Jump to
S1C2
Energy calculated at PBEPBE/3-21G*
| | hartrees |
| Energy at 0K | -488.975368 |
| Energy at 298.15K | -488.976002 |
| HF Energy | -488.975368 |
| Nuclear repulsion energy | 79.101948 |
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/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' |
3628 |
3460 |
332.43 |
|
|
|
| 2 |
A' |
2101 |
2003 |
429.43 |
|
|
|
| 3 |
A' |
855 |
815 |
7.93 |
|
|
|
| 4 |
A' |
504 |
481 |
30.85 |
|
|
|
| 5 |
A' |
423 |
403 |
337.83 |
|
|
|
| 6 |
A" |
505 |
482 |
0.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4008.1 cm
-1
Scaled (by 0.9535) Zero Point Vibrational Energy (zpe) 3821.7 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/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.089 |
1.700 |
0.000 |
| C2 |
0.000 |
0.497 |
0.000 |
| S3 |
0.013 |
-1.091 |
0.000 |
| H4 |
0.419 |
2.575 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2057 | 2.7923 | 1.0121 |
C2 | 1.2057 | | 1.5880 | 2.1195 | S3 | 2.7923 | 1.5880 | | 3.6881 | H4 | 1.0121 | 2.1195 | 3.6881 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
176.218 |
|
C2 |
N1 |
H4 |
145.608 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.685 |
|
|
|
| 2 |
C |
0.270 |
|
|
|
| 3 |
S |
0.060 |
|
|
|
| 4 |
H |
0.356 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.048 |
2.706 |
0.000 |
2.902 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.520 |
2.751 |
0.000 |
| y |
2.751 |
-17.329 |
0.000 |
| z |
0.000 |
0.000 |
-25.017 |
|
| Traceless |
| | x | y | z |
| x |
-3.348 |
2.751 |
0.000 |
| y |
2.751 |
7.440 |
0.000 |
| z |
0.000 |
0.000 |
-4.092 |
|
| Polar |
| 3z2-r2 | -8.184 |
| x2-y2 | -7.192 |
| xy | 2.751 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.047 |
-0.088 |
0.000 |
| y |
-0.088 |
8.322 |
0.000 |
| z |
0.000 |
0.000 |
1.942 |
<r2> (average value of r
2) Å
2
| <r2> |
61.526 |
| (<r2>)1/2 |
7.844 |
Jump to
S1C1
Energy calculated at PBEPBE/3-21G*
| | hartrees |
| Energy at 0K | -488.974521 |
| Energy at 298.15K | |
| HF Energy | -488.974521 |
| Nuclear repulsion energy | 79.148510 |
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/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 |
3768 |
3593 |
632.60 |
|
|
|
| 2 |
Σ |
2158 |
2057 |
427.36 |
|
|
|
| 3 |
Σ |
847 |
808 |
19.61 |
|
|
|
| 4 |
Π |
511 |
488 |
0.39 |
|
|
|
| 4 |
Π |
511 |
488 |
0.39 |
|
|
|
| 5 |
Π |
290i |
277i |
220.19 |
|
|
|
| 5 |
Π |
290i |
277i |
220.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3607.6 cm
-1
Scaled (by 0.9535) Zero Point Vibrational Energy (zpe) 3439.9 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/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.692 |
| C2 |
0.000 |
0.000 |
-0.498 |
| S3 |
0.000 |
0.000 |
1.095 |
| H4 |
0.000 |
0.000 |
-2.693 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1940 | 2.7872 | 1.0007 |
C2 | 1.1940 | | 1.5932 | 2.1947 | S3 | 2.7872 | 1.5932 | | 3.7879 | H4 | 1.0007 | 2.1947 | 3.7879 | |
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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.733 |
|
|
|
| 2 |
C |
0.326 |
|
|
|
| 3 |
S |
0.036 |
|
|
|
| 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 |
-3.426 |
3.426 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.979 |
0.000 |
0.000 |
| y |
0.000 |
-24.979 |
0.000 |
| z |
0.000 |
0.000 |
-15.323 |
|
| Traceless |
| | x | y | z |
| x |
-4.828 |
0.000 |
0.000 |
| y |
0.000 |
-4.828 |
0.000 |
| z |
0.000 |
0.000 |
9.656 |
|
| Polar |
| 3z2-r2 | 19.313 |
| 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 |
1.936 |
0.000 |
0.000 |
| y |
0.000 |
1.936 |
0.000 |
| z |
0.000 |
0.000 |
8.105 |
<r2> (average value of r
2) Å
2
| <r2> |
61.561 |
| (<r2>)1/2 |
7.846 |