Jump to
S1C2
Energy calculated at mPW1PW91/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.680893 |
| Energy at 298.15K | -491.681667 |
| HF Energy | -491.680893 |
| Nuclear repulsion energy | 80.106755 |
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 mPW1PW91/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' |
3721 |
3570 |
253.11 |
|
|
|
| 2 |
A' |
2081 |
1996 |
737.86 |
|
|
|
| 3 |
A' |
895 |
858 |
3.30 |
|
|
|
| 4 |
A' |
640 |
614 |
325.57 |
|
|
|
| 5 |
A' |
464 |
445 |
96.52 |
|
|
|
| 6 |
A" |
499 |
479 |
1.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4150.1 cm
-1
Scaled (by 0.9592) Zero Point Vibrational Energy (zpe) 3980.8 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 mPW1PW91/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.137 |
1.683 |
0.000 |
| C2 |
0.000 |
0.494 |
0.000 |
| S3 |
0.027 |
-1.074 |
0.000 |
| H4 |
0.526 |
2.434 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1967 | 2.7612 | 1.0023 |
C2 | 1.1967 | | 1.5677 | 2.0101 | S3 | 2.7612 | 1.5677 | | 3.5428 | H4 | 1.0023 | 2.0101 | 3.5428 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.407 |
|
C2 |
N1 |
H4 |
131.958 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.145 |
|
|
|
| 2 |
C |
0.088 |
|
|
|
| 3 |
S |
-0.141 |
|
|
|
| 4 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.121 |
1.718 |
0.000 |
2.052 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.204 |
2.996 |
0.000 |
| y |
2.996 |
-19.168 |
0.000 |
| z |
0.000 |
0.000 |
-25.062 |
|
| Traceless |
| | x | y | z |
| x |
-2.089 |
2.996 |
0.000 |
| y |
2.996 |
5.465 |
0.000 |
| z |
0.000 |
0.000 |
-3.377 |
|
| Polar |
| 3z2-r2 | -6.753 |
| x2-y2 | -5.036 |
| xy | 2.996 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.222 |
-0.150 |
0.000 |
| y |
-0.150 |
9.126 |
0.000 |
| z |
0.000 |
0.000 |
3.094 |
<r2> (average value of r
2) Å
2
| <r2> |
60.317 |
| (<r2>)1/2 |
7.766 |
Jump to
S1C1
Energy calculated at mPW1PW91/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.677323 |
| Energy at 298.15K | |
| HF Energy | -491.677323 |
| Nuclear repulsion energy | 80.134410 |
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 mPW1PW91/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 |
3932 |
3771 |
713.10 |
|
|
|
| 2 |
Σ |
2192 |
2102 |
760.36 |
|
|
|
| 3 |
Σ |
875 |
839 |
29.89 |
|
|
|
| 4 |
Π |
495 |
475 |
6.13 |
|
|
|
| 4 |
Π |
495 |
475 |
6.13 |
|
|
|
| 5 |
Π |
451i |
433i |
147.80 |
|
|
|
| 5 |
Π |
451i |
433i |
147.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3543.2 cm
-1
Scaled (by 0.9592) Zero Point Vibrational Energy (zpe) 3398.7 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 mPW1PW91/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.670 |
| C2 |
0.000 |
0.000 |
-0.496 |
| S3 |
0.000 |
0.000 |
1.083 |
| H4 |
0.000 |
0.000 |
-2.658 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1732 | 2.7521 | 0.9882 |
C2 | 1.1732 | | 1.5789 | 2.1614 | S3 | 2.7521 | 1.5789 | | 3.7404 | H4 | 0.9882 | 2.1614 | 3.7404 | |
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 mPW1PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.125 |
|
|
|
| 2 |
C |
0.098 |
|
|
|
| 3 |
S |
-0.197 |
|
|
|
| 4 |
H |
0.224 |
|
|
|
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 |
-3.078 |
3.078 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.032 |
0.000 |
0.000 |
| y |
0.000 |
-25.032 |
0.000 |
| z |
0.000 |
0.000 |
-15.720 |
|
| Traceless |
| | x | y | z |
| x |
-4.656 |
0.000 |
0.000 |
| y |
0.000 |
-4.656 |
0.000 |
| z |
0.000 |
0.000 |
9.313 |
|
| Polar |
| 3z2-r2 | 18.625 |
| 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 |
3.074 |
0.000 |
0.000 |
| y |
0.000 |
3.074 |
0.000 |
| z |
0.000 |
0.000 |
8.930 |
<r2> (average value of r
2) Å
2
| <r2> |
60.502 |
| (<r2>)1/2 |
7.778 |