Jump to
S1C2
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.708870 |
| Energy at 298.15K | -491.709637 |
| HF Energy | -491.708870 |
| Nuclear repulsion energy | 79.854873 |
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 B3LYP/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' |
3674 |
3551 |
233.31 |
|
|
|
| 2 |
A' |
2047 |
1979 |
702.39 |
|
|
|
| 3 |
A' |
876 |
847 |
2.29 |
|
|
|
| 4 |
A' |
652 |
630 |
341.07 |
|
|
|
| 5 |
A' |
461 |
446 |
76.77 |
|
|
|
| 6 |
A" |
492 |
475 |
2.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4101.1 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 3964.1 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 B3LYP/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.142 |
1.687 |
0.000 |
| C2 |
0.000 |
0.496 |
0.000 |
| S3 |
0.030 |
-1.077 |
0.000 |
| H4 |
0.521 |
2.442 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1996 | 2.7698 | 1.0044 |
C2 | 1.1996 | | 1.5736 | 2.0143 | S3 | 2.7698 | 1.5736 | | 3.5533 | H4 | 1.0044 | 2.0143 | 3.5533 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.276 |
|
C2 |
N1 |
H4 |
131.907 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.139 |
|
|
|
| 2 |
C |
0.054 |
|
|
|
| 3 |
S |
-0.118 |
|
|
|
| 4 |
H |
0.203 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.115 |
1.692 |
0.000 |
2.026 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.390 |
2.980 |
0.000 |
| y |
2.980 |
-19.442 |
0.000 |
| z |
0.000 |
0.000 |
-25.225 |
|
| Traceless |
| | x | y | z |
| x |
-2.056 |
2.980 |
0.000 |
| y |
2.980 |
5.365 |
0.000 |
| z |
0.000 |
0.000 |
-3.309 |
|
| Polar |
| 3z2-r2 | -6.618 |
| x2-y2 | -4.948 |
| xy | 2.980 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.227 |
-0.156 |
0.000 |
| y |
-0.156 |
9.212 |
0.000 |
| z |
0.000 |
0.000 |
3.093 |
<r2> (average value of r
2) Å
2
| <r2> |
60.739 |
| (<r2>)1/2 |
7.794 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.704963 |
| Energy at 298.15K | |
| HF Energy | -491.704963 |
| Nuclear repulsion energy | 79.880696 |
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 B3LYP/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 |
3894 |
3764 |
701.76 |
|
|
|
| 2 |
Σ |
2159 |
2087 |
732.28 |
|
|
|
| 3 |
Σ |
854 |
826 |
28.60 |
|
|
|
| 4 |
Π |
488 |
472 |
6.33 |
|
|
|
| 4 |
Π |
488 |
472 |
6.33 |
|
|
|
| 5 |
Π |
472i |
456i |
147.55 |
|
|
|
| 5 |
Π |
472i |
456i |
147.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3469.8 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 3353.9 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 B3LYP/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.675 |
| C2 |
0.000 |
0.000 |
-0.499 |
| S3 |
0.000 |
0.000 |
1.086 |
| H4 |
0.000 |
0.000 |
-2.664 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1759 | 2.7611 | 0.9897 |
C2 | 1.1759 | | 1.5851 | 2.1656 | S3 | 2.7611 | 1.5851 | | 3.7508 | H4 | 0.9897 | 2.1656 | 3.7508 | |
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 B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.125 |
|
|
|
| 2 |
C |
0.070 |
|
|
|
| 3 |
S |
-0.174 |
|
|
|
| 4 |
H |
0.229 |
|
|
|
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 |
-3.051 |
3.051 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.194 |
0.000 |
0.000 |
| y |
0.000 |
-25.194 |
0.000 |
| z |
0.000 |
0.000 |
-15.999 |
|
| Traceless |
| | x | y | z |
| x |
-4.598 |
0.000 |
0.000 |
| y |
0.000 |
-4.598 |
0.000 |
| z |
0.000 |
0.000 |
9.195 |
|
| Polar |
| 3z2-r2 | 18.390 |
| 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 |
9.005 |
<r2> (average value of r
2) Å
2
| <r2> |
60.928 |
| (<r2>)1/2 |
7.806 |