Jump to
S1C2
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -135.231468 |
| Energy at 298.15K | -135.239603 |
| Nuclear repulsion energy | 82.748785 |
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/cc-pVTZ
| 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' |
3476 |
3360 |
1.49 |
|
|
|
| 2 |
A' |
3075 |
2972 |
50.64 |
|
|
|
| 3 |
A' |
3024 |
2923 |
35.02 |
|
|
|
| 4 |
A' |
3012 |
2912 |
23.70 |
|
|
|
| 5 |
A' |
1662 |
1606 |
20.16 |
|
|
|
| 6 |
A' |
1507 |
1457 |
2.17 |
|
|
|
| 7 |
A' |
1488 |
1438 |
0.19 |
|
|
|
| 8 |
A' |
1409 |
1362 |
6.44 |
|
|
|
| 9 |
A' |
1383 |
1337 |
12.92 |
|
|
|
| 10 |
A' |
1146 |
1108 |
9.47 |
|
|
|
| 11 |
A' |
1055 |
1020 |
26.76 |
|
|
|
| 12 |
A' |
894 |
864 |
50.21 |
|
|
|
| 13 |
A' |
847 |
819 |
130.14 |
|
|
|
| 14 |
A' |
401 |
388 |
6.19 |
|
|
|
| 15 |
A" |
3552 |
3433 |
0.00 |
|
|
|
| 16 |
A" |
3081 |
2978 |
62.39 |
|
|
|
| 17 |
A" |
3047 |
2945 |
5.30 |
|
|
|
| 18 |
A" |
1494 |
1444 |
7.24 |
|
|
|
| 19 |
A" |
1390 |
1343 |
0.04 |
|
|
|
| 20 |
A" |
1273 |
1230 |
0.08 |
|
|
|
| 21 |
A" |
1008 |
974 |
0.75 |
|
|
|
| 22 |
A" |
781 |
755 |
1.06 |
|
|
|
| 23 |
A" |
283 |
273 |
27.23 |
|
|
|
| 24 |
A" |
247 |
239 |
15.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20267.2 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 19590.3 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.308 |
-0.086 |
0.000 |
| C2 |
0.000 |
0.573 |
0.000 |
| C3 |
1.216 |
-0.355 |
0.000 |
| H4 |
2.150 |
0.211 |
0.000 |
| H5 |
1.215 |
-0.999 |
0.882 |
| H6 |
1.215 |
-0.999 |
-0.882 |
| H7 |
0.039 |
1.229 |
-0.873 |
| H8 |
0.039 |
1.229 |
0.873 |
| H9 |
-1.399 |
-0.687 |
0.812 |
| H10 |
-1.399 |
-0.687 |
-0.812 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4646 | 2.5382 | 3.4712 | 2.8248 | 2.8248 | 2.0751 | 2.0751 | 1.0138 | 1.0138 |
C2 | 1.4646 | | 1.5293 | 2.1805 | 2.1739 | 2.1739 | 1.0925 | 1.0925 | 2.0501 | 2.0501 | C3 | 2.5382 | 1.5293 | | 1.0927 | 1.0924 | 1.0924 | 2.1573 | 2.1573 | 2.7581 | 2.7581 | H4 | 3.4712 | 2.1805 | 1.0927 | | 1.7657 | 1.7657 | 2.5006 | 2.5006 | 3.7503 | 3.7503 | H5 | 2.8248 | 2.1739 | 1.0924 | 1.7657 | | 1.7647 | 3.0702 | 2.5191 | 2.6340 | 3.1309 | H6 | 2.8248 | 2.1739 | 1.0924 | 1.7657 | 1.7647 | | 2.5191 | 3.0702 | 3.1309 | 2.6340 | H7 | 2.0751 | 1.0925 | 2.1573 | 2.5006 | 3.0702 | 2.5191 | | 1.7453 | 2.9284 | 2.3965 | H8 | 2.0751 | 1.0925 | 2.1573 | 2.5006 | 2.5191 | 3.0702 | 1.7453 | | 2.3965 | 2.9284 | H9 | 1.0138 | 2.0501 | 2.7581 | 3.7503 | 2.6340 | 3.1309 | 2.9284 | 2.3965 | | 1.6231 | H10 | 1.0138 | 2.0501 | 2.7581 | 3.7503 | 3.1309 | 2.6340 | 2.3965 | 2.9284 | 1.6231 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.928 |
|
N1 |
C2 |
H7 |
107.597 |
| N1 |
C2 |
H8 |
107.597 |
|
C2 |
N1 |
H9 |
110.292 |
| C2 |
N1 |
H10 |
110.292 |
|
C2 |
C3 |
H4 |
111.440 |
| C2 |
C3 |
H5 |
110.929 |
|
C2 |
C3 |
H6 |
110.929 |
| C3 |
C2 |
H7 |
109.611 |
|
C3 |
C2 |
H8 |
109.611 |
| H4 |
C3 |
H5 |
107.817 |
|
H4 |
C3 |
H6 |
107.817 |
| H5 |
C3 |
H6 |
107.751 |
|
H7 |
C2 |
H8 |
106.025 |
| H9 |
N1 |
H10 |
106.348 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.320 |
|
|
-0.933 |
| 2 |
C |
-0.083 |
|
|
0.490 |
| 3 |
C |
-0.281 |
|
|
-0.370 |
| 4 |
H |
0.085 |
|
|
0.062 |
| 5 |
H |
0.083 |
|
|
0.078 |
| 6 |
H |
0.083 |
|
|
0.078 |
| 7 |
H |
0.092 |
|
|
-0.033 |
| 8 |
H |
0.092 |
|
|
-0.033 |
| 9 |
H |
0.125 |
|
|
0.330 |
| 10 |
H |
0.125 |
|
|
0.330 |
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.837 |
-0.878 |
0.000 |
1.213 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.806 |
-0.894 |
0.000 |
1.204 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.013 |
2.504 |
0.000 |
| y |
2.504 |
-20.614 |
0.000 |
| z |
0.000 |
0.000 |
-19.344 |
|
| Traceless |
| | x | y | z |
| x |
-4.034 |
2.504 |
0.000 |
| y |
2.504 |
1.064 |
0.000 |
| z |
0.000 |
0.000 |
2.970 |
|
| Polar |
| 3z2-r2 | 5.940 |
| x2-y2 | -3.399 |
| xy | 2.504 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.819 |
-0.006 |
0.006 |
| y |
-0.006 |
5.141 |
-0.063 |
| z |
0.006 |
-0.063 |
4.760 |
<r2> (average value of r
2) Å
2
| <r2> |
58.840 |
| (<r2>)1/2 |
7.671 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -135.231210 |
| 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/cc-pVTZ
Geometric Data calculated at B3LYP/cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability