Jump to
S1C2
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.440052 |
| Energy at 298.15K | -491.440823 |
| HF Energy | -491.440052 |
| Nuclear repulsion energy | 80.065764 |
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 PBE1PBE/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' |
3716 |
3571 |
256.37 |
|
|
|
| 2 |
A' |
2082 |
2001 |
731.00 |
|
|
|
| 3 |
A' |
896 |
861 |
3.35 |
|
|
|
| 4 |
A' |
638 |
613 |
321.23 |
|
|
|
| 5 |
A' |
463 |
445 |
98.43 |
|
|
|
| 6 |
A" |
499 |
479 |
1.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4146.3 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 3984.6 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 PBE1PBE/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.139 |
1.683 |
0.000 |
| C2 |
0.000 |
0.494 |
0.000 |
| S3 |
0.028 |
-1.074 |
0.000 |
| H4 |
0.526 |
2.436 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1976 | 2.7625 | 1.0034 |
C2 | 1.1976 | | 1.5682 | 2.0116 | S3 | 2.7625 | 1.5682 | | 3.5448 | H4 | 1.0034 | 2.0116 | 3.5448 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.370 |
|
C2 |
N1 |
H4 |
131.915 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.152 |
|
|
|
| 2 |
C |
0.082 |
|
|
|
| 3 |
S |
-0.138 |
|
|
|
| 4 |
H |
0.208 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.122 |
1.724 |
0.000 |
2.057 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.260 |
2.999 |
0.000 |
| y |
2.999 |
-19.178 |
0.000 |
| z |
0.000 |
0.000 |
-25.120 |
|
| Traceless |
| | x | y | z |
| x |
-2.111 |
2.999 |
0.000 |
| y |
2.999 |
5.512 |
0.000 |
| z |
0.000 |
0.000 |
-3.401 |
|
| Polar |
| 3z2-r2 | -6.802 |
| x2-y2 | -5.082 |
| xy | 2.999 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.227 |
-0.153 |
0.000 |
| y |
-0.153 |
9.131 |
0.000 |
| z |
0.000 |
0.000 |
3.100 |
<r2> (average value of r
2) Å
2
| <r2> |
60.388 |
| (<r2>)1/2 |
7.771 |
Jump to
S1C1
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.436473 |
| Energy at 298.15K | |
| HF Energy | -491.436473 |
| Nuclear repulsion energy | 80.095219 |
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 PBE1PBE/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 |
Σ |
3925 |
3772 |
717.12 |
|
|
|
| 2 |
Σ |
2192 |
2107 |
751.40 |
|
|
|
| 3 |
Σ |
876 |
842 |
29.52 |
|
|
|
| 4 |
Π |
495 |
476 |
6.25 |
|
|
|
| 4 |
Π |
495 |
476 |
6.25 |
|
|
|
| 5 |
Π |
450i |
433i |
147.47 |
|
|
|
| 5 |
Π |
450i |
433i |
147.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3540.9 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 3402.8 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 PBE1PBE/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.670 |
| C2 |
0.000 |
0.000 |
-0.496 |
| S3 |
0.000 |
0.000 |
1.083 |
| H4 |
0.000 |
0.000 |
-2.660 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1741 | 2.7534 | 0.9894 |
C2 | 1.1741 | | 1.5793 | 2.1635 | S3 | 2.7534 | 1.5793 | | 3.7428 | H4 | 0.9894 | 2.1635 | 3.7428 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
180.000 |
|
C2 |
N1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.138 |
|
|
|
| 2 |
C |
0.096 |
|
|
|
| 3 |
S |
-0.194 |
|
|
|
| 4 |
H |
0.236 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-3.081 |
3.081 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.088 |
0.000 |
0.000 |
| y |
0.000 |
-25.088 |
0.000 |
| z |
0.000 |
0.000 |
-15.728 |
|
| Traceless |
| | x | y | z |
| x |
-4.680 |
0.000 |
0.000 |
| y |
0.000 |
-4.680 |
0.000 |
| z |
0.000 |
0.000 |
9.360 |
|
| Polar |
| 3z2-r2 | 18.720 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.080 |
0.000 |
0.000 |
| y |
0.000 |
3.080 |
0.000 |
| z |
0.000 |
0.000 |
8.936 |
<r2> (average value of r
2) Å
2
| <r2> |
60.571 |
| (<r2>)1/2 |
7.783 |