Jump to
S1C2
Energy calculated at B2PLYP/6-31G
| | hartrees |
| Energy at 0K | -491.274915 |
| Energy at 298.15K | -491.275409 |
| HF Energy | -491.179945 |
| Nuclear repulsion energy | 77.778425 |
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' |
3835 |
3835 |
436.60 |
|
|
|
| 2 |
A' |
2082 |
2082 |
506.67 |
|
|
|
| 3 |
A' |
781 |
781 |
10.02 |
|
|
|
| 4 |
A' |
460 |
460 |
372.38 |
|
|
|
| 5 |
A' |
415 |
415 |
40.85 |
|
|
|
| 6 |
A" |
417 |
417 |
8.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3995.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3995.5 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 |
-0.144 |
1.720 |
0.000 |
| C2 |
0.000 |
0.525 |
0.000 |
| S3 |
0.047 |
-1.114 |
0.000 |
| H4 |
0.249 |
2.638 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2033 | 2.8400 | 0.9989 |
C2 | 1.2033 | | 1.6395 | 2.1277 | S3 | 2.8400 | 1.6395 | | 3.7574 | H4 | 0.9989 | 2.1277 | 3.7574 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.791 |
|
C2 |
N1 |
H4 |
149.982 |
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 |
-0.531 |
|
|
|
| 2 |
C |
0.065 |
|
|
|
| 3 |
S |
0.087 |
|
|
|
| 4 |
H |
0.380 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.859 |
3.236 |
0.000 |
3.348 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.308 |
2.321 |
0.000 |
| y |
2.321 |
-17.682 |
0.000 |
| z |
0.000 |
0.000 |
-25.471 |
|
| Traceless |
| | x | y | z |
| x |
-3.731 |
2.321 |
0.000 |
| y |
2.321 |
7.707 |
0.000 |
| z |
0.000 |
0.000 |
-3.976 |
|
| Polar |
| 3z2-r2 | -7.952 |
| x2-y2 | -7.625 |
| xy | 2.321 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.055 |
-0.417 |
0.000 |
| y |
-0.417 |
9.156 |
0.000 |
| z |
0.000 |
0.000 |
1.935 |
<r2> (average value of r
2) Å
2
| <r2> |
63.661 |
| (<r2>)1/2 |
7.979 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31G
| | hartrees |
| Energy at 0K | -491.274088 |
| Energy at 298.15K | |
| HF Energy | -491.181136 |
| Nuclear repulsion energy | 77.787646 |
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 |
3928 |
3928 |
678.58 |
|
|
|
| 2 |
Σ |
2128 |
2128 |
512.54 |
|
|
|
| 3 |
Σ |
766 |
766 |
25.00 |
|
|
|
| 4 |
Π |
413 |
413 |
8.35 |
|
|
|
| 4 |
Π |
413 |
413 |
8.35 |
|
|
|
| 5 |
Π |
348i |
348i |
238.97 |
|
|
|
| 5 |
Π |
348i |
348i |
238.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3476.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3476.5 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 C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.719 |
| C2 |
0.000 |
0.000 |
-0.527 |
| S3 |
0.000 |
0.000 |
1.119 |
| H4 |
0.000 |
0.000 |
-2.711 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1921 | 2.8381 | 0.9924 |
C2 | 1.1921 | | 1.6460 | 2.1844 | S3 | 2.8381 | 1.6460 | | 3.8304 | H4 | 0.9924 | 2.1844 | 3.8304 | |
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 |
-0.546 |
|
|
|
| 2 |
C |
0.084 |
|
|
|
| 3 |
S |
0.065 |
|
|
|
| 4 |
H |
0.396 |
|
|
|
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 |
-3.798 |
3.798 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.463 |
0.000 |
0.000 |
| y |
0.000 |
-25.463 |
0.000 |
| z |
0.000 |
0.000 |
-16.369 |
|
| Traceless |
| | x | y | z |
| x |
-4.547 |
0.000 |
0.000 |
| y |
0.000 |
-4.547 |
0.000 |
| z |
0.000 |
0.000 |
9.094 |
|
| Polar |
| 3z2-r2 | 18.188 |
| 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 |
1.934 |
0.000 |
0.000 |
| y |
0.000 |
1.934 |
0.000 |
| z |
0.000 |
0.000 |
8.972 |
<r2> (average value of r
2) Å
2
| <r2> |
63.749 |
| (<r2>)1/2 |
7.984 |