Jump to
S1C2
Energy calculated at B3LYP/6-31+G**
| | hartrees |
| Energy at 0K | -135.192570 |
| Energy at 298.15K | -135.200691 |
| Nuclear repulsion energy | 82.455879 |
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 B3LYP/6-31+G**
| 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' |
3497 |
3372 |
1.20 |
|
|
|
| 2 |
A' |
3092 |
2982 |
51.04 |
|
|
|
| 3 |
A' |
3039 |
2931 |
35.89 |
|
|
|
| 4 |
A' |
3022 |
2914 |
29.18 |
|
|
|
| 5 |
A' |
1668 |
1609 |
30.73 |
|
|
|
| 6 |
A' |
1508 |
1454 |
3.14 |
|
|
|
| 7 |
A' |
1491 |
1437 |
0.29 |
|
|
|
| 8 |
A' |
1414 |
1363 |
10.85 |
|
|
|
| 9 |
A' |
1382 |
1333 |
15.96 |
|
|
|
| 10 |
A' |
1142 |
1101 |
10.91 |
|
|
|
| 11 |
A' |
1062 |
1024 |
32.03 |
|
|
|
| 12 |
A' |
887 |
855 |
16.46 |
|
|
|
| 13 |
A' |
828 |
799 |
183.18 |
|
|
|
| 14 |
A' |
402 |
388 |
8.72 |
|
|
|
| 15 |
A" |
3586 |
3458 |
0.72 |
|
|
|
| 16 |
A" |
3100 |
2989 |
67.55 |
|
|
|
| 17 |
A" |
3070 |
2960 |
3.97 |
|
|
|
| 18 |
A" |
1498 |
1445 |
8.86 |
|
|
|
| 19 |
A" |
1386 |
1336 |
0.12 |
|
|
|
| 20 |
A" |
1268 |
1222 |
0.01 |
|
|
|
| 21 |
A" |
1003 |
968 |
1.10 |
|
|
|
| 22 |
A" |
778 |
750 |
0.78 |
|
|
|
| 23 |
A" |
288 |
278 |
39.15 |
|
|
|
| 24 |
A" |
251 |
242 |
16.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20331.2 cm
-1
Scaled (by 0.9642) Zero Point Vibrational Energy (zpe) 19603.4 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 B3LYP/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.311 |
-0.087 |
0.000 |
| C2 |
0.000 |
0.572 |
0.000 |
| C3 |
1.222 |
-0.356 |
0.000 |
| H4 |
2.157 |
0.218 |
0.000 |
| H5 |
1.225 |
-1.003 |
0.886 |
| H6 |
1.225 |
-1.003 |
-0.886 |
| H7 |
0.037 |
1.230 |
-0.877 |
| H8 |
0.037 |
1.230 |
0.877 |
| H9 |
-1.421 |
-0.680 |
0.818 |
| H10 |
-1.421 |
-0.680 |
-0.818 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4667 | 2.5471 | 3.4808 | 2.8383 | 2.8383 | 2.0780 | 2.0780 | 1.0171 | 1.0171 |
C2 | 1.4667 | | 1.5348 | 2.1857 | 2.1834 | 2.1834 | 1.0967 | 1.0967 | 2.0632 | 2.0632 | C3 | 2.5471 | 1.5348 | | 1.0971 | 1.0968 | 1.0968 | 2.1654 | 2.1654 | 2.7859 | 2.7859 | H4 | 3.4808 | 2.1857 | 1.0971 | | 1.7730 | 1.7730 | 2.5071 | 2.5071 | 3.7786 | 3.7786 | H5 | 2.8383 | 2.1834 | 1.0968 | 1.7730 | | 1.7718 | 3.0830 | 2.5294 | 2.6669 | 3.1643 | H6 | 2.8383 | 2.1834 | 1.0968 | 1.7730 | 1.7718 | | 2.5294 | 3.0830 | 3.1643 | 2.6669 | H7 | 2.0780 | 1.0967 | 2.1654 | 2.5071 | 3.0830 | 2.5294 | | 1.7534 | 2.9407 | 2.4036 | H8 | 2.0780 | 1.0967 | 2.1654 | 2.5071 | 2.5294 | 3.0830 | 1.7534 | | 2.4036 | 2.9407 | H9 | 1.0171 | 2.0632 | 2.7859 | 3.7786 | 2.6669 | 3.1643 | 2.9407 | 2.4036 | | 1.6370 | H10 | 1.0171 | 2.0632 | 2.7859 | 3.7786 | 3.1643 | 2.6669 | 2.4036 | 2.9407 | 1.6370 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.106 |
|
N1 |
C2 |
H7 |
107.434 |
| N1 |
C2 |
H8 |
107.434 |
|
C2 |
N1 |
H9 |
111.039 |
| C2 |
N1 |
H10 |
111.039 |
|
C2 |
C3 |
H4 |
111.205 |
| C2 |
C3 |
H5 |
111.034 |
|
C2 |
C3 |
H6 |
111.034 |
| C3 |
C2 |
H7 |
109.625 |
|
C3 |
C2 |
H8 |
109.625 |
| H4 |
C3 |
H5 |
107.833 |
|
H4 |
C3 |
H6 |
107.833 |
| H5 |
C3 |
H6 |
107.745 |
|
H7 |
C2 |
H8 |
106.137 |
| H9 |
N1 |
H10 |
107.173 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.611 |
|
|
-1.076 |
| 2 |
C |
-0.172 |
|
|
0.554 |
| 3 |
C |
-0.485 |
|
|
-0.383 |
| 4 |
H |
0.143 |
|
|
0.060 |
| 5 |
H |
0.143 |
|
|
0.082 |
| 6 |
H |
0.143 |
|
|
0.082 |
| 7 |
H |
0.140 |
|
|
-0.036 |
| 8 |
H |
0.140 |
|
|
-0.036 |
| 9 |
H |
0.280 |
|
|
0.376 |
| 10 |
H |
0.280 |
|
|
0.376 |
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.050 |
-0.978 |
0.000 |
1.435 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.971 |
-0.984 |
0.000 |
1.383 |
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.539 |
-0.065 |
-0.057 |
| y |
-0.065 |
5.074 |
0.110 |
| z |
-0.057 |
0.110 |
4.802 |
<r2> (average value of r
2) Å
2
| <r2> |
59.454 |
| (<r2>)1/2 |
7.711 |
Jump to
S1C1
Energy calculated at B3LYP/6-31+G**
| | hartrees |
| Energy at 0K | -135.192453 |
| Energy at 298.15K | |
| Nuclear repulsion energy | |
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 B3LYP/6-31+G**
Geometric Data calculated at B3LYP/6-31+G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability