Jump to
S1C2
Energy calculated at B97D3/6-31G*
| | hartrees |
| Energy at 0K | -491.575961 |
| Energy at 298.15K | -491.576702 |
| HF Energy | -491.575961 |
| Nuclear repulsion energy | 79.155327 |
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 B97D3/6-31G*
| 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' |
3590 |
3520 |
145.46 |
|
|
|
| 2 |
A' |
2017 |
1978 |
543.81 |
|
|
|
| 3 |
A' |
867 |
850 |
1.85 |
|
|
|
| 4 |
A' |
718 |
704 |
349.03 |
|
|
|
| 5 |
A' |
443 |
434 |
39.73 |
|
|
|
| 6 |
A" |
466 |
457 |
2.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4050.3 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 3970.9 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 B97D3/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.183 |
1.702 |
0.000 |
| C2 |
0.000 |
0.497 |
0.000 |
| S3 |
0.049 |
-1.084 |
0.000 |
| H4 |
0.506 |
2.445 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2188 | 2.7960 | 1.0131 |
C2 | 1.2188 | | 1.5822 | 2.0119 | S3 | 2.7960 | 1.5822 | | 3.5582 | H4 | 1.0131 | 2.0119 | 3.5582 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
173.110 |
|
C2 |
N1 |
H4 |
128.457 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.559 |
|
|
|
| 2 |
C |
0.253 |
|
|
|
| 3 |
S |
-0.058 |
|
|
|
| 4 |
H |
0.365 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.223 |
1.718 |
0.000 |
2.108 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.976 |
3.174 |
0.000 |
| y |
3.174 |
-19.351 |
0.000 |
| z |
0.000 |
0.000 |
-24.791 |
|
| Traceless |
| | x | y | z |
| x |
-1.904 |
3.174 |
0.000 |
| y |
3.174 |
5.032 |
0.000 |
| z |
0.000 |
0.000 |
-3.128 |
|
| Polar |
| 3z2-r2 | -6.256 |
| x2-y2 | -4.625 |
| xy | 3.174 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.538 |
-0.258 |
0.000 |
| y |
-0.258 |
8.821 |
0.000 |
| z |
0.000 |
0.000 |
2.315 |
<r2> (average value of r
2) Å
2
| <r2> |
61.259 |
| (<r2>)1/2 |
7.827 |
Jump to
S1C1
Energy calculated at B97D3/6-31G*
| | hartrees |
| Energy at 0K | -491.569694 |
| Energy at 298.15K | |
| HF Energy | -491.569694 |
| Nuclear repulsion energy | 79.251775 |
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 B97D3/6-31G*
| 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 |
3874 |
3798 |
619.91 |
|
|
|
| 2 |
Σ |
2145 |
2103 |
581.94 |
|
|
|
| 3 |
Σ |
849 |
832 |
21.22 |
|
|
|
| 4 |
Π |
462 |
453 |
6.09 |
|
|
|
| 4 |
Π |
462 |
453 |
6.09 |
|
|
|
| 5 |
Π |
562i |
551i |
173.09 |
|
|
|
| 5 |
Π |
562i |
551i |
173.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3333.4 cm
-1
Scaled (by 0.9804) Zero Point Vibrational Energy (zpe) 3268.1 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 B97D3/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.690 |
| C2 |
0.000 |
0.000 |
-0.499 |
| S3 |
0.000 |
0.000 |
1.094 |
| H4 |
0.000 |
0.000 |
-2.685 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1914 | 2.7842 | 0.9951 |
C2 | 1.1914 | | 1.5928 | 2.1864 | S3 | 2.7842 | 1.5928 | | 3.7793 | H4 | 0.9951 | 2.1864 | 3.7793 | |
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 B97D3/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.552 |
|
|
|
| 2 |
C |
0.291 |
|
|
|
| 3 |
S |
-0.105 |
|
|
|
| 4 |
H |
0.367 |
|
|
|
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 |
-3.163 |
3.163 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.713 |
0.000 |
0.000 |
| y |
0.000 |
-24.713 |
0.000 |
| z |
0.000 |
0.000 |
-15.514 |
|
| Traceless |
| | x | y | z |
| x |
-4.599 |
0.000 |
0.000 |
| y |
0.000 |
-4.599 |
0.000 |
| z |
0.000 |
0.000 |
9.198 |
|
| Polar |
| 3z2-r2 | 18.397 |
| 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 |
2.307 |
0.000 |
0.000 |
| y |
0.000 |
2.307 |
0.000 |
| z |
0.000 |
0.000 |
8.562 |
<r2> (average value of r
2) Å
2
| <r2> |
61.370 |
| (<r2>)1/2 |
7.834 |