Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -135.153422 |
| Energy at 298.15K | -135.161392 |
| Nuclear repulsion energy | 81.915058 |
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/LANL2DZ
| 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' |
3536 |
3398 |
0.79 |
|
|
|
| 2 |
A' |
3116 |
2995 |
73.38 |
|
|
|
| 3 |
A' |
3056 |
2937 |
42.74 |
|
|
|
| 4 |
A' |
3024 |
2907 |
32.74 |
|
|
|
| 5 |
A' |
1686 |
1621 |
33.88 |
|
|
|
| 6 |
A' |
1524 |
1465 |
8.97 |
|
|
|
| 7 |
A' |
1508 |
1450 |
0.68 |
|
|
|
| 8 |
A' |
1428 |
1372 |
11.72 |
|
|
|
| 9 |
A' |
1389 |
1335 |
8.91 |
|
|
|
| 10 |
A' |
1153 |
1108 |
25.80 |
|
|
|
| 11 |
A' |
1068 |
1027 |
23.00 |
|
|
|
| 12 |
A' |
891 |
856 |
4.75 |
|
|
|
| 13 |
A' |
623 |
599 |
306.24 |
|
|
|
| 14 |
A' |
392 |
377 |
19.82 |
|
|
|
| 15 |
A" |
3659 |
3517 |
0.26 |
|
|
|
| 16 |
A" |
3129 |
3007 |
98.82 |
|
|
|
| 17 |
A" |
3097 |
2977 |
1.49 |
|
|
|
| 18 |
A" |
1514 |
1455 |
10.76 |
|
|
|
| 19 |
A" |
1370 |
1317 |
0.40 |
|
|
|
| 20 |
A" |
1267 |
1218 |
0.57 |
|
|
|
| 21 |
A" |
994 |
955 |
0.41 |
|
|
|
| 22 |
A" |
785 |
754 |
5.41 |
|
|
|
| 23 |
A" |
262 |
251 |
23.55 |
|
|
|
| 24 |
A" |
241 |
232 |
38.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20355.1 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 19565.3 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/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.306 |
-0.107 |
0.000 |
| C2 |
0.000 |
0.577 |
0.000 |
| C3 |
1.238 |
-0.354 |
0.000 |
| H4 |
2.173 |
0.226 |
0.000 |
| H5 |
1.239 |
-1.001 |
0.889 |
| H6 |
1.239 |
-1.001 |
-0.889 |
| H7 |
0.036 |
1.235 |
-0.879 |
| H8 |
0.036 |
1.235 |
0.879 |
| H9 |
-1.506 |
-0.640 |
0.843 |
| H10 |
-1.506 |
-0.640 |
-0.843 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4747 | 2.5565 | 3.4946 | 2.8401 | 2.8401 | 2.0920 | 2.0920 | 1.0172 | 1.0172 |
C2 | 1.4747 | | 1.5498 | 2.2009 | 2.1945 | 2.1945 | 1.0982 | 1.0982 | 2.1121 | 2.1121 | C3 | 2.5565 | 1.5498 | | 1.0995 | 1.0990 | 1.0990 | 2.1779 | 2.1779 | 2.8853 | 2.8853 | H4 | 3.4946 | 2.2009 | 1.0995 | | 1.7790 | 1.7790 | 2.5208 | 2.5208 | 3.8720 | 3.8720 | H5 | 2.8401 | 2.1945 | 1.0990 | 1.7790 | | 1.7777 | 3.0934 | 2.5386 | 2.7692 | 3.2660 | H6 | 2.8401 | 2.1945 | 1.0990 | 1.7790 | 1.7777 | | 2.5386 | 3.0934 | 3.2660 | 2.7692 | H7 | 2.0920 | 1.0982 | 2.1779 | 2.5208 | 3.0934 | 2.5386 | | 1.7578 | 2.9765 | 2.4280 | H8 | 2.0920 | 1.0982 | 2.1779 | 2.5208 | 2.5386 | 3.0934 | 1.7578 | | 2.4280 | 2.9765 | H9 | 1.0172 | 2.1121 | 2.8853 | 3.8720 | 2.7692 | 3.2660 | 2.9765 | 2.4280 | | 1.6865 | H10 | 1.0172 | 2.1121 | 2.8853 | 3.8720 | 3.2660 | 2.7692 | 2.4280 | 2.9765 | 1.6865 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.377 |
|
N1 |
C2 |
H7 |
107.898 |
| N1 |
C2 |
H8 |
107.898 |
|
C2 |
N1 |
H9 |
114.659 |
| C2 |
N1 |
H10 |
114.659 |
|
C2 |
C3 |
H4 |
111.209 |
| C2 |
C3 |
H5 |
110.738 |
|
C2 |
C3 |
H6 |
110.738 |
| C3 |
C2 |
H7 |
109.481 |
|
C3 |
C2 |
H8 |
109.481 |
| H4 |
C3 |
H5 |
108.037 |
|
H4 |
C3 |
H6 |
108.037 |
| H5 |
C3 |
H6 |
107.958 |
|
H7 |
C2 |
H8 |
106.314 |
| H9 |
N1 |
H10 |
111.992 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.570 |
|
|
|
| 2 |
C |
-0.310 |
|
|
|
| 3 |
C |
-0.602 |
|
|
|
| 4 |
H |
0.192 |
|
|
|
| 5 |
H |
0.191 |
|
|
|
| 6 |
H |
0.191 |
|
|
|
| 7 |
H |
0.194 |
|
|
|
| 8 |
H |
0.194 |
|
|
|
| 9 |
H |
0.260 |
|
|
|
| 10 |
H |
0.260 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.883 |
-1.071 |
0.000 |
1.388 |
| 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 |
4.793 |
-0.066 |
-0.152 |
| y |
-0.066 |
4.234 |
-0.170 |
| z |
-0.152 |
-0.170 |
3.732 |
<r2> (average value of r
2) Å
2
| <r2> |
59.712 |
| (<r2>)1/2 |
7.727 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -135.153129 |
| 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/LANL2DZ
Geometric Data calculated at B3LYP/LANL2DZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability