Jump to
S1C2
Energy calculated at BLYP/6-31G
| | hartrees |
| Energy at 0K | -491.545533 |
| Energy at 298.15K | -491.546050 |
| HF Energy | -491.545533 |
| Nuclear repulsion energy | 77.473518 |
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 BLYP/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' |
3692 |
3663 |
296.80 |
|
|
|
| 2 |
A' |
2038 |
2022 |
452.90 |
|
|
|
| 3 |
A' |
772 |
766 |
5.43 |
|
|
|
| 4 |
A' |
485 |
482 |
343.70 |
|
|
|
| 5 |
A' |
415 |
412 |
30.61 |
|
|
|
| 6 |
A" |
423 |
420 |
6.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3912.2 cm
-1
Scaled (by 0.9924) Zero Point Vibrational Energy (zpe) 3882.5 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 BLYP/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.153 |
1.728 |
0.000 |
| C2 |
0.000 |
0.524 |
0.000 |
| S3 |
0.048 |
-1.117 |
0.000 |
| H4 |
0.307 |
2.625 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2130 | 2.8516 | 1.0086 |
C2 | 1.2130 | | 1.6418 | 2.1232 | S3 | 2.8516 | 1.6418 | | 3.7511 | H4 | 1.0086 | 2.1232 | 3.7511 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.416 |
|
C2 |
N1 |
H4 |
145.622 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.468 |
|
|
|
| 2 |
C |
0.043 |
|
|
|
| 3 |
S |
0.086 |
|
|
|
| 4 |
H |
0.339 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.956 |
2.852 |
0.000 |
3.008 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.885 |
2.567 |
0.000 |
| y |
2.567 |
-18.021 |
0.000 |
| z |
0.000 |
0.000 |
-25.134 |
|
| Traceless |
| | x | y | z |
| x |
-3.307 |
2.567 |
0.000 |
| y |
2.567 |
6.988 |
0.000 |
| z |
0.000 |
0.000 |
-3.681 |
|
| Polar |
| 3z2-r2 | -7.363 |
| x2-y2 | -6.864 |
| xy | 2.567 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.116 |
-0.362 |
0.000 |
| y |
-0.362 |
8.978 |
0.000 |
| z |
0.000 |
0.000 |
1.972 |
<r2> (average value of r
2) Å
2
| <r2> |
63.852 |
| (<r2>)1/2 |
7.991 |
Jump to
S1C1
Energy calculated at BLYP/6-31G
| | hartrees |
| Energy at 0K | -491.544370 |
| Energy at 298.15K | |
| HF Energy | -491.544370 |
| Nuclear repulsion energy | 77.527404 |
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 BLYP/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 |
3839 |
3810 |
591.40 |
|
|
|
| 2 |
Σ |
2099 |
2083 |
472.20 |
|
|
|
| 3 |
Σ |
760 |
755 |
16.99 |
|
|
|
| 4 |
Π |
421 |
417 |
5.99 |
|
|
|
| 4 |
Π |
421 |
417 |
5.99 |
|
|
|
| 5 |
Π |
353i |
351i |
222.33 |
|
|
|
| 5 |
Π |
353i |
351i |
222.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3416.7 cm
-1
Scaled (by 0.9924) Zero Point Vibrational Energy (zpe) 3390.7 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 BLYP/6-31G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.725 |
| C2 |
0.000 |
0.000 |
-0.526 |
| S3 |
0.000 |
0.000 |
1.122 |
| H4 |
0.000 |
0.000 |
-2.724 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1994 | 2.8474 | 0.9984 |
C2 | 1.1994 | | 1.6480 | 2.1978 | S3 | 2.8474 | 1.6480 | | 3.8458 | H4 | 0.9984 | 2.1978 | 3.8458 | |
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 BLYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.476 |
|
|
|
| 2 |
C |
0.059 |
|
|
|
| 3 |
S |
0.064 |
|
|
|
| 4 |
H |
0.352 |
|
|
|
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 |
-3.519 |
3.519 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.105 |
0.000 |
0.000 |
| y |
0.000 |
-25.105 |
0.000 |
| z |
0.000 |
0.000 |
-16.299 |
|
| Traceless |
| | x | y | z |
| x |
-4.403 |
0.000 |
0.000 |
| y |
0.000 |
-4.403 |
0.000 |
| z |
0.000 |
0.000 |
8.806 |
|
| Polar |
| 3z2-r2 | 17.612 |
| 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 |
1.970 |
0.000 |
0.000 |
| y |
0.000 |
1.970 |
0.000 |
| z |
0.000 |
0.000 |
8.778 |
<r2> (average value of r
2) Å
2
| <r2> |
63.907 |
| (<r2>)1/2 |
7.994 |