Jump to
S1C2
Energy calculated at wB97X-D/CEP-31G*
| | hartrees |
| Energy at 0K | -26.282705 |
| Energy at 298.15K | -26.283394 |
| HF Energy | -26.282705 |
| 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 wB97X-D/CEP-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' |
3732 |
3732 |
246.31 |
|
|
|
| 2 |
A' |
2064 |
2064 |
786.52 |
|
|
|
| 3 |
A' |
877 |
877 |
3.70 |
|
|
|
| 4 |
A' |
602 |
602 |
342.89 |
|
|
|
| 5 |
A' |
436 |
436 |
126.32 |
|
|
|
| 6 |
A" |
478 |
478 |
1.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4093.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4093.8 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 wB97X-D/CEP-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.160 |
1.714 |
0.000 |
| C2 |
0.000 |
0.502 |
0.000 |
| S3 |
0.036 |
-1.091 |
0.000 |
| H4 |
0.538 |
2.450 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2216 | 2.8116 | 1.0139 |
C2 | 1.2216 | | 1.5941 | 2.0199 | S3 | 2.8116 | 1.5941 | | 3.5761 | H4 | 1.0139 | 2.0199 | 3.5761 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
173.789 |
|
C2 |
N1 |
H4 |
129.027 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.002 |
|
|
|
| 2 |
C |
-0.083 |
|
|
|
| 3 |
S |
-0.282 |
|
|
|
| 4 |
H |
0.366 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.360 |
1.784 |
0.000 |
2.243 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.549 |
3.507 |
0.000 |
| y |
3.507 |
-18.462 |
0.000 |
| z |
0.000 |
0.000 |
-24.492 |
|
| Traceless |
| | x | y | z |
| x |
-2.072 |
3.507 |
0.000 |
| y |
3.507 |
5.558 |
0.000 |
| z |
0.000 |
0.000 |
-3.487 |
|
| Polar |
| 3z2-r2 | -6.973 |
| x2-y2 | -5.087 |
| xy | 3.507 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.335 |
-0.290 |
0.000 |
| y |
-0.290 |
9.259 |
0.000 |
| z |
0.000 |
0.000 |
2.151 |
<r2> (average value of r
2) Å
2
| <r2> |
43.106 |
| (<r2>)1/2 |
6.566 |
Jump to
S1C1
Energy calculated at wB97X-D/CEP-31G*
| | hartrees |
| Energy at 0K | -26.280456 |
| Energy at 298.15K | |
| HF Energy | -26.280456 |
| 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 wB97X-D/CEP-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 |
3954 |
3954 |
746.81 |
|
|
|
| 2 |
Σ |
2214 |
2214 |
781.87 |
|
|
|
| 3 |
Σ |
847 |
847 |
37.10 |
|
|
|
| 4 |
Π |
473 |
473 |
7.43 |
|
|
|
| 4 |
Π |
473 |
473 |
7.43 |
|
|
|
| 5 |
Π |
259i |
259i |
182.19 |
|
|
|
| 5 |
Π |
259i |
259i |
182.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3721.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3721.8 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 wB97X-D/CEP-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.698 |
| C2 |
0.000 |
0.000 |
-0.506 |
| S3 |
0.000 |
0.000 |
1.101 |
| H4 |
0.000 |
0.000 |
-2.699 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1923 | 2.7998 | 1.0003 |
C2 | 1.1923 | | 1.6075 | 2.1926 | S3 | 2.7998 | 1.6075 | | 3.8000 | H4 | 1.0003 | 2.1926 | 3.8000 | |
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 wB97X-D/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.062 |
|
|
|
| 2 |
C |
-0.174 |
|
|
|
| 3 |
S |
-0.295 |
|
|
|
| 4 |
H |
0.406 |
|
|
|
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 |
-3.320 |
3.320 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.414 |
0.000 |
0.000 |
| y |
0.000 |
-24.414 |
0.000 |
| z |
0.000 |
0.000 |
-14.511 |
|
| Traceless |
| | x | y | z |
| x |
-4.952 |
0.000 |
0.000 |
| y |
0.000 |
-4.952 |
0.000 |
| z |
0.000 |
0.000 |
9.903 |
|
| Polar |
| 3z2-r2 | 19.806 |
| 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 |
2.091 |
0.000 |
0.000 |
| y |
0.000 |
2.091 |
0.000 |
| z |
0.000 |
0.000 |
9.031 |
<r2> (average value of r
2) Å
2
| <r2> |
43.194 |
| (<r2>)1/2 |
6.572 |