Jump to
S1C2
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -489.180177 |
| Energy at 298.15K | -489.180506 |
| HF Energy | -489.180177 |
| Nuclear repulsion energy | 79.664107 |
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 B3PW91/3-21G*
| 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' |
3832 |
3676 |
628.47 |
|
|
|
| 2 |
A' |
2204 |
2114 |
514.95 |
|
|
|
| 3 |
A' |
866 |
831 |
23.27 |
|
|
|
| 4 |
A' |
526 |
504 |
0.56 |
|
|
|
| 5 |
A' |
151 |
145 |
289.46 |
|
|
|
| 6 |
A" |
529 |
507 |
0.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4053.1 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 3888.5 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 B3PW91/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.033 |
1.682 |
0.000 |
| C2 |
0.000 |
0.497 |
0.000 |
| S3 |
0.001 |
-1.088 |
0.000 |
| H4 |
0.219 |
2.645 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1852 | 2.7696 | 0.9959 |
C2 | 1.1852 | | 1.5847 | 2.1593 | S3 | 2.7696 | 1.5847 | | 3.7392 | H4 | 0.9959 | 2.1593 | 3.7392 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
178.426 |
|
C2 |
N1 |
H4 |
163.724 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.767 |
|
|
|
| 2 |
C |
0.353 |
|
|
|
| 3 |
S |
0.025 |
|
|
|
| 4 |
H |
0.388 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.574 |
3.334 |
0.000 |
3.383 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.893 |
1.526 |
0.000 |
| y |
1.526 |
-15.979 |
0.000 |
| z |
0.000 |
0.000 |
-25.031 |
|
| Traceless |
| | x | y | z |
| x |
-4.388 |
1.526 |
0.000 |
| y |
1.526 |
8.983 |
0.000 |
| z |
0.000 |
0.000 |
-4.596 |
|
| Polar |
| 3z2-r2 | -9.191 |
| x2-y2 | -8.914 |
| xy | 1.526 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.937 |
-0.049 |
0.000 |
| y |
-0.049 |
8.057 |
0.000 |
| z |
0.000 |
0.000 |
1.917 |
<r2> (average value of r
2) Å
2
| <r2> |
60.981 |
| (<r2>)1/2 |
7.809 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -489.180157 |
| Energy at 298.15K | |
| HF Energy | -489.180157 |
| Nuclear repulsion energy | 79.662886 |
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 B3PW91/3-21G*
| 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 |
3860 |
3703 |
709.77 |
|
|
|
| 2 |
Σ |
2217 |
2127 |
507.93 |
|
|
|
| 3 |
Σ |
863 |
828 |
28.13 |
|
|
|
| 4 |
Π |
531 |
509 |
0.35 |
|
|
|
| 4 |
Π |
531 |
509 |
0.35 |
|
|
|
| 5 |
Π |
92i |
88i |
236.90 |
|
|
|
| 5 |
Π |
92i |
88i |
236.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3908.5 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 3749.8 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 B3PW91/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.680 |
| C2 |
0.000 |
0.000 |
-0.498 |
| S3 |
0.000 |
0.000 |
1.089 |
| H4 |
0.000 |
0.000 |
-2.674 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1825 | 2.7688 | 0.9935 |
C2 | 1.1825 | | 1.5863 | 2.1760 | S3 | 2.7688 | 1.5863 | | 3.7623 | H4 | 0.9935 | 2.1760 | 3.7623 | |
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 B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.781 |
|
|
|
| 2 |
C |
0.369 |
|
|
|
| 3 |
S |
0.019 |
|
|
|
| 4 |
H |
0.393 |
|
|
|
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 |
-3.515 |
3.515 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.025 |
0.000 |
0.000 |
| y |
0.000 |
-25.025 |
0.000 |
| z |
0.000 |
0.000 |
-15.480 |
|
| Traceless |
| | x | y | z |
| x |
-4.772 |
0.000 |
0.000 |
| y |
0.000 |
-4.772 |
0.000 |
| z |
0.000 |
0.000 |
9.545 |
|
| Polar |
| 3z2-r2 | 19.089 |
| 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 |
1.915 |
0.000 |
0.000 |
| y |
0.000 |
1.915 |
0.000 |
| z |
0.000 |
0.000 |
7.995 |
<r2> (average value of r
2) Å
2
| <r2> |
61.001 |
| (<r2>)1/2 |
7.810 |