15K | -130.523850 |
| HF Energy | -130.443326 |
| Nuclear repulsion energy | 47.244126 |
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/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' |
3394 |
3394 |
23.57 |
|
|
|
| 2 |
A' |
1834 |
1834 |
20.45 |
|
|
|
| 3 |
A' |
1193 |
1193 |
9.58 |
|
|
|
| 4 |
A' |
551 |
551 |
6.92 |
|
|
|
| 5 |
A' |
374 |
374 |
31.39 |
|
|
|
| 6 |
A" |
542 |
542 |
2.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3943.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3943.4 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 B2PLYP/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.159 |
-1.221 |
0.000 |
| C2 |
0.000 |
0.088 |
0.000 |
| N3 |
0.093 |
1.283 |
0.000 |
| H4 |
0.297 |
-2.188 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3182 | 2.5163 | 1.0692 |
C2 | 1.3182 | | 1.1987 | 2.2953 | N3 | 2.5163 | 1.1987 | | 3.4770 | H4 | 1.0692 | 2.2953 | 3.4770 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
177.564 |
|
C2 |
C1 |
H4 |
147.873 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B2PLYP/3-21G
| | hartrees |
| Energy at 0K | -130.524324 |
| Energy at 298.15K | -130.523611 |
| HF Energy | -130.444674 |
| Nuclear repulsion energy | 47.343357 |
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/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 |
3472 |
3472 |
56.99 |
|
|
|
| 2 |
Σ |
1662 |
1662 |
31.38 |
|
|
|
| 3 |
Σ |
1273 |
1273 |
6.05 |
|
|
|
| 4 |
Π |
585 |
585 |
6.90 |
|
|
|
| 4 |
Π |
585 |
585 |
6.90 |
|
|
|
| 5 |
Π |
250 |
250 |
51.72 |
|
|
|
| 5 |
Π |
250 |
250 |
51.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4038.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4038.5 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 B2PLYP/3-21G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.210 |
| C2 |
0.000 |
0.000 |
0.079 |
| N3 |
0.000 |
0.000 |
1.293 |
| H4 |
0.000 |
0.000 |
-2.272 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2890 | 2.5030 | 1.0624 |
C2 | 1.2890 | | 1.2141 | 2.3514 | N3 | 2.5030 | 1.2141 | | 3.5654 | H4 | 1.0624 | 2.3514 | 3.5654 | |
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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.046 |
|
|
|
| 2 |
C |
0.101 |
|
|
|
| 3 |
N |
-0.456 |
|
|
|
| 4 |
H |
0.309 |
|
|
|
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 |
-3.114 |
3.114 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.133 |
0.000 |
0.000 |
| y |
0.000 |
-17.133 |
0.000 |
| z |
0.000 |
0.000 |
-15.750 |
|
| Traceless |
| | x | y | z |
| x |
-0.692 |
0.000 |
0.000 |
| y |
0.000 |
-0.692 |
0.000 |
| z |
0.000 |
0.000 |
1.384 |
|
| Polar |
| 3z2-r2 | 2.767 |
| 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 |
1.260 |
0.000 |
0.000 |
| y |
0.000 |
1.260 |
0.000 |
| z |
0.000 |
0.000 |
5.448 |
<r2> (average value of r
2) Å
2
| <r2> |
36.103 |
| (<r2>)1/2 |
6.009 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B2PLYP/3-21G
| | hartrees |
| Energy at 0K | -130.494780 |
| Energy at 298.15K | -130.494371 |
| HF Energy | -130.397470 |
| Nuclear repulsion energy | 46.678942 |
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/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' |
3055 |
3055 |
14.30 |
|
|
|
| 2 |
A' |
2067 |
2067 |
23.41 |
|
|
|
| 3 |
A' |
1100 |
1100 |
60.38 |
|
|
|
| 4 |
A' |
900 |
900 |
37.97 |
|
|
|
| 5 |
A' |
479 |
479 |
24.97 |
|
|
|
| 6 |
A" |
446 |
446 |
7.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4023.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4023.5 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 B2PLYP/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.056 |
-1.286 |
0.000 |
| C2 |
0.000 |
0.090 |
0.000 |
| N3 |
-0.203 |
1.266 |
0.000 |
| H4 |
1.083 |
-1.687 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3778 | 2.5653 | 1.1019 |
C2 | 1.3778 | | 1.1929 | 2.0810 | N3 | 2.5653 | 1.1929 | | 3.2204 | H4 | 1.1019 | 2.0810 | 3.2204 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.020 |
|
|
|
| 2 |
C |
0.191 |
|
|
|
| 3 |
N |
-0.398 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.843 |
-1.276 |
0.000 |
2.241 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.068 |
-2.689 |
0.000 |
| y |
-2.689 |
-21.122 |
0.000 |
| z |
0.000 |
0.000 |
-15.750 |
|
| Traceless |
| | x | y | z |
| x |
1.368 |
-2.689 |
0.000 |
| y |
-2.689 |
-4.712 |
0.000 |
| z |
0.000 |
0.000 |
3.345 |
|
| Polar |
| 3z2-r2 | 6.689 |
| x2-y2 | 4.053 |
| xy | -2.689 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.994 |
-0.737 |
0.000 |
| y |
-0.737 |
5.594 |
0.000 |
| z |
0.000 |
0.000 |
2.043 |
<r2> (average value of r
2) Å
2
| <r2> |
36.748 |
| (<r2>)1/2 |
6.062 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B2PLYP/3-21G
| | hartrees |
| Energy at 0K | -130.494780 |
| Energy at 298.15K | -130.494371 |
| HF Energy | -130.397470 |
| Nuclear repulsion energy | 46.678942 |
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/3-21G
Geometric Data calculated at B2PLYP/3-21G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability