Jump to
S1C2
Energy calculated at B3PW91/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.616782 |
| Energy at 298.15K | -491.617551 |
| HF Energy | -491.616782 |
| Nuclear repulsion energy | 79.985493 |
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 B3PW91/cc-pVTZ
| 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' |
3698 |
3556 |
242.03 |
|
|
|
| 2 |
A' |
2066 |
1987 |
709.77 |
|
|
|
| 3 |
A' |
888 |
854 |
2.73 |
|
|
|
| 4 |
A' |
644 |
619 |
327.20 |
|
|
|
| 5 |
A' |
462 |
444 |
84.88 |
|
|
|
| 6 |
A" |
494 |
476 |
2.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4126.0 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 3967.6 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 B3PW91/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.143 |
1.685 |
0.000 |
| C2 |
0.000 |
0.494 |
0.000 |
| S3 |
0.030 |
-1.075 |
0.000 |
| H4 |
0.519 |
2.439 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1991 | 2.7653 | 1.0039 |
C2 | 1.1991 | | 1.5697 | 2.0132 | S3 | 2.7653 | 1.5697 | | 3.5483 | H4 | 1.0039 | 2.0132 | 3.5483 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.255 |
|
C2 |
N1 |
H4 |
131.884 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.149 |
|
|
|
| 2 |
C |
0.084 |
|
|
|
| 3 |
S |
-0.135 |
|
|
|
| 4 |
H |
0.200 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.112 |
1.701 |
0.000 |
2.032 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.220 |
2.976 |
0.000 |
| y |
2.976 |
-19.170 |
0.000 |
| z |
0.000 |
0.000 |
-25.058 |
|
| Traceless |
| | x | y | z |
| x |
-2.107 |
2.976 |
0.000 |
| y |
2.976 |
5.469 |
0.000 |
| z |
0.000 |
0.000 |
-3.363 |
|
| Polar |
| 3z2-r2 | -6.725 |
| x2-y2 | -5.051 |
| xy | 2.976 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.231 |
-0.167 |
0.000 |
| y |
-0.167 |
9.177 |
0.000 |
| z |
0.000 |
0.000 |
3.100 |
<r2> (average value of r
2) Å
2
| <r2> |
60.457 |
| (<r2>)1/2 |
7.775 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.612992 |
| Energy at 298.15K | |
| HF Energy | -491.612992 |
| Nuclear repulsion energy | 80.018315 |
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 B3PW91/cc-pVTZ
| 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 |
3911 |
3761 |
699.54 |
|
|
|
| 2 |
Σ |
2175 |
2092 |
738.32 |
|
|
|
| 3 |
Σ |
869 |
836 |
27.77 |
|
|
|
| 4 |
Π |
491 |
472 |
6.49 |
|
|
|
| 4 |
Π |
491 |
472 |
6.49 |
|
|
|
| 5 |
Π |
464i |
446i |
146.57 |
|
|
|
| 5 |
Π |
464i |
446i |
146.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3504.1 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 3369.5 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 B3PW91/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.672 |
| C2 |
0.000 |
0.000 |
-0.496 |
| S3 |
0.000 |
0.000 |
1.084 |
| H4 |
0.000 |
0.000 |
-2.662 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1757 | 2.7562 | 0.9896 |
C2 | 1.1757 | | 1.5806 | 2.1653 | S3 | 2.7562 | 1.5806 | | 3.7459 | H4 | 0.9896 | 2.1653 | 3.7459 | |
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 B3PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.131 |
|
|
|
| 2 |
C |
0.094 |
|
|
|
| 3 |
S |
-0.190 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
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 |
-3.047 |
3.047 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.028 |
0.000 |
0.000 |
| y |
0.000 |
-25.028 |
0.000 |
| z |
0.000 |
0.000 |
-15.748 |
|
| Traceless |
| | x | y | z |
| x |
-4.640 |
0.000 |
0.000 |
| y |
0.000 |
-4.640 |
0.000 |
| z |
0.000 |
0.000 |
9.280 |
|
| Polar |
| 3z2-r2 | 18.560 |
| 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 |
3.080 |
0.000 |
0.000 |
| y |
0.000 |
3.080 |
0.000 |
| z |
0.000 |
0.000 |
8.985 |
<r2> (average value of r
2) Å
2
| <r2> |
60.640 |
| (<r2>)1/2 |
7.787 |