Jump to
S1C2
Energy calculated at B2PLYP/6-31G*
| | hartrees |
| Energy at 0K | -491.385276 |
| Energy at 298.15K | -491.386016 |
| HF Energy | -491.243876 |
| Nuclear repulsion energy | 79.363948 |
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 B2PLYP/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' |
3704 |
3516 |
224.90 |
|
|
|
| 2 |
A' |
2056 |
1951 |
595.75 |
|
|
|
| 3 |
A' |
879 |
835 |
1.97 |
|
|
|
| 4 |
A' |
675 |
641 |
407.21 |
|
|
|
| 5 |
A' |
452 |
429 |
58.19 |
|
|
|
| 6 |
A" |
474 |
450 |
1.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4119.8 cm
-1
Scaled (by 0.9492) Zero Point Vibrational Energy (zpe) 3910.5 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 B2PLYP/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.173 |
1.696 |
0.000 |
| C2 |
0.000 |
0.497 |
0.000 |
| S3 |
0.046 |
-1.083 |
0.000 |
| H4 |
0.478 |
2.465 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2120 | 2.7875 | 1.0079 |
C2 | 1.2120 | | 1.5800 | 2.0256 | S3 | 2.7875 | 1.5800 | | 3.5739 | H4 | 1.0079 | 2.0256 | 3.5739 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
173.440 |
|
C2 |
N1 |
H4 |
131.484 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.574 |
|
|
|
| 2 |
C |
0.253 |
|
|
|
| 3 |
S |
-0.063 |
|
|
|
| 4 |
H |
0.384 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.209 |
1.943 |
0.000 |
2.288 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.360 |
3.147 |
0.000 |
| y |
3.147 |
-19.193 |
0.000 |
| z |
0.000 |
0.000 |
-25.103 |
|
| Traceless |
| | x | y | z |
| x |
-2.212 |
3.147 |
0.000 |
| y |
3.147 |
5.538 |
0.000 |
| z |
0.000 |
0.000 |
-3.326 |
|
| Polar |
| 3z2-r2 | -6.652 |
| x2-y2 | -5.167 |
| xy | 3.147 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.483 |
-0.287 |
0.000 |
| y |
-0.287 |
8.971 |
0.000 |
| z |
0.000 |
0.000 |
2.283 |
<r2> (average value of r
2) Å
2
| <r2> |
61.218 |
| (<r2>)1/2 |
7.824 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31G*
| | hartrees |
| Energy at 0K | -491.380579 |
| Energy at 298.15K | |
| HF Energy | -491.241181 |
| Nuclear repulsion energy | 79.426045 |
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 B2PLYP/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 |
3931 |
3731 |
704.72 |
|
|
|
| 2 |
Σ |
2173 |
2063 |
609.83 |
|
|
|
| 3 |
Σ |
858 |
814 |
29.09 |
|
|
|
| 4 |
Π |
469 |
446 |
5.99 |
|
|
|
| 4 |
Π |
469 |
446 |
5.99 |
|
|
|
| 5 |
Π |
515i |
489i |
181.70 |
|
|
|
| 5 |
Π |
515i |
489i |
181.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3434.9 cm
-1
Scaled (by 0.9492) Zero Point Vibrational Energy (zpe) 3260.4 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 B2PLYP/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.686 |
| C2 |
0.000 |
0.000 |
-0.499 |
| S3 |
0.000 |
0.000 |
1.092 |
| H4 |
0.000 |
0.000 |
-2.679 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1861 | 2.7777 | 0.9933 |
C2 | 1.1861 | | 1.5915 | 2.1794 | S3 | 2.7777 | 1.5915 | | 3.7709 | H4 | 0.9933 | 2.1794 | 3.7709 | |
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 B2PLYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.566 |
|
|
|
| 2 |
C |
0.290 |
|
|
|
| 3 |
S |
-0.113 |
|
|
|
| 4 |
H |
0.390 |
|
|
|
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 |
-3.358 |
3.358 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.052 |
0.000 |
0.000 |
| y |
0.000 |
-25.052 |
0.000 |
| z |
0.000 |
0.000 |
-15.631 |
|
| Traceless |
| | x | y | z |
| x |
-4.710 |
0.000 |
0.000 |
| y |
0.000 |
-4.710 |
0.000 |
| z |
0.000 |
0.000 |
9.420 |
|
| Polar |
| 3z2-r2 | 18.841 |
| 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 |
2.278 |
0.000 |
0.000 |
| y |
0.000 |
2.278 |
0.000 |
| z |
0.000 |
0.000 |
8.666 |
<r2> (average value of r
2) Å
2
| <r2> |
61.329 |
| (<r2>)1/2 |
7.831 |