Jump to
S1C2
Energy calculated at PBE1PBE/6-31G
| | hartrees |
| Energy at 0K | -491.309644 |
| Energy at 298.15K | -491.309940 |
| HF Energy | -491.309644 |
| Nuclear repulsion energy | 78.422036 |
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 PBE1PBE/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' |
3936 |
3763 |
605.38 |
|
|
|
| 2 |
A' |
2186 |
2090 |
573.45 |
|
|
|
| 3 |
A' |
806 |
770 |
20.51 |
|
|
|
| 4 |
A' |
440 |
420 |
1.75 |
|
|
|
| 5 |
A' |
233 |
222 |
315.02 |
|
|
|
| 6 |
A" |
441 |
422 |
2.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4020.7 cm
-1
Scaled (by 0.9559) Zero Point Vibrational Energy (zpe) 3843.4 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 PBE1PBE/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.071 |
1.706 |
0.000 |
| C2 |
0.000 |
0.520 |
0.000 |
| S3 |
0.020 |
-1.108 |
0.000 |
| H4 |
0.177 |
2.667 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1878 | 2.8149 | 0.9925 |
C2 | 1.1878 | | 1.6278 | 2.1541 | S3 | 2.8149 | 1.6278 | | 3.7778 | H4 | 0.9925 | 2.1541 | 3.7778 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
177.282 |
|
C2 |
N1 |
H4 |
162.121 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.574 |
|
|
|
| 2 |
C |
0.077 |
|
|
|
| 3 |
S |
0.097 |
|
|
|
| 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 |
| |
0.575 |
3.512 |
0.000 |
3.559 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.156 |
1.542 |
0.000 |
| y |
1.542 |
-16.859 |
0.000 |
| z |
0.000 |
0.000 |
-25.246 |
|
| Traceless |
| | x | y | z |
| x |
-4.104 |
1.542 |
0.000 |
| y |
1.542 |
8.342 |
0.000 |
| z |
0.000 |
0.000 |
-4.238 |
|
| Polar |
| 3z2-r2 | -8.477 |
| x2-y2 | -8.298 |
| xy | 1.542 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.974 |
-0.211 |
0.000 |
| y |
-0.211 |
8.670 |
0.000 |
| z |
0.000 |
0.000 |
1.937 |
<r2> (average value of r
2) Å
2
| <r2> |
62.808 |
| (<r2>)1/2 |
7.925 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-31G
| | hartrees |
| Energy at 0K | -491.309576 |
| Energy at 298.15K | |
| HF Energy | -491.309576 |
| Nuclear repulsion energy | 78.422749 |
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 PBE1PBE/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 |
3971 |
3796 |
696.90 |
|
|
|
| 2 |
Σ |
2202 |
2105 |
569.29 |
|
|
|
| 3 |
Σ |
801 |
766 |
25.75 |
|
|
|
| 4 |
Π |
440 |
421 |
2.98 |
|
|
|
| 4 |
Π |
440 |
421 |
2.98 |
|
|
|
| 5 |
Π |
166i |
159i |
251.62 |
|
|
|
| 5 |
Π |
166i |
159i |
251.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3760.8 cm
-1
Scaled (by 0.9559) Zero Point Vibrational Energy (zpe) 3595.0 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 PBE1PBE/6-31G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.705 |
| C2 |
0.000 |
0.000 |
-0.521 |
| S3 |
0.000 |
0.000 |
1.109 |
| H4 |
0.000 |
0.000 |
-2.695 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1842 | 2.8142 | 0.9901 |
C2 | 1.1842 | | 1.6300 | 2.1743 | S3 | 2.8142 | 1.6300 | | 3.8043 | H4 | 0.9901 | 2.1743 | 3.8043 | |
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 PBE1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.579 |
|
|
|
| 2 |
C |
0.084 |
|
|
|
| 3 |
S |
0.090 |
|
|
|
| 4 |
H |
0.405 |
|
|
|
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 |
-3.709 |
3.709 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.240 |
0.000 |
0.000 |
| y |
0.000 |
-25.240 |
0.000 |
| z |
0.000 |
0.000 |
-16.366 |
|
| Traceless |
| | x | y | z |
| x |
-4.437 |
0.000 |
0.000 |
| y |
0.000 |
-4.437 |
0.000 |
| z |
0.000 |
0.000 |
8.874 |
|
| Polar |
| 3z2-r2 | 17.748 |
| 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 |
1.937 |
0.000 |
0.000 |
| y |
0.000 |
1.937 |
0.000 |
| z |
0.000 |
0.000 |
8.610 |
<r2> (average value of r
2) Å
2
| <r2> |
62.841 |
| (<r2>)1/2 |
7.927 |