Jump to
S1C2
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -25.421343 |
| Energy at 298.15K | -25.429446 |
| Nuclear repulsion energy | 49.631530 |
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/CEP-121G*
| 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' |
3444 |
3339 |
5.55 |
|
|
|
| 2 |
A' |
3065 |
2972 |
75.81 |
|
|
|
| 3 |
A' |
3019 |
2926 |
39.92 |
|
|
|
| 4 |
A' |
2997 |
2905 |
35.61 |
|
|
|
| 5 |
A' |
1699 |
1647 |
28.12 |
|
|
|
| 6 |
A' |
1513 |
1467 |
2.72 |
|
|
|
| 7 |
A' |
1493 |
1447 |
0.03 |
|
|
|
| 8 |
A' |
1415 |
1372 |
8.88 |
|
|
|
| 9 |
A' |
1378 |
1336 |
20.32 |
|
|
|
| 10 |
A' |
1140 |
1105 |
10.60 |
|
|
|
| 11 |
A' |
1047 |
1015 |
36.08 |
|
|
|
| 12 |
A' |
898 |
871 |
136.64 |
|
|
|
| 13 |
A' |
857 |
831 |
52.83 |
|
|
|
| 14 |
A' |
391 |
379 |
7.38 |
|
|
|
| 15 |
A" |
3525 |
3417 |
3.46 |
|
|
|
| 16 |
A" |
3075 |
2981 |
99.96 |
|
|
|
| 17 |
A" |
3045 |
2952 |
1.16 |
|
|
|
| 18 |
A" |
1505 |
1459 |
7.96 |
|
|
|
| 19 |
A" |
1391 |
1349 |
0.01 |
|
|
|
| 20 |
A" |
1266 |
1227 |
0.24 |
|
|
|
| 21 |
A" |
1002 |
971 |
1.02 |
|
|
|
| 22 |
A" |
770 |
747 |
0.48 |
|
|
|
| 23 |
A" |
287 |
278 |
37.78 |
|
|
|
| 24 |
A" |
244 |
237 |
18.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20233.4 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 19614.3 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 B3LYP/CEP-121G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.334 |
-0.048 |
0.000 |
| C2 |
0.000 |
0.594 |
0.000 |
| C3 |
1.210 |
-0.368 |
0.000 |
| H4 |
2.162 |
0.184 |
0.000 |
| H5 |
1.198 |
-1.016 |
0.888 |
| H6 |
1.198 |
-1.016 |
-0.888 |
| H7 |
0.052 |
1.252 |
-0.879 |
| H8 |
0.052 |
1.252 |
0.879 |
| H9 |
-1.417 |
-0.658 |
0.816 |
| H10 |
-1.417 |
-0.658 |
-0.816 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4804 | 2.5645 | 3.5036 | 2.8529 | 2.8529 | 2.0935 | 2.0935 | 1.0217 | 1.0217 |
C2 | 1.4804 | | 1.5459 | 2.2005 | 2.1948 | 2.1948 | 1.0992 | 1.0992 | 2.0590 | 2.0590 | C3 | 2.5645 | 1.5459 | | 1.0998 | 1.0996 | 1.0996 | 2.1770 | 2.1770 | 2.7666 | 2.7666 | H4 | 3.5036 | 2.2005 | 1.0998 | | 1.7768 | 1.7768 | 2.5233 | 2.5233 | 3.7661 | 3.7661 | H5 | 2.8529 | 2.1948 | 1.0996 | 1.7768 | | 1.7759 | 3.0955 | 2.5419 | 2.6411 | 3.1422 | H6 | 2.8529 | 2.1948 | 1.0996 | 1.7768 | 1.7759 | | 2.5419 | 3.0955 | 3.1422 | 2.6411 | H7 | 2.0935 | 1.0992 | 2.1770 | 2.5233 | 3.0955 | 2.5419 | | 1.7573 | 2.9454 | 2.4099 | H8 | 2.0935 | 1.0992 | 2.1770 | 2.5233 | 2.5419 | 3.0955 | 1.7573 | | 2.4099 | 2.9454 | H9 | 1.0217 | 2.0590 | 2.7666 | 3.7661 | 2.6411 | 3.1422 | 2.9454 | 2.4099 | | 1.6319 | H10 | 1.0217 | 2.0590 | 2.7666 | 3.7661 | 3.1422 | 2.6411 | 2.4099 | 2.9454 | 1.6319 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.839 |
|
N1 |
C2 |
H7 |
107.578 |
| N1 |
C2 |
H8 |
107.578 |
|
C2 |
N1 |
H9 |
109.384 |
| C2 |
N1 |
H10 |
109.384 |
|
C2 |
C3 |
H4 |
111.436 |
| C2 |
C3 |
H5 |
110.995 |
|
C2 |
C3 |
H6 |
110.995 |
| C3 |
C2 |
H7 |
109.621 |
|
C3 |
C2 |
H8 |
109.621 |
| H4 |
C3 |
H5 |
107.772 |
|
H4 |
C3 |
H6 |
107.772 |
| H5 |
C3 |
H6 |
107.705 |
|
H7 |
C2 |
H8 |
106.147 |
| H9 |
N1 |
H10 |
105.994 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.624 |
|
|
|
| 2 |
C |
-0.215 |
|
|
|
| 3 |
C |
-0.509 |
|
|
|
| 4 |
H |
0.157 |
|
|
|
| 5 |
H |
0.146 |
|
|
|
| 6 |
H |
0.146 |
|
|
|
| 7 |
H |
0.158 |
|
|
|
| 8 |
H |
0.158 |
|
|
|
| 9 |
H |
0.291 |
|
|
|
| 10 |
H |
0.291 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.973 |
-1.046 |
0.000 |
1.428 |
| 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 |
5.544 |
-0.033 |
-0.038 |
| y |
-0.033 |
4.971 |
-0.085 |
| z |
-0.038 |
-0.085 |
4.580 |
<r2> (average value of r
2) Å
2
| <r2> |
52.235 |
| (<r2>)1/2 |
7.227 |
Jump to
S1C1
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -25.421092 |
| 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/CEP-121G*
Geometric Data calculated at B3LYP/CEP-121G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability