Jump to
S1C2
Energy calculated at HF/cc-pVTZ
| | hartrees |
| Energy at 0K | -490.464262 |
| Energy at 298.15K | -490.464952 |
| HF Energy | -490.464262 |
| Nuclear repulsion energy | 80.528426 |
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 HF/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' |
3931 |
3578 |
459.05 |
|
|
|
| 2 |
A' |
2192 |
1995 |
1154.57 |
|
|
|
| 3 |
A' |
895 |
815 |
22.36 |
|
|
|
| 4 |
A' |
582 |
529 |
104.02 |
|
|
|
| 5 |
A' |
373 |
340 |
504.91 |
|
|
|
| 6 |
A" |
547 |
498 |
0.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4260.2 cm
-1
Scaled (by 0.9101) Zero Point Vibrational Energy (zpe) 3877.2 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 HF/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.089 |
1.670 |
0.000 |
| C2 |
0.000 |
0.503 |
0.000 |
| S3 |
0.006 |
-1.072 |
0.000 |
| H4 |
0.523 |
2.447 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1705 | 2.7445 | 0.9885 |
C2 | 1.1705 | | 1.5758 | 2.0124 | S3 | 2.7445 | 1.5758 | | 3.5567 | H4 | 0.9885 | 2.0124 | 3.5567 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
175.854 |
|
C2 |
N1 |
H4 |
137.372 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.185 |
|
|
|
| 2 |
C |
0.162 |
|
|
|
| 3 |
S |
-0.229 |
|
|
|
| 4 |
H |
0.252 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.162 |
2.384 |
0.000 |
2.652 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.751 |
3.086 |
0.000 |
| y |
3.086 |
-19.106 |
0.000 |
| z |
0.000 |
0.000 |
-25.614 |
|
| Traceless |
| | x | y | z |
| x |
-2.391 |
3.086 |
0.000 |
| y |
3.086 |
6.076 |
0.000 |
| z |
0.000 |
0.000 |
-3.685 |
|
| Polar |
| 3z2-r2 | -7.370 |
| x2-y2 | -5.645 |
| xy | 3.086 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.128 |
-0.062 |
0.000 |
| y |
-0.062 |
8.785 |
0.000 |
| z |
0.000 |
0.000 |
3.042 |
<r2> (average value of r
2) Å
2
| <r2> |
60.232 |
| (<r2>)1/2 |
7.761 |
Jump to
S1C1
Energy calculated at HF/cc-pVTZ
| | hartrees |
| Energy at 0K | -490.463454 |
| Energy at 298.15K | |
| HF Energy | -490.463454 |
| Nuclear repulsion energy | 80.430886 |
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 HF/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 |
4081 |
3714 |
890.85 |
|
|
|
| 2 |
Σ |
2314 |
2106 |
1069.35 |
|
|
|
| 3 |
Σ |
856 |
779 |
75.34 |
|
|
|
| 4 |
Π |
541 |
493 |
0.52 |
|
|
|
| 4 |
Π |
541 |
493 |
0.52 |
|
|
|
| 5 |
Π |
208i |
189i |
175.90 |
|
|
|
| 5 |
Π |
208i |
189i |
175.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3958.8 cm
-1
Scaled (by 0.9101) Zero Point Vibrational Energy (zpe) 3602.9 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 HF/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.659 |
| C2 |
0.000 |
0.000 |
-0.510 |
| S3 |
0.000 |
0.000 |
1.082 |
| H4 |
0.000 |
0.000 |
-2.638 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1490 | 2.7410 | 0.9787 |
C2 | 1.1490 | | 1.5920 | 2.1277 | S3 | 2.7410 | 1.5920 | | 3.7196 | H4 | 0.9787 | 2.1277 | 3.7196 | |
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 HF/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.160 |
|
|
|
| 2 |
C |
0.166 |
|
|
|
| 3 |
S |
-0.289 |
|
|
|
| 4 |
H |
0.283 |
|
|
|
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 |
-3.738 |
3.738 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.607 |
0.000 |
0.000 |
| y |
0.000 |
-25.607 |
0.000 |
| z |
0.000 |
0.000 |
-15.939 |
|
| Traceless |
| | x | y | z |
| x |
-4.834 |
0.000 |
0.000 |
| y |
0.000 |
-4.834 |
0.000 |
| z |
0.000 |
0.000 |
9.668 |
|
| Polar |
| 3z2-r2 | 19.336 |
| 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 |
3.029 |
0.000 |
0.000 |
| y |
0.000 |
3.029 |
0.000 |
| z |
0.000 |
0.000 |
8.504 |
<r2> (average value of r
2) Å
2
| <r2> |
60.495 |
| (<r2>)1/2 |
7.778 |