Jump to
S1C2
Energy calculated at BLYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.674868 |
| Energy at 298.15K | -491.675612 |
| HF Energy | -491.674868 |
| Nuclear repulsion energy | 79.208670 |
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/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' |
3557 |
3546 |
164.80 |
|
|
|
| 2 |
A' |
1973 |
1967 |
569.26 |
|
|
|
| 3 |
A' |
847 |
844 |
1.08 |
|
|
|
| 4 |
A' |
684 |
682 |
327.99 |
|
|
|
| 5 |
A' |
448 |
447 |
43.20 |
|
|
|
| 6 |
A" |
469 |
468 |
3.98 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3988.7 cm
-1
Scaled (by 0.997) Zero Point Vibrational Energy (zpe) 3976.8 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 BLYP/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.166 |
1.701 |
0.000 |
| C2 |
0.000 |
0.499 |
0.000 |
| S3 |
0.041 |
-1.085 |
0.000 |
| H4 |
0.510 |
2.455 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2132 | 2.7931 | 1.0126 |
C2 | 1.2132 | | 1.5842 | 2.0209 | S3 | 2.7931 | 1.5842 | | 3.5701 | H4 | 1.0126 | 2.0209 | 3.5701 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
173.602 |
|
C2 |
N1 |
H4 |
130.230 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.125 |
|
|
|
| 2 |
C |
0.025 |
|
|
|
| 3 |
S |
-0.088 |
|
|
|
| 4 |
H |
0.188 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.084 |
1.564 |
0.000 |
1.903 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.464 |
2.909 |
0.000 |
| y |
2.909 |
-19.605 |
0.000 |
| z |
0.000 |
0.000 |
-25.264 |
|
| Traceless |
| | x | y | z |
| x |
-2.029 |
2.909 |
0.000 |
| y |
2.909 |
5.259 |
0.000 |
| z |
0.000 |
0.000 |
-3.229 |
|
| Polar |
| 3z2-r2 | -6.459 |
| x2-y2 | -4.858 |
| xy | 2.909 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.288 |
-0.201 |
0.000 |
| y |
-0.201 |
9.421 |
0.000 |
| z |
0.000 |
0.000 |
3.130 |
<r2> (average value of r
2) Å
2
| <r2> |
61.504 |
| (<r2>)1/2 |
7.842 |
Jump to
S1C1
Energy calculated at BLYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.669681 |
| Energy at 298.15K | |
| HF Energy | -491.669681 |
| Nuclear repulsion energy | 79.275285 |
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/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 |
3808 |
3797 |
629.16 |
|
|
|
| 2 |
Σ |
2088 |
2081 |
622.96 |
|
|
|
| 3 |
Σ |
829 |
826 |
19.67 |
|
|
|
| 4 |
Π |
466 |
464 |
8.69 |
|
|
|
| 4 |
Π |
466 |
464 |
8.69 |
|
|
|
| 5 |
Π |
529i |
527i |
138.46 |
|
|
|
| 5 |
Π |
529i |
527i |
138.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3298.7 cm
-1
Scaled (by 0.997) Zero Point Vibrational Energy (zpe) 3288.8 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 BLYP/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.689 |
| C2 |
0.000 |
0.000 |
-0.500 |
| S3 |
0.000 |
0.000 |
1.094 |
| H4 |
0.000 |
0.000 |
-2.684 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1882 | 2.7828 | 0.9957 |
C2 | 1.1882 | | 1.5947 | 2.1839 | S3 | 2.7828 | 1.5947 | | 3.7785 | H4 | 0.9957 | 2.1839 | 3.7785 | |
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/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.115 |
|
|
|
| 2 |
C |
0.045 |
|
|
|
| 3 |
S |
-0.144 |
|
|
|
| 4 |
H |
0.214 |
|
|
|
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 |
-2.926 |
2.926 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.225 |
0.000 |
0.000 |
| y |
0.000 |
-25.225 |
0.000 |
| z |
0.000 |
0.000 |
-16.080 |
|
| Traceless |
| | x | y | z |
| x |
-4.572 |
0.000 |
0.000 |
| y |
0.000 |
-4.572 |
0.000 |
| z |
0.000 |
0.000 |
9.144 |
|
| Polar |
| 3z2-r2 | 18.289 |
| 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 |
3.110 |
0.000 |
0.000 |
| y |
0.000 |
3.110 |
0.000 |
| z |
0.000 |
0.000 |
9.214 |
<r2> (average value of r
2) Å
2
| <r2> |
61.676 |
| (<r2>)1/2 |
7.853 |