Jump to
S1C2
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.700043 |
| Energy at 298.15K | -491.700808 |
| HF Energy | -491.700043 |
| Nuclear repulsion energy | 80.198928 |
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 B1B95/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' |
3723 |
3563 |
261.04 |
|
|
|
| 2 |
A' |
2084 |
1995 |
741.54 |
|
|
|
| 3 |
A' |
894 |
855 |
3.70 |
|
|
|
| 4 |
A' |
628 |
601 |
315.83 |
|
|
|
| 5 |
A' |
462 |
442 |
105.51 |
|
|
|
| 6 |
A" |
499 |
477 |
1.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4143.8 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 3966.0 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 B1B95/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.134 |
1.681 |
0.000 |
| C2 |
0.000 |
0.493 |
0.000 |
| S3 |
0.026 |
-1.072 |
0.000 |
| H4 |
0.523 |
2.436 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1952 | 2.7578 | 1.0011 |
C2 | 1.1952 | | 1.5658 | 2.0118 | S3 | 2.7578 | 1.5658 | | 3.5433 | H4 | 1.0011 | 2.0118 | 3.5433 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.501 |
|
C2 |
N1 |
H4 |
132.503 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.157 |
|
|
|
| 2 |
C |
0.078 |
|
|
|
| 3 |
S |
-0.138 |
|
|
|
| 4 |
H |
0.217 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.112 |
1.721 |
0.000 |
2.049 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.162 |
2.965 |
0.000 |
| y |
2.965 |
-19.104 |
0.000 |
| z |
0.000 |
0.000 |
-25.003 |
|
| Traceless |
| | x | y | z |
| x |
-2.109 |
2.965 |
0.000 |
| y |
2.965 |
5.479 |
0.000 |
| z |
0.000 |
0.000 |
-3.370 |
|
| Polar |
| 3z2-r2 | -6.741 |
| x2-y2 | -5.059 |
| xy | 2.965 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.202 |
-0.142 |
0.000 |
| y |
-0.142 |
9.103 |
0.000 |
| z |
0.000 |
0.000 |
3.077 |
<r2> (average value of r
2) Å
2
| <r2> |
60.192 |
| (<r2>)1/2 |
7.758 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.696746 |
| Energy at 298.15K | |
| HF Energy | -491.696746 |
| Nuclear repulsion energy | 80.216427 |
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 B1B95/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 |
3926 |
3757 |
712.76 |
|
|
|
| 2 |
Σ |
2192 |
2098 |
759.07 |
|
|
|
| 3 |
Σ |
872 |
835 |
30.43 |
|
|
|
| 4 |
Π |
495 |
473 |
5.95 |
|
|
|
| 4 |
Π |
495 |
473 |
5.95 |
|
|
|
| 5 |
Π |
437i |
418i |
146.90 |
|
|
|
| 5 |
Π |
437i |
418i |
146.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3552.9 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 3400.5 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 B1B95/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.668 |
| C2 |
0.000 |
0.000 |
-0.495 |
| S3 |
0.000 |
0.000 |
1.081 |
| H4 |
0.000 |
0.000 |
-2.655 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1724 | 2.7493 | 0.9875 |
C2 | 1.1724 | | 1.5770 | 2.1599 | S3 | 2.7493 | 1.5770 | | 3.7368 | H4 | 0.9875 | 2.1599 | 3.7368 | |
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 B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.142 |
|
|
|
| 2 |
C |
0.093 |
|
|
|
| 3 |
S |
-0.196 |
|
|
|
| 4 |
H |
0.244 |
|
|
|
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 |
-3.052 |
3.052 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.974 |
0.000 |
0.000 |
| y |
0.000 |
-24.974 |
0.000 |
| z |
0.000 |
0.000 |
-15.736 |
|
| Traceless |
| | x | y | z |
| x |
-4.619 |
0.000 |
0.000 |
| y |
0.000 |
-4.619 |
0.000 |
| z |
0.000 |
0.000 |
9.238 |
|
| Polar |
| 3z2-r2 | 18.476 |
| 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 |
3.058 |
0.000 |
0.000 |
| y |
0.000 |
3.058 |
0.000 |
| z |
0.000 |
0.000 |
8.912 |
<r2> (average value of r
2) Å
2
| <r2> |
60.384 |
| (<r2>)1/2 |
7.771 |