Jump to
S1C2
Energy calculated at B3LYP/6-31G
| | hartrees |
| Energy at 0K | -135.133642 |
| Energy at 298.15K | -135.141684 |
| Nuclear repulsion energy | 82.247851 |
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/6-31G
| 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' |
3533 |
3399 |
0.58 |
|
|
|
| 2 |
A' |
3106 |
2988 |
57.09 |
|
|
|
| 3 |
A' |
3044 |
2928 |
38.64 |
|
|
|
| 4 |
A' |
3029 |
2914 |
30.58 |
|
|
|
| 5 |
A' |
1711 |
1646 |
26.41 |
|
|
|
| 6 |
A' |
1547 |
1488 |
3.53 |
|
|
|
| 7 |
A' |
1530 |
1472 |
0.17 |
|
|
|
| 8 |
A' |
1450 |
1395 |
3.30 |
|
|
|
| 9 |
A' |
1414 |
1360 |
13.14 |
|
|
|
| 10 |
A' |
1163 |
1119 |
19.34 |
|
|
|
| 11 |
A' |
1069 |
1029 |
22.63 |
|
|
|
| 12 |
A' |
898 |
864 |
4.19 |
|
|
|
| 13 |
A' |
619 |
596 |
317.45 |
|
|
|
| 14 |
A' |
402 |
387 |
19.79 |
|
|
|
| 15 |
A" |
3649 |
3510 |
0.01 |
|
|
|
| 16 |
A" |
3113 |
2995 |
75.61 |
|
|
|
| 17 |
A" |
3078 |
2961 |
6.20 |
|
|
|
| 18 |
A" |
1539 |
1481 |
6.99 |
|
|
|
| 19 |
A" |
1397 |
1344 |
0.16 |
|
|
|
| 20 |
A" |
1290 |
1241 |
0.25 |
|
|
|
| 21 |
A" |
1013 |
975 |
0.23 |
|
|
|
| 22 |
A" |
795 |
765 |
2.55 |
|
|
|
| 23 |
A" |
279 |
268 |
38.75 |
|
|
|
| 24 |
A" |
253 |
244 |
18.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20460.3 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 19682.9 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 B3LYP/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.299 |
-0.105 |
0.000 |
| C2 |
0.000 |
0.572 |
0.000 |
| C3 |
1.233 |
-0.353 |
0.000 |
| H4 |
2.167 |
0.224 |
0.000 |
| H5 |
1.235 |
-1.000 |
0.887 |
| H6 |
1.235 |
-1.000 |
-0.887 |
| H7 |
0.036 |
1.230 |
-0.877 |
| H8 |
0.036 |
1.230 |
0.877 |
| H9 |
-1.507 |
-0.632 |
0.840 |
| H10 |
-1.507 |
-0.632 |
-0.840 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4648 | 2.5442 | 3.4811 | 2.8301 | 2.8301 | 2.0820 | 2.0820 | 1.0135 | 1.0135 |
C2 | 1.4648 | | 1.5416 | 2.1943 | 2.1870 | 2.1870 | 1.0974 | 1.0974 | 2.1043 | 2.1043 | C3 | 2.5442 | 1.5416 | | 1.0977 | 1.0976 | 1.0976 | 2.1704 | 2.1704 | 2.8798 | 2.8798 | H4 | 3.4811 | 2.1943 | 1.0977 | | 1.7754 | 1.7754 | 2.5142 | 2.5142 | 3.8648 | 3.8648 | H5 | 2.8301 | 2.1870 | 1.0976 | 1.7754 | | 1.7740 | 3.0861 | 2.5320 | 2.7675 | 3.2618 | H6 | 2.8301 | 2.1870 | 1.0976 | 1.7754 | 1.7740 | | 2.5320 | 3.0861 | 3.2618 | 2.7675 | H7 | 2.0820 | 1.0974 | 2.1704 | 2.5142 | 3.0861 | 2.5320 | | 1.7546 | 2.9666 | 2.4193 | H8 | 2.0820 | 1.0974 | 2.1704 | 2.5142 | 2.5320 | 3.0861 | 1.7546 | | 2.4193 | 2.9666 | H9 | 1.0135 | 2.1043 | 2.8798 | 3.8648 | 2.7675 | 3.2618 | 2.9666 | 2.4193 | | 1.6800 | H10 | 1.0135 | 2.1043 | 2.8798 | 3.8648 | 3.2618 | 2.7675 | 2.4193 | 2.9666 | 1.6800 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.586 |
|
N1 |
C2 |
H7 |
107.839 |
| N1 |
C2 |
H8 |
107.839 |
|
C2 |
N1 |
H9 |
115.014 |
| C2 |
N1 |
H10 |
115.014 |
|
C2 |
C3 |
H4 |
111.371 |
| C2 |
C3 |
H5 |
110.798 |
|
C2 |
C3 |
H6 |
110.798 |
| C3 |
C2 |
H7 |
109.501 |
|
C3 |
C2 |
H8 |
109.501 |
| H4 |
C3 |
H5 |
107.949 |
|
H4 |
C3 |
H6 |
107.949 |
| H5 |
C3 |
H6 |
107.836 |
|
H7 |
C2 |
H8 |
106.150 |
| H9 |
N1 |
H10 |
111.960 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.688 |
|
|
|
| 2 |
C |
-0.115 |
|
|
|
| 3 |
C |
-0.401 |
|
|
|
| 4 |
H |
0.126 |
|
|
|
| 5 |
H |
0.126 |
|
|
|
| 6 |
H |
0.126 |
|
|
|
| 7 |
H |
0.139 |
|
|
|
| 8 |
H |
0.139 |
|
|
|
| 9 |
H |
0.274 |
|
|
|
| 10 |
H |
0.274 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.706 |
-1.043 |
0.000 |
1.259 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
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 |
4.798 |
-0.126 |
-0.130 |
| y |
-0.126 |
4.285 |
-0.197 |
| z |
-0.130 |
-0.197 |
3.815 |
<r2> (average value of r
2) Å
2
| <r2> |
59.413 |
| (<r2>)1/2 |
7.708 |
Jump to
S1C1
Energy calculated at B3LYP/6-31G
| | hartrees |
| Energy at 0K | -135.132800 |
| 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/6-31G
Geometric Data calculated at B3LYP/6-31G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability