Jump to
S1C2
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -135.009971 |
| Energy at 298.15K | -135.018080 |
| Nuclear repulsion energy | 82.280154 |
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 PBEPBE/6-311G*
| 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' |
3378 |
3343 |
7.30 |
|
|
|
| 2 |
A' |
3020 |
2989 |
56.87 |
|
|
|
| 3 |
A' |
2962 |
2931 |
39.72 |
|
|
|
| 4 |
A' |
2949 |
2918 |
31.11 |
|
|
|
| 5 |
A' |
1672 |
1654 |
27.45 |
|
|
|
| 6 |
A' |
1471 |
1456 |
4.76 |
|
|
|
| 7 |
A' |
1450 |
1435 |
0.15 |
|
|
|
| 8 |
A' |
1368 |
1354 |
10.66 |
|
|
|
| 9 |
A' |
1342 |
1328 |
12.86 |
|
|
|
| 10 |
A' |
1133 |
1121 |
8.76 |
|
|
|
| 11 |
A' |
1042 |
1031 |
27.12 |
|
|
|
| 12 |
A' |
883 |
873 |
112.87 |
|
|
|
| 13 |
A' |
848 |
839 |
89.81 |
|
|
|
| 14 |
A' |
389 |
385 |
7.11 |
|
|
|
| 15 |
A" |
3456 |
3420 |
3.04 |
|
|
|
| 16 |
A" |
3027 |
2995 |
69.79 |
|
|
|
| 17 |
A" |
2990 |
2959 |
7.53 |
|
|
|
| 18 |
A" |
1464 |
1449 |
11.21 |
|
|
|
| 19 |
A" |
1371 |
1357 |
0.01 |
|
|
|
| 20 |
A" |
1244 |
1231 |
0.09 |
|
|
|
| 21 |
A" |
990 |
980 |
0.98 |
|
|
|
| 22 |
A" |
760 |
752 |
1.32 |
|
|
|
| 23 |
A" |
303 |
300 |
41.06 |
|
|
|
| 24 |
A" |
251 |
249 |
11.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19880.1 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 19673.4 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 PBEPBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.317 |
-0.077 |
0.000 |
| C2 |
0.000 |
0.573 |
0.000 |
| C3 |
1.219 |
-0.361 |
0.000 |
| H4 |
2.168 |
0.202 |
0.000 |
| H5 |
1.218 |
-1.013 |
0.890 |
| H6 |
1.218 |
-1.013 |
-0.890 |
| H7 |
0.042 |
1.238 |
-0.880 |
| H8 |
0.042 |
1.238 |
0.880 |
| H9 |
-1.391 |
-0.692 |
0.817 |
| H10 |
-1.391 |
-0.692 |
-0.817 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4681 | 2.5511 | 3.4955 | 2.8442 | 2.8442 | 2.0855 | 2.0855 | 1.0249 | 1.0249 |
C2 | 1.4681 | | 1.5350 | 2.1991 | 2.1883 | 2.1883 | 1.1040 | 1.1040 | 2.0496 | 2.0496 | C3 | 2.5511 | 1.5350 | | 1.1035 | 1.1033 | 1.1033 | 2.1716 | 2.1716 | 2.7547 | 2.7547 | H4 | 3.4955 | 2.1991 | 1.1035 | | 1.7811 | 1.7811 | 2.5232 | 2.5232 | 3.7593 | 3.7593 | H5 | 2.8442 | 2.1883 | 1.1033 | 1.7811 | | 1.7794 | 3.0956 | 2.5401 | 2.6295 | 3.1338 | H6 | 2.8442 | 2.1883 | 1.1033 | 1.7811 | 1.7794 | | 2.5401 | 3.0956 | 3.1338 | 2.6295 | H7 | 2.0855 | 1.1040 | 2.1716 | 2.5232 | 3.0956 | 2.5401 | | 1.7593 | 2.9422 | 2.4047 | H8 | 2.0855 | 1.1040 | 2.1716 | 2.5232 | 2.5401 | 3.0956 | 1.7593 | | 2.4047 | 2.9422 | H9 | 1.0249 | 2.0496 | 2.7547 | 3.7593 | 2.6295 | 3.1338 | 2.9422 | 2.4047 | | 1.6336 | H10 | 1.0249 | 2.0496 | 2.7547 | 3.7593 | 3.1338 | 2.6295 | 2.4047 | 2.9422 | 1.6336 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.292 |
|
N1 |
C2 |
H7 |
107.507 |
| N1 |
C2 |
H8 |
107.507 |
|
C2 |
N1 |
H9 |
109.308 |
| C2 |
N1 |
H10 |
109.308 |
|
C2 |
C3 |
H4 |
111.870 |
| C2 |
C3 |
H5 |
111.022 |
|
C2 |
C3 |
H6 |
111.022 |
| C3 |
C2 |
H7 |
109.670 |
|
C3 |
C2 |
H8 |
109.670 |
| H4 |
C3 |
H5 |
107.620 |
|
H4 |
C3 |
H6 |
107.620 |
| H5 |
C3 |
H6 |
107.488 |
|
H7 |
C2 |
H8 |
105.648 |
| H9 |
N1 |
H10 |
105.674 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.697 |
|
|
|
| 2 |
C |
-0.317 |
|
|
|
| 3 |
C |
-0.635 |
|
|
|
| 4 |
H |
0.208 |
|
|
|
| 5 |
H |
0.201 |
|
|
|
| 6 |
H |
0.201 |
|
|
|
| 7 |
H |
0.216 |
|
|
|
| 8 |
H |
0.216 |
|
|
|
| 9 |
H |
0.304 |
|
|
|
| 10 |
H |
0.304 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.875 |
-1.018 |
0.000 |
1.343 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.358 |
2.796 |
0.000 |
| y |
2.796 |
-20.641 |
0.000 |
| z |
0.000 |
0.000 |
-19.335 |
|
| Traceless |
| | x | y | z |
| x |
-4.371 |
2.796 |
0.000 |
| y |
2.796 |
1.205 |
0.000 |
| z |
0.000 |
0.000 |
3.165 |
|
| Polar |
| 3z2-r2 | 6.330 |
| x2-y2 | -3.717 |
| xy | 2.796 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.469 |
0.134 |
0.000 |
| y |
0.134 |
4.841 |
0.000 |
| z |
0.000 |
0.000 |
4.740 |
<r2> (average value of r
2) Å
2
| <r2> |
59.350 |
| (<r2>)1/2 |
7.704 |
Jump to
S1C1
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -135.009241 |
| 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 PBEPBE/6-311G*
Geometric Data calculated at PBEPBE/6-311G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability