Jump to
S1C2
Energy calculated at PBEPBE/6-31G*
| | hartrees |
| Energy at 0K | -491.342536 |
| Energy at 298.15K | -491.343265 |
| HF Energy | -491.342536 |
| Nuclear repulsion energy | 79.004956 |
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 PBEPBE/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' |
3588 |
3537 |
160.57 |
|
|
|
| 2 |
A' |
2023 |
1994 |
526.16 |
|
|
|
| 3 |
A' |
866 |
854 |
1.40 |
|
|
|
| 4 |
A' |
694 |
684 |
342.37 |
|
|
|
| 5 |
A' |
442 |
436 |
42.05 |
|
|
|
| 6 |
A" |
465 |
458 |
2.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4039.1 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 3981.4 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 PBEPBE/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.184 |
1.704 |
0.000 |
| C2 |
0.000 |
0.498 |
0.000 |
| S3 |
0.050 |
-1.086 |
0.000 |
| H4 |
0.494 |
2.462 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2202 | 2.8004 | 1.0167 |
C2 | 1.2202 | | 1.5852 | 2.0247 | S3 | 2.8004 | 1.5852 | | 3.5756 | H4 | 1.0167 | 2.0247 | 3.5756 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
173.114 |
|
C2 |
N1 |
H4 |
129.458 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.555 |
|
|
|
| 2 |
C |
0.237 |
|
|
|
| 3 |
S |
-0.048 |
|
|
|
| 4 |
H |
0.366 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.196 |
1.808 |
0.000 |
2.168 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.144 |
3.121 |
0.000 |
| y |
3.121 |
-19.162 |
0.000 |
| z |
0.000 |
0.000 |
-24.930 |
|
| Traceless |
| | x | y | z |
| x |
-2.098 |
3.121 |
0.000 |
| y |
3.121 |
5.375 |
0.000 |
| z |
0.000 |
0.000 |
-3.277 |
|
| Polar |
| 3z2-r2 | -6.554 |
| x2-y2 | -4.982 |
| xy | 3.121 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.540 |
-0.265 |
0.000 |
| y |
-0.265 |
8.876 |
0.000 |
| z |
0.000 |
0.000 |
2.323 |
<r2> (average value of r
2) Å
2
| <r2> |
61.490 |
| (<r2>)1/2 |
7.842 |
Jump to
S1C1
Energy calculated at PBEPBE/6-31G*
| | hartrees |
| Energy at 0K | -491.336878 |
| Energy at 298.15K | |
| HF Energy | -491.336878 |
| Nuclear repulsion energy | 79.106831 |
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 PBEPBE/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 |
3853 |
3798 |
629.24 |
|
|
|
| 2 |
Σ |
2145 |
2114 |
554.35 |
|
|
|
| 3 |
Σ |
851 |
838 |
20.09 |
|
|
|
| 4 |
Π |
460 |
454 |
6.71 |
|
|
|
| 4 |
Π |
460 |
454 |
6.71 |
|
|
|
| 5 |
Π |
543i |
535i |
169.73 |
|
|
|
| 5 |
Π |
543i |
535i |
169.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3341.5 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 3293.7 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 PBEPBE/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.693 |
| C2 |
0.000 |
0.000 |
-0.499 |
| S3 |
0.000 |
0.000 |
1.096 |
| H4 |
0.000 |
0.000 |
-2.692 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1943 | 2.7890 | 0.9993 |
C2 | 1.1943 | | 1.5946 | 2.1936 | S3 | 2.7890 | 1.5946 | | 3.7882 | H4 | 0.9993 | 2.1936 | 3.7882 | |
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 PBEPBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.547 |
|
|
|
| 2 |
C |
0.273 |
|
|
|
| 3 |
S |
-0.092 |
|
|
|
| 4 |
H |
0.366 |
|
|
|
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 |
-3.190 |
3.190 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.852 |
0.000 |
0.000 |
| y |
0.000 |
-24.852 |
0.000 |
| z |
0.000 |
0.000 |
-15.467 |
|
| Traceless |
| | x | y | z |
| x |
-4.692 |
0.000 |
0.000 |
| y |
0.000 |
-4.692 |
0.000 |
| z |
0.000 |
0.000 |
9.385 |
|
| Polar |
| 3z2-r2 | 18.770 |
| 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 |
2.315 |
0.000 |
0.000 |
| y |
0.000 |
2.315 |
0.000 |
| z |
0.000 |
0.000 |
8.619 |
<r2> (average value of r
2) Å
2
| <r2> |
61.590 |
| (<r2>)1/2 |
7.848 |