Jump to
S1C2
Energy calculated at HSEh1PBE/3-21G
| | hartrees |
| Energy at 0K | -134.273001 |
| Energy at 298.15K | -134.281152 |
| HF Energy | -134.273001 |
| Nuclear repulsion energy | 82.300378 |
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/3-21G
| 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' |
3441 |
3315 |
1.65 |
|
|
|
| 2 |
A' |
3134 |
3019 |
36.93 |
|
|
|
| 3 |
A' |
3074 |
2961 |
29.69 |
|
|
|
| 4 |
A' |
3054 |
2942 |
18.31 |
|
|
|
| 5 |
A' |
1730 |
1666 |
20.42 |
|
|
|
| 6 |
A' |
1562 |
1505 |
4.67 |
|
|
|
| 7 |
A' |
1543 |
1486 |
1.75 |
|
|
|
| 8 |
A' |
1452 |
1398 |
8.58 |
|
|
|
| 9 |
A' |
1402 |
1350 |
5.67 |
|
|
|
| 10 |
A' |
1168 |
1126 |
13.23 |
|
|
|
| 11 |
A' |
1056 |
1017 |
8.37 |
|
|
|
| 12 |
A' |
902 |
869 |
17.37 |
|
|
|
| 13 |
A' |
718 |
691 |
263.55 |
|
|
|
| 14 |
A' |
396 |
382 |
8.65 |
|
|
|
| 15 |
A" |
3542 |
3412 |
0.35 |
|
|
|
| 16 |
A" |
3140 |
3024 |
50.55 |
|
|
|
| 17 |
A" |
3108 |
2994 |
1.15 |
|
|
|
| 18 |
A" |
1562 |
1505 |
10.50 |
|
|
|
| 19 |
A" |
1414 |
1362 |
0.12 |
|
|
|
| 20 |
A" |
1304 |
1256 |
0.03 |
|
|
|
| 21 |
A" |
1029 |
991 |
1.77 |
|
|
|
| 22 |
A" |
794 |
764 |
3.16 |
|
|
|
| 23 |
A" |
314 |
302 |
54.99 |
|
|
|
| 24 |
A" |
261 |
251 |
10.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20548.3 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 19794.2 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/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.305 |
-0.103 |
0.000 |
| C2 |
0.000 |
0.583 |
0.000 |
| C3 |
1.223 |
-0.352 |
0.000 |
| H4 |
2.161 |
0.216 |
0.000 |
| H5 |
1.210 |
-0.995 |
0.889 |
| H6 |
1.210 |
-0.995 |
-0.889 |
| H7 |
0.035 |
1.235 |
-0.880 |
| H8 |
0.035 |
1.235 |
0.880 |
| H9 |
-1.428 |
-0.680 |
0.835 |
| H10 |
-1.428 |
-0.680 |
-0.835 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4735 | 2.5395 | 3.4801 | 2.8123 | 2.8123 | 2.0877 | 2.0877 | 1.0225 | 1.0225 |
C2 | 1.4735 | | 1.5389 | 2.1918 | 2.1778 | 2.1778 | 1.0963 | 1.0963 | 2.0809 | 2.0809 | C3 | 2.5395 | 1.5389 | | 1.0967 | 1.0970 | 1.0970 | 2.1686 | 2.1686 | 2.7984 | 2.7984 | H4 | 3.4801 | 2.1918 | 1.0967 | | 1.7778 | 1.7778 | 2.5164 | 2.5164 | 3.7922 | 3.7922 | H5 | 2.8123 | 2.1778 | 1.0970 | 1.7778 | | 1.7770 | 3.0793 | 2.5206 | 2.6574 | 3.1668 | H6 | 2.8123 | 2.1778 | 1.0970 | 1.7778 | 1.7770 | | 2.5206 | 3.0793 | 3.1668 | 2.6574 | H7 | 2.0877 | 1.0963 | 2.1686 | 2.5164 | 3.0793 | 2.5206 | | 1.7608 | 2.9579 | 2.4103 | H8 | 2.0877 | 1.0963 | 2.1686 | 2.5164 | 2.5206 | 3.0793 | 1.7608 | | 2.4103 | 2.9579 | H9 | 1.0225 | 2.0809 | 2.7984 | 3.7922 | 2.6574 | 3.1668 | 2.9579 | 2.4103 | | 1.6696 | H10 | 1.0225 | 2.0809 | 2.7984 | 3.7922 | 3.1668 | 2.6574 | 2.4103 | 2.9579 | 1.6696 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
114.899 |
|
N1 |
C2 |
H7 |
107.760 |
| N1 |
C2 |
H8 |
107.760 |
|
C2 |
N1 |
H9 |
111.686 |
| C2 |
N1 |
H10 |
111.686 |
|
C2 |
C3 |
H4 |
111.432 |
| C2 |
C3 |
H5 |
110.298 |
|
C2 |
C3 |
H6 |
110.298 |
| C3 |
C2 |
H7 |
109.623 |
|
C3 |
C2 |
H8 |
109.623 |
| H4 |
C3 |
H5 |
108.268 |
|
H4 |
C3 |
H6 |
108.268 |
| H5 |
C3 |
H6 |
108.180 |
|
H7 |
C2 |
H8 |
106.855 |
| H9 |
N1 |
H10 |
109.468 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.686 |
|
|
|
| 2 |
C |
-0.291 |
|
|
|
| 3 |
C |
-0.640 |
|
|
|
| 4 |
H |
0.206 |
|
|
|
| 5 |
H |
0.204 |
|
|
|
| 6 |
H |
0.204 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.225 |
|
|
|
| 9 |
H |
0.276 |
|
|
|
| 10 |
H |
0.276 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.911 |
-1.103 |
0.000 |
1.431 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.616 |
2.837 |
0.000 |
| y |
2.837 |
-19.854 |
0.000 |
| z |
0.000 |
0.000 |
-18.791 |
|
| Traceless |
| | x | y | z |
| x |
-4.293 |
2.837 |
0.000 |
| y |
2.837 |
1.350 |
0.000 |
| z |
0.000 |
0.000 |
2.944 |
|
| Polar |
| 3z2-r2 | 5.888 |
| x2-y2 | -3.762 |
| xy | 2.837 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.293 |
0.345 |
0.000 |
| y |
0.345 |
3.826 |
0.000 |
| z |
0.000 |
0.000 |
4.035 |
<r2> (average value of r
2) Å
2
| <r2> |
58.901 |
| (<r2>)1/2 |
7.675 |
Jump to
S1C1
Energy calculated at HSEh1PBE/3-21G
| | hartrees |
| Energy at 0K | -134.271848 |
| 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/3-21G
Geometric Data calculated at HSEh1PBE/3-21G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability