Jump to
S1C2
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -491.633518 |
| Energy at 298.15K | -491.634262 |
| HF Energy | -491.633518 |
| Nuclear repulsion energy | 79.424594 |
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 B3LYP/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' |
3675 |
3529 |
206.75 |
|
|
|
| 2 |
A' |
2067 |
1985 |
644.68 |
|
|
|
| 3 |
A' |
876 |
842 |
2.43 |
|
|
|
| 4 |
A' |
669 |
643 |
378.76 |
|
|
|
| 5 |
A' |
454 |
436 |
64.59 |
|
|
|
| 6 |
A" |
482 |
463 |
0.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4111.4 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 3948.2 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 B3LYP/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.154 |
1.696 |
0.000 |
| C2 |
0.000 |
0.498 |
0.000 |
| S3 |
0.035 |
-1.082 |
0.000 |
| H4 |
0.514 |
2.452 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2080 | 2.7853 | 1.0090 |
C2 | 1.2080 | | 1.5811 | 2.0202 | S3 | 2.7853 | 1.5811 | | 3.5666 | H4 | 1.0090 | 2.0202 | 3.5666 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
173.938 |
|
C2 |
N1 |
H4 |
131.136 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.576 |
|
|
|
| 2 |
C |
0.278 |
|
|
|
| 3 |
S |
-0.074 |
|
|
|
| 4 |
H |
0.372 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.234 |
1.906 |
0.000 |
2.271 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.147 |
3.206 |
0.000 |
| y |
3.206 |
-19.351 |
0.000 |
| z |
0.000 |
0.000 |
-24.979 |
|
| Traceless |
| | x | y | z |
| x |
-1.983 |
3.206 |
0.000 |
| y |
3.206 |
5.213 |
0.000 |
| z |
0.000 |
0.000 |
-3.230 |
|
| Polar |
| 3z2-r2 | -6.460 |
| x2-y2 | -4.797 |
| xy | 3.206 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.490 |
-0.187 |
0.000 |
| y |
-0.187 |
8.760 |
0.000 |
| z |
0.000 |
0.000 |
2.298 |
<r2> (average value of r
2) Å
2
| <r2> |
61.099 |
| (<r2>)1/2 |
7.817 |
Jump to
S1C1
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -491.629059 |
| Energy at 298.15K | |
| HF Energy | -491.629059 |
| Nuclear repulsion energy | 79.462318 |
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 B3LYP/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 |
3920 |
3764 |
689.15 |
|
|
|
| 2 |
Σ |
2190 |
2103 |
653.92 |
|
|
|
| 3 |
Σ |
852 |
818 |
30.25 |
|
|
|
| 4 |
Π |
478 |
459 |
4.10 |
|
|
|
| 4 |
Π |
478 |
459 |
4.10 |
|
|
|
| 5 |
Π |
494i |
474i |
180.14 |
|
|
|
| 5 |
Π |
494i |
474i |
180.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3464.6 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 3327.1 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 B3LYP/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.684 |
| C2 |
0.000 |
0.000 |
-0.501 |
| S3 |
0.000 |
0.000 |
1.092 |
| H4 |
0.000 |
0.000 |
-2.677 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1829 | 2.7760 | 0.9933 |
C2 | 1.1829 | | 1.5931 | 2.1762 | S3 | 2.7760 | 1.5931 | | 3.7693 | H4 | 0.9933 | 2.1762 | 3.7693 | |
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 B3LYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.564 |
|
|
|
| 2 |
C |
0.313 |
|
|
|
| 3 |
S |
-0.120 |
|
|
|
| 4 |
H |
0.371 |
|
|
|
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 |
-3.319 |
3.319 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.916 |
0.000 |
0.000 |
| y |
0.000 |
-24.916 |
0.000 |
| z |
0.000 |
0.000 |
-15.686 |
|
| Traceless |
| | x | y | z |
| x |
-4.615 |
0.000 |
0.000 |
| y |
0.000 |
-4.615 |
0.000 |
| z |
0.000 |
0.000 |
9.230 |
|
| Polar |
| 3z2-r2 | 18.460 |
| 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 |
2.292 |
0.000 |
0.000 |
| y |
0.000 |
2.292 |
0.000 |
| z |
0.000 |
0.000 |
8.479 |
<r2> (average value of r
2) Å
2
| <r2> |
61.245 |
| (<r2>)1/2 |
7.826 |