Jump to
S1C2
Energy calculated at wB97X-D/3-21G*
| | hartrees |
| Energy at 0K | -489.213348 |
| Energy at 298.15K | -489.213700 |
| HF Energy | -489.213348 |
| Nuclear repulsion energy | |
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 wB97X-D/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' |
3892 |
3689 |
740.81 |
|
|
|
| 2 |
A' |
2236 |
2120 |
553.15 |
|
|
|
| 3 |
A' |
853 |
808 |
36.83 |
|
|
|
| 4 |
A' |
534 |
507 |
3.09 |
|
|
|
| 5 |
A' |
231 |
219 |
239.94 |
|
|
|
| 6 |
A" |
408 |
387 |
97.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4076.9 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 3864.1 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 wB97X-D/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.000 |
1.678 |
0.000 |
| C2 |
0.000 |
0.500 |
0.000 |
| S3 |
0.000 |
-1.089 |
0.000 |
| H4 |
-0.000 |
2.670 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1780 | 2.7668 | 0.9921 |
C2 | 1.1780 | | 1.5888 | 2.1701 | S3 | 2.7668 | 1.5888 | | 3.7589 | H4 | 0.9921 | 2.1701 | 3.7589 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
179.993 |
|
C2 |
N1 |
H4 |
179.984 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.783 |
|
|
|
| 2 |
C |
0.391 |
|
|
|
| 3 |
S |
-0.008 |
|
|
|
| 4 |
H |
0.400 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
3.661 |
0.000 |
3.661 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.067 |
0.000 |
0.000 |
| y |
0.000 |
-15.581 |
0.000 |
| z |
0.000 |
0.000 |
-25.067 |
|
| Traceless |
| | x | y | z |
| x |
-4.743 |
0.000 |
0.000 |
| y |
0.000 |
9.486 |
0.000 |
| z |
0.000 |
0.000 |
-4.743 |
|
| Polar |
| 3z2-r2 | -9.486 |
| x2-y2 | -9.486 |
| 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 |
1.894 |
-0.001 |
0.000 |
| y |
-0.001 |
7.985 |
0.000 |
| z |
0.000 |
0.000 |
1.894 |
<r2> (average value of r
2) Å
2
| <r2> |
60.987 |
| (<r2>)1/2 |
7.809 |
Jump to
S1C1
Energy calculated at wB97X-D/3-21G*
| | hartrees |
| Energy at 0K | -489.213348 |
| Energy at 298.15K | -489.213735 |
| HF Energy | -489.213348 |
| Nuclear repulsion energy | |
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 wB97X-D/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 |
3891 |
3688 |
740.96 |
|
|
|
| 2 |
Σ |
2237 |
2120 |
553.08 |
|
|
|
| 3 |
Σ |
853 |
809 |
36.83 |
|
|
|
| 4 |
Π |
534 |
506 |
3.07 |
|
|
|
| 4 |
Π |
534 |
506 |
3.07 |
|
|
|
| 5 |
Π |
233 |
221 |
239.95 |
|
|
|
| 5 |
Π |
233 |
221 |
239.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4257.5 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 4035.3 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 wB97X-D/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.678 |
| C2 |
0.000 |
0.000 |
-0.500 |
| S3 |
0.000 |
0.000 |
1.089 |
| H4 |
0.000 |
0.000 |
-2.670 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1779 | 2.7666 | 0.9922 |
C2 | 1.1779 | | 1.5887 | 2.1701 | S3 | 2.7666 | 1.5887 | | 3.7588 | H4 | 0.9922 | 2.1701 | 3.7588 | |
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 wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.783 |
|
|
|
| 2 |
C |
0.391 |
|
|
|
| 3 |
S |
-0.008 |
|
|
|
| 4 |
H |
0.400 |
|
|
|
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 |
-3.662 |
3.662 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.067 |
0.000 |
0.000 |
| y |
0.000 |
-25.067 |
0.000 |
| z |
0.000 |
0.000 |
-15.581 |
|
| Traceless |
| | x | y | z |
| x |
-4.743 |
0.000 |
0.000 |
| y |
0.000 |
-4.743 |
0.000 |
| z |
0.000 |
0.000 |
9.486 |
|
| Polar |
| 3z2-r2 | 18.972 |
| 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 |
1.894 |
0.000 |
0.000 |
| y |
0.000 |
1.894 |
0.000 |
| z |
0.000 |
0.000 |
7.984 |
<r2> (average value of r
2) Å
2
| <r2> |
60.983 |
| (<r2>)1/2 |
7.809 |