Jump to
S1C2
Energy calculated at HSEh1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -135.068341 |
| Energy at 298.15K | -135.076479 |
| HF Energy | -135.068341 |
| Nuclear repulsion energy | 83.067958 |
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 HSEh1PBE/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' |
3518 |
3381 |
1.02 |
|
|
|
| 2 |
A' |
3106 |
2985 |
43.35 |
|
|
|
| 3 |
A' |
3045 |
2926 |
35.82 |
|
|
|
| 4 |
A' |
3031 |
2913 |
21.48 |
|
|
|
| 5 |
A' |
1661 |
1596 |
21.69 |
|
|
|
| 6 |
A' |
1500 |
1441 |
2.97 |
|
|
|
| 7 |
A' |
1481 |
1423 |
0.15 |
|
|
|
| 8 |
A' |
1403 |
1349 |
11.30 |
|
|
|
| 9 |
A' |
1377 |
1324 |
9.91 |
|
|
|
| 10 |
A' |
1157 |
1112 |
9.27 |
|
|
|
| 11 |
A' |
1084 |
1042 |
27.48 |
|
|
|
| 12 |
A' |
900 |
865 |
16.52 |
|
|
|
| 13 |
A' |
858 |
825 |
161.41 |
|
|
|
| 14 |
A' |
401 |
385 |
6.53 |
|
|
|
| 15 |
A" |
3599 |
3459 |
0.20 |
|
|
|
| 16 |
A" |
3109 |
2988 |
54.48 |
|
|
|
| 17 |
A" |
3073 |
2954 |
5.51 |
|
|
|
| 18 |
A" |
1487 |
1429 |
8.36 |
|
|
|
| 19 |
A" |
1390 |
1336 |
0.04 |
|
|
|
| 20 |
A" |
1270 |
1221 |
0.04 |
|
|
|
| 21 |
A" |
1005 |
966 |
0.92 |
|
|
|
| 22 |
A" |
777 |
747 |
1.49 |
|
|
|
| 23 |
A" |
282 |
271 |
24.50 |
|
|
|
| 24 |
A" |
246 |
236 |
19.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20379.4 cm
-1
Scaled (by 0.9611) Zero Point Vibrational Energy (zpe) 19586.7 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 HSEh1PBE/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.300 |
-0.085 |
0.000 |
| C2 |
0.000 |
0.571 |
0.000 |
| C3 |
1.206 |
-0.354 |
0.000 |
| H4 |
2.145 |
0.206 |
0.000 |
| H5 |
1.204 |
-1.000 |
0.882 |
| H6 |
1.204 |
-1.000 |
-0.882 |
| H7 |
0.040 |
1.229 |
-0.872 |
| H8 |
0.040 |
1.229 |
0.872 |
| H9 |
-1.386 |
-0.686 |
0.810 |
| H10 |
-1.386 |
-0.686 |
-0.810 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4561 | 2.5210 | 3.4573 | 2.8083 | 2.8083 | 2.0696 | 2.0696 | 1.0123 | 1.0123 |
C2 | 1.4561 | | 1.5206 | 2.1758 | 2.1670 | 2.1670 | 1.0934 | 1.0934 | 2.0386 | 2.0386 | C3 | 2.5210 | 1.5206 | | 1.0931 | 1.0931 | 1.0931 | 2.1517 | 2.1517 | 2.7359 | 2.7359 | H4 | 3.4573 | 2.1758 | 1.0931 | | 1.7658 | 1.7658 | 2.4978 | 2.4978 | 3.7305 | 3.7305 | H5 | 2.8083 | 2.1670 | 1.0931 | 1.7658 | | 1.7647 | 3.0663 | 2.5147 | 2.6096 | 3.1095 | H6 | 2.8083 | 2.1670 | 1.0931 | 1.7658 | 1.7647 | | 2.5147 | 3.0663 | 3.1095 | 2.6096 | H7 | 2.0696 | 1.0934 | 2.1517 | 2.4978 | 3.0663 | 2.5147 | | 1.7444 | 2.9206 | 2.3883 | H8 | 2.0696 | 1.0934 | 2.1517 | 2.4978 | 2.5147 | 3.0663 | 1.7444 | | 2.3883 | 2.9206 | H9 | 1.0123 | 2.0386 | 2.7359 | 3.7305 | 2.6096 | 3.1095 | 2.9206 | 2.3883 | | 1.6199 | H10 | 1.0123 | 2.0386 | 2.7359 | 3.7305 | 3.1095 | 2.6096 | 2.3883 | 2.9206 | 1.6199 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.740 |
|
N1 |
C2 |
H7 |
107.683 |
| N1 |
C2 |
H8 |
107.683 |
|
C2 |
N1 |
H9 |
110.054 |
| C2 |
N1 |
H10 |
110.054 |
|
C2 |
C3 |
H4 |
111.660 |
| C2 |
C3 |
H5 |
110.948 |
|
C2 |
C3 |
H6 |
110.948 |
| C3 |
C2 |
H7 |
109.719 |
|
C3 |
C2 |
H8 |
109.719 |
| H4 |
C3 |
H5 |
107.736 |
|
H4 |
C3 |
H6 |
107.736 |
| H5 |
C3 |
H6 |
107.639 |
|
H7 |
C2 |
H8 |
105.814 |
| H9 |
N1 |
H10 |
106.290 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.306 |
|
|
|
| 2 |
C |
-0.091 |
|
|
|
| 3 |
C |
-0.287 |
|
|
|
| 4 |
H |
0.086 |
|
|
|
| 5 |
H |
0.086 |
|
|
|
| 6 |
H |
0.086 |
|
|
|
| 7 |
H |
0.091 |
|
|
|
| 8 |
H |
0.091 |
|
|
|
| 9 |
H |
0.122 |
|
|
|
| 10 |
H |
0.122 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.846 |
-0.896 |
0.000 |
1.232 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.817 |
2.502 |
0.000 |
| y |
2.502 |
-20.401 |
0.000 |
| z |
0.000 |
0.000 |
-19.131 |
|
| Traceless |
| | x | y | z |
| x |
-4.051 |
2.502 |
0.000 |
| y |
2.502 |
1.073 |
0.000 |
| z |
0.000 |
0.000 |
2.978 |
|
| Polar |
| 3z2-r2 | 5.956 |
| x2-y2 | -3.416 |
| xy | 2.502 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.654 |
0.085 |
0.000 |
| y |
0.085 |
5.074 |
0.000 |
| z |
0.000 |
0.000 |
4.871 |
<r2> (average value of r
2) Å
2
| <r2> |
58.253 |
| (<r2>)1/2 |
7.632 |
Jump to
S1C1
Energy calculated at HSEh1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -135.068074 |
| 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 HSEh1PBE/cc-pVTZ
Geometric Data calculated at HSEh1PBE/cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability