Jump to
S1C2
Energy calculated at B97D3/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.649310 |
| Energy at 298.15K | -491.650073 |
| HF Energy | -491.649310 |
| Nuclear repulsion energy | 79.583941 |
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 B97D3/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' |
3605 |
3554 |
166.91 |
|
|
|
| 2 |
A' |
2002 |
1974 |
589.46 |
|
|
|
| 3 |
A' |
866 |
854 |
0.88 |
|
|
|
| 4 |
A' |
694 |
685 |
323.52 |
|
|
|
| 5 |
A' |
452 |
446 |
45.26 |
|
|
|
| 6 |
A" |
475 |
468 |
3.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4047.2 cm
-1
Scaled (by 0.986) Zero Point Vibrational Energy (zpe) 3990.5 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 B97D3/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.166 |
1.694 |
0.000 |
| C2 |
0.000 |
0.495 |
0.000 |
| S3 |
0.040 |
-1.079 |
0.000 |
| H4 |
0.518 |
2.434 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2102 | 2.7806 | 1.0081 |
C2 | 1.2102 | | 1.5747 | 2.0071 | S3 | 2.7806 | 1.5747 | | 3.5456 | H4 | 1.0081 | 2.0071 | 3.5456 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
173.582 |
|
C2 |
N1 |
H4 |
129.362 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.119 |
|
|
|
| 2 |
C |
0.035 |
|
|
|
| 3 |
S |
-0.106 |
|
|
|
| 4 |
H |
0.190 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.096 |
1.543 |
0.000 |
1.893 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.153 |
2.932 |
0.000 |
| y |
2.932 |
-19.452 |
0.000 |
| z |
0.000 |
0.000 |
-24.983 |
|
| Traceless |
| | x | y | z |
| x |
-1.935 |
2.932 |
0.000 |
| y |
2.932 |
5.116 |
0.000 |
| z |
0.000 |
0.000 |
-3.181 |
|
| Polar |
| 3z2-r2 | -6.362 |
| x2-y2 | -4.701 |
| xy | 2.932 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.279 |
-0.207 |
0.000 |
| y |
-0.207 |
9.303 |
0.000 |
| z |
0.000 |
0.000 |
3.122 |
<r2> (average value of r
2) Å
2
| <r2> |
60.879 |
| (<r2>)1/2 |
7.802 |
Jump to
S1C1
Energy calculated at B97D3/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.643896 |
| Energy at 298.15K | |
| HF Energy | -491.643896 |
| Nuclear repulsion energy | 79.663319 |
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 B97D3/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 |
3861 |
3807 |
630.39 |
|
|
|
| 2 |
Σ |
2118 |
2088 |
645.95 |
|
|
|
| 3 |
Σ |
851 |
839 |
19.87 |
|
|
|
| 4 |
Π |
472 |
465 |
8.36 |
|
|
|
| 4 |
Π |
472 |
465 |
8.36 |
|
|
|
| 5 |
Π |
533i |
525i |
138.83 |
|
|
|
| 5 |
Π |
533i |
525i |
138.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3353.5 cm
-1
Scaled (by 0.986) Zero Point Vibrational Energy (zpe) 3306.6 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 B97D3/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.681 |
| C2 |
0.000 |
0.000 |
-0.497 |
| S3 |
0.000 |
0.000 |
1.089 |
| H4 |
0.000 |
0.000 |
-2.672 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1844 | 2.7695 | 0.9913 |
C2 | 1.1844 | | 1.5851 | 2.1756 | S3 | 2.7695 | 1.5851 | | 3.7607 | H4 | 0.9913 | 2.1756 | 3.7607 | |
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 B97D3/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.104 |
|
|
|
| 2 |
C |
0.052 |
|
|
|
| 3 |
S |
-0.167 |
|
|
|
| 4 |
H |
0.219 |
|
|
|
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 |
-2.933 |
2.933 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.944 |
0.000 |
0.000 |
| y |
0.000 |
-24.944 |
0.000 |
| z |
0.000 |
0.000 |
-15.856 |
|
| Traceless |
| | x | y | z |
| x |
-4.544 |
0.000 |
0.000 |
| y |
0.000 |
-4.544 |
0.000 |
| z |
0.000 |
0.000 |
9.087 |
|
| Polar |
| 3z2-r2 | 18.175 |
| 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 |
3.097 |
0.000 |
0.000 |
| y |
0.000 |
3.097 |
0.000 |
| z |
0.000 |
0.000 |
9.115 |
<r2> (average value of r
2) Å
2
| <r2> |
61.044 |
| (<r2>)1/2 |
7.813 |