Jump to
S1C2
S2C1
S2C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -131.363430 |
| Energy at 298.15K | -131.362728 |
| HF Energy | -131.363430 |
| Nuclear repulsion energy | 47.361551 |
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 B1B95/6-31G*
| 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' |
3429 |
3255 |
36.35 |
|
|
|
| 2 |
A' |
1815 |
1723 |
32.98 |
|
|
|
| 3 |
A' |
1255 |
1192 |
7.64 |
|
|
|
| 4 |
A' |
472 |
448 |
22.18 |
|
|
|
| 5 |
A' |
378 |
359 |
30.85 |
|
|
|
| 6 |
A" |
451 |
428 |
1.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3899.5 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 3701.8 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.085 |
-1.218 |
0.000 |
| C2 |
0.000 |
0.085 |
0.000 |
| N3 |
-0.164 |
1.275 |
0.000 |
| H4 |
0.640 |
-2.133 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3057 | 2.5054 | 1.0704 |
C2 | 1.3057 | | 1.2013 | 2.3084 | N3 | 2.5054 | 1.2013 | | 3.5015 | H4 | 1.0704 | 2.3084 | 3.5015 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.870 |
|
C2 |
C1 |
H4 |
152.450 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -131.362901 |
| Energy at 298.15K | |
| HF Energy | -131.362901 |
| Nuclear repulsion energy | 47.415453 |
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 B1B95/6-31G*
| 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 |
3484 |
3308 |
65.05 |
|
|
|
| 2 |
Σ |
1749 |
1661 |
37.10 |
|
|
|
| 3 |
Σ |
1297 |
1231 |
5.21 |
|
|
|
| 4 |
Π |
453 |
430 |
0.90 |
|
|
|
| 4 |
Π |
453 |
430 |
0.90 |
|
|
|
| 5 |
Π |
268i |
254i |
52.52 |
|
|
|
| 5 |
Π |
268i |
254i |
52.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3450.2 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 3275.3 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 B1B95/6-31G*
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 |
0.080 |
| N3 |
0.000 |
0.000 |
1.291 |
| H4 |
0.000 |
0.000 |
-2.274 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2880 | 2.4984 | 1.0660 |
C2 | 1.2880 | | 1.2104 | 2.3540 | N3 | 2.4984 | 1.2104 | | 3.5644 | H4 | 1.0660 | 2.3540 | 3.5644 | |
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 B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.105 |
|
|
|
| 2 |
C |
0.299 |
|
|
|
| 3 |
N |
-0.456 |
|
|
|
| 4 |
H |
0.262 |
|
|
|
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 |
-3.276 |
3.276 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.855 |
0.000 |
0.000 |
| y |
0.000 |
-16.855 |
0.000 |
| z |
0.000 |
0.000 |
-15.039 |
|
| Traceless |
| | x | y | z |
| x |
-0.908 |
0.000 |
0.000 |
| y |
0.000 |
-0.908 |
0.000 |
| z |
0.000 |
0.000 |
1.816 |
|
| Polar |
| 3z2-r2 | 3.633 |
| 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 |
1.620 |
0.000 |
0.000 |
| y |
0.000 |
1.620 |
0.000 |
| z |
0.000 |
0.000 |
6.158 |
<r2> (average value of r
2) Å
2
| <r2> |
35.770 |
| (<r2>)1/2 |
5.981 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -131.335951 |
| Energy at 298.15K | -131.335385 |
| HF Energy | -131.335951 |
| Nuclear repulsion energy | 47.025785 |
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 B1B95/6-31G*
| 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' |
3101 |
2944 |
13.01 |
|
|
|
| 2 |
A' |
2138 |
2030 |
18.68 |
|
|
|
| 3 |
A' |
1106 |
1050 |
38.06 |
|
|
|
| 4 |
A' |
943 |
896 |
47.96 |
|
|
|
| 5 |
A' |
444 |
421 |
22.88 |
|
|
|
| 6 |
A" |
319 |
303 |
10.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4025.0 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 3821.0 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.117 |
-1.277 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.267 |
1.242 |
0.000 |
| H4 |
1.173 |
-1.583 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3740 | 2.5479 | 1.0994 |
C2 | 1.3740 | | 1.1804 | 2.0447 | N3 | 2.5479 | 1.1804 | | 3.1707 | H4 | 1.0994 | 2.0447 | 3.1707 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.118 |
|
|
|
| 2 |
C |
0.305 |
|
|
|
| 3 |
N |
-0.394 |
|
|
|
| 4 |
H |
0.206 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.801 |
-1.325 |
0.000 |
2.236 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.464 |
-2.211 |
0.000 |
| y |
-2.211 |
-20.751 |
0.000 |
| z |
0.000 |
0.000 |
-15.517 |
|
| Traceless |
| | x | y | z |
| x |
1.670 |
-2.211 |
0.000 |
| y |
-2.211 |
-4.760 |
0.000 |
| z |
0.000 |
0.000 |
3.091 |
|
| Polar |
| 3z2-r2 | 6.181 |
| x2-y2 | 4.287 |
| xy | -2.211 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.434 |
-0.900 |
0.000 |
| y |
-0.900 |
6.006 |
0.000 |
| z |
0.000 |
0.000 |
2.169 |
<r2> (average value of r
2) Å
2
| <r2> |
36.071 |
| (<r2>)1/2 |
6.006 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -131.335951 |
| Energy at 298.15K | -131.335385 |
| HF Energy | -131.335951 |
| Nuclear repulsion energy | 47.025785 |
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 B1B95/6-31G*
Geometric Data calculated at B1B95/6-31G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability