Jump to
S1C2
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -489.212761 |
| Energy at 298.15K | -489.213426 |
| HF Energy | -489.212761 |
| Nuclear repulsion energy | 79.244178 |
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 B97D3/3-21G*
| 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' |
3639 |
3639 |
308.27 |
|
|
|
| 2 |
A' |
2093 |
2093 |
440.22 |
|
|
|
| 3 |
A' |
855 |
855 |
7.10 |
|
|
|
| 4 |
A' |
513 |
513 |
110.81 |
|
|
|
| 5 |
A' |
453 |
453 |
274.12 |
|
|
|
| 6 |
A" |
504 |
504 |
0.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4027.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4027.6 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 B97D3/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.097 |
1.697 |
0.000 |
| C2 |
0.000 |
0.497 |
0.000 |
| S3 |
0.015 |
-1.088 |
0.000 |
| H4 |
0.435 |
2.554 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2048 | 2.7881 | 1.0088 |
C2 | 1.2048 | | 1.5851 | 2.1033 | S3 | 2.7881 | 1.5851 | | 3.6670 | H4 | 1.0088 | 2.1033 | 3.6670 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
175.927 |
|
C2 |
N1 |
H4 |
143.527 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.697 |
|
|
|
| 2 |
C |
0.288 |
|
|
|
| 3 |
S |
0.054 |
|
|
|
| 4 |
H |
0.355 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.099 |
2.576 |
0.000 |
2.801 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.365 |
2.866 |
0.000 |
| y |
2.866 |
-17.619 |
0.000 |
| z |
0.000 |
0.000 |
-24.900 |
|
| Traceless |
| | x | y | z |
| x |
-3.106 |
2.866 |
0.000 |
| y |
2.866 |
7.013 |
0.000 |
| z |
0.000 |
0.000 |
-3.907 |
|
| Polar |
| 3z2-r2 | -7.815 |
| x2-y2 | -6.746 |
| xy | 2.866 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.053 |
-0.100 |
0.000 |
| y |
-0.100 |
8.278 |
0.000 |
| z |
0.000 |
0.000 |
1.936 |
<r2> (average value of r
2) Å
2
| <r2> |
61.313 |
| (<r2>)1/2 |
7.830 |
Jump to
S1C1
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -489.211631 |
| Energy at 298.15K | |
| HF Energy | -489.211631 |
| Nuclear repulsion energy | 79.285995 |
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 B97D3/3-21G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3798 |
3798 |
637.21 |
|
|
|
| 2 |
Σ |
2158 |
2158 |
442.40 |
|
|
|
| 3 |
Σ |
845 |
845 |
20.05 |
|
|
|
| 4 |
Π |
509 |
509 |
0.42 |
|
|
|
| 4 |
Π |
509 |
509 |
0.42 |
|
|
|
| 5 |
Π |
311i |
311i |
224.52 |
|
|
|
| 5 |
Π |
311i |
311i |
224.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3599.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3599.5 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 B97D3/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.689 |
| C2 |
0.000 |
0.000 |
-0.498 |
| S3 |
0.000 |
0.000 |
1.094 |
| H4 |
0.000 |
0.000 |
-2.685 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1912 | 2.7827 | 0.9962 |
C2 | 1.1912 | | 1.5916 | 2.1874 | S3 | 2.7827 | 1.5916 | | 3.7790 | H4 | 0.9962 | 2.1874 | 3.7790 | |
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 B97D3/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.751 |
|
|
|
| 2 |
C |
0.351 |
|
|
|
| 3 |
S |
0.027 |
|
|
|
| 4 |
H |
0.373 |
|
|
|
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 |
-3.383 |
3.383 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.860 |
0.000 |
0.000 |
| y |
0.000 |
-24.860 |
0.000 |
| z |
0.000 |
0.000 |
-15.400 |
|
| Traceless |
| | x | y | z |
| x |
-4.730 |
0.000 |
0.000 |
| y |
0.000 |
-4.730 |
0.000 |
| z |
0.000 |
0.000 |
9.460 |
|
| Polar |
| 3z2-r2 | 18.919 |
| 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 |
1.929 |
0.000 |
0.000 |
| y |
0.000 |
1.929 |
0.000 |
| z |
0.000 |
0.000 |
8.045 |
<r2> (average value of r
2) Å
2
| <r2> |
61.364 |
| (<r2>)1/2 |
7.834 |