Jump to
S1C2
Energy calculated at BLYP/3-21G
| | hartrees |
| Energy at 0K | -489.118212 |
| Energy at 298.15K | -489.118791 |
| HF Energy | -489.118212 |
| Nuclear repulsion energy | 77.782794 |
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 BLYP/3-21G
| 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' |
3609 |
3589 |
336.84 |
|
|
|
| 2 |
A' |
2091 |
2079 |
398.77 |
|
|
|
| 3 |
A' |
781 |
777 |
6.04 |
|
|
|
| 4 |
A' |
501 |
498 |
14.42 |
|
|
|
| 5 |
A' |
387 |
385 |
342.81 |
|
|
|
| 6 |
A" |
507 |
504 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3937.1 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 3915.5 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 BLYP/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.068 |
1.724 |
0.000 |
| C2 |
0.000 |
0.525 |
0.000 |
| S3 |
0.003 |
-1.114 |
0.000 |
| H4 |
0.424 |
2.608 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2008 | 2.8394 | 1.0115 |
C2 | 1.2008 | | 1.6396 | 2.1253 | S3 | 2.8394 | 1.6396 | | 3.7458 | H4 | 1.0115 | 2.1253 | 3.7458 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
176.867 |
|
C2 |
N1 |
H4 |
147.637 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.662 |
|
|
|
| 2 |
C |
0.084 |
|
|
|
| 3 |
S |
0.236 |
|
|
|
| 4 |
H |
0.341 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.996 |
3.194 |
0.000 |
3.346 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.646 |
2.650 |
0.000 |
| y |
2.650 |
-17.718 |
0.000 |
| z |
0.000 |
0.000 |
-25.142 |
|
| Traceless |
| | x | y | z |
| x |
-3.216 |
2.650 |
0.000 |
| y |
2.650 |
7.176 |
0.000 |
| z |
0.000 |
0.000 |
-3.960 |
|
| Polar |
| 3z2-r2 | -7.920 |
| x2-y2 | -6.928 |
| xy | 2.650 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.815 |
-0.024 |
0.000 |
| y |
-0.024 |
8.342 |
0.000 |
| z |
0.000 |
0.000 |
1.706 |
<r2> (average value of r
2) Å
2
| <r2> |
63.399 |
| (<r2>)1/2 |
7.962 |
Jump to
S1C1
Energy calculated at BLYP/3-21G
| | hartrees |
| Energy at 0K | -489.117598 |
| Energy at 298.15K | |
| HF Energy | -489.117598 |
| Nuclear repulsion energy | 77.792017 |
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 BLYP/3-21G
| 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 |
3739 |
3718 |
616.45 |
|
|
|
| 2 |
Σ |
2142 |
2130 |
396.53 |
|
|
|
| 3 |
Σ |
771 |
767 |
16.86 |
|
|
|
| 4 |
Π |
513 |
510 |
0.03 |
|
|
|
| 4 |
Π |
513 |
510 |
0.03 |
|
|
|
| 5 |
Π |
258i |
257i |
209.33 |
|
|
|
| 5 |
Π |
258i |
257i |
209.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3580.8 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 3561.1 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 BLYP/3-21G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.717 |
| C2 |
0.000 |
0.000 |
-0.527 |
| S3 |
0.000 |
0.000 |
1.119 |
| H4 |
0.000 |
0.000 |
-2.718 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1906 | 2.8361 | 1.0011 |
C2 | 1.1906 | | 1.6456 | 2.1916 | S3 | 2.8361 | 1.6456 | | 3.8372 | H4 | 1.0011 | 2.1916 | 3.8372 | |
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 BLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.703 |
|
|
|
| 2 |
C |
0.136 |
|
|
|
| 3 |
S |
0.211 |
|
|
|
| 4 |
H |
0.355 |
|
|
|
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 |
-3.863 |
3.863 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.111 |
0.000 |
0.000 |
| y |
0.000 |
-25.111 |
0.000 |
| z |
0.000 |
0.000 |
-15.822 |
|
| Traceless |
| | x | y | z |
| x |
-4.644 |
0.000 |
0.000 |
| y |
0.000 |
-4.644 |
0.000 |
| z |
0.000 |
0.000 |
9.289 |
|
| Polar |
| 3z2-r2 | 18.578 |
| 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 |
1.704 |
0.000 |
0.000 |
| y |
0.000 |
1.704 |
0.000 |
| z |
0.000 |
0.000 |
8.128 |
<r2> (average value of r
2) Å
2
| <r2> |
63.477 |
| (<r2>)1/2 |
7.967 |