Jump to
S1C2
Energy calculated at B97D3/6-31G
| | hartrees |
| Energy at 0K | -491.522051 |
| Energy at 298.15K | -491.522587 |
| HF Energy | -491.522051 |
| Nuclear repulsion energy | 77.828746 |
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 B97D3/6-31G
| 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' |
3737 |
3737 |
303.36 |
|
|
|
| 2 |
A' |
2061 |
2061 |
473.34 |
|
|
|
| 3 |
A' |
788 |
788 |
5.62 |
|
|
|
| 4 |
A' |
500 |
500 |
355.95 |
|
|
|
| 5 |
A' |
417 |
417 |
25.33 |
|
|
|
| 6 |
A" |
424 |
424 |
7.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3962.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3962.9 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 B97D3/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.160 |
1.720 |
0.000 |
| C2 |
0.000 |
0.521 |
0.000 |
| S3 |
0.051 |
-1.111 |
0.000 |
| H4 |
0.302 |
2.611 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2100 | 2.8388 | 1.0039 |
C2 | 1.2100 | | 1.6324 | 2.1124 | S3 | 2.8388 | 1.6324 | | 3.7307 | H4 | 1.0039 | 2.1124 | 3.7307 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.200 |
|
C2 |
N1 |
H4 |
145.007 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.514 |
|
|
|
| 2 |
C |
0.049 |
|
|
|
| 3 |
S |
0.106 |
|
|
|
| 4 |
H |
0.359 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.983 |
2.809 |
0.000 |
2.976 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.767 |
2.622 |
0.000 |
| y |
2.622 |
-17.936 |
0.000 |
| z |
0.000 |
0.000 |
-25.011 |
|
| Traceless |
| | x | y | z |
| x |
-3.294 |
2.622 |
0.000 |
| y |
2.622 |
6.953 |
0.000 |
| z |
0.000 |
0.000 |
-3.659 |
|
| Polar |
| 3z2-r2 | -7.319 |
| x2-y2 | -6.831 |
| xy | 2.622 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.118 |
-0.402 |
0.000 |
| y |
-0.402 |
8.901 |
0.000 |
| z |
0.000 |
0.000 |
1.971 |
<r2> (average value of r
2) Å
2
| <r2> |
63.312 |
| (<r2>)1/2 |
7.957 |
Jump to
S1C1
Energy calculated at B97D3/6-31G
| | hartrees |
| Energy at 0K | -491.520763 |
| Energy at 298.15K | |
| HF Energy | -491.520763 |
| Nuclear repulsion energy | 77.882544 |
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 B97D3/6-31G
| 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 |
3888 |
3888 |
597.02 |
|
|
|
| 2 |
Σ |
2123 |
2123 |
493.57 |
|
|
|
| 3 |
Σ |
775 |
775 |
17.45 |
|
|
|
| 4 |
Π |
421 |
421 |
6.58 |
|
|
|
| 4 |
Π |
421 |
421 |
6.58 |
|
|
|
| 5 |
Π |
365i |
365i |
231.38 |
|
|
|
| 5 |
Π |
365i |
365i |
231.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3448.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3448.3 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 B97D3/6-31G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.718 |
| C2 |
0.000 |
0.000 |
-0.522 |
| S3 |
0.000 |
0.000 |
1.117 |
| H4 |
0.000 |
0.000 |
-2.712 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1959 | 2.8346 | 0.9937 |
C2 | 1.1959 | | 1.6387 | 2.1897 | S3 | 2.8346 | 1.6387 | | 3.8284 | H4 | 0.9937 | 2.1897 | 3.8284 | |
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 B97D3/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.528 |
|
|
|
| 2 |
C |
0.071 |
|
|
|
| 3 |
S |
0.083 |
|
|
|
| 4 |
H |
0.374 |
|
|
|
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 |
-3.485 |
3.485 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.980 |
0.000 |
0.000 |
| y |
0.000 |
-24.980 |
0.000 |
| z |
0.000 |
0.000 |
-16.205 |
|
| Traceless |
| | x | y | z |
| x |
-4.388 |
0.000 |
0.000 |
| y |
0.000 |
-4.388 |
0.000 |
| z |
0.000 |
0.000 |
8.776 |
|
| Polar |
| 3z2-r2 | 17.551 |
| 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 |
1.968 |
0.000 |
0.000 |
| y |
0.000 |
1.968 |
0.000 |
| z |
0.000 |
0.000 |
8.715 |
<r2> (average value of r
2) Å
2
| <r2> |
63.375 |
| (<r2>)1/2 |
7.961 |