Jump to
S1C2
Energy calculated at B3LYP/6-311G**
| hartrees |
Energy at 0K | -1195.851935 |
Energy at 298.15K | -1195.854199 |
HF Energy | -1195.851935 |
Nuclear repulsion energy | 191.429359 |
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/6-311G**
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 |
2635 |
2548 |
0.30 |
|
|
|
2 |
A |
859 |
831 |
0.55 |
|
|
|
3 |
A |
451 |
436 |
0.58 |
|
|
|
4 |
A |
318 |
307 |
29.25 |
|
|
|
5 |
A |
196 |
189 |
0.03 |
|
|
|
6 |
B |
2634 |
2546 |
5.95 |
|
|
|
7 |
B |
846 |
818 |
11.25 |
|
|
|
8 |
B |
428 |
414 |
37.25 |
|
|
|
9 |
B |
347 |
335 |
21.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4356.4 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 4211.8 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/6-311G**
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.846 |
S2 |
0.000 |
1.713 |
-0.387 |
S3 |
0.000 |
-1.713 |
-0.387 |
H4 |
-1.335 |
1.813 |
-0.579 |
H5 |
1.335 |
-1.813 |
-0.579 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.1101 | 2.1101 | 2.6648 | 2.6648 |
S2 | 2.1101 | | 3.4251 | 1.3527 | 3.7749 | S3 | 2.1101 | 3.4251 | | 3.7749 | 1.3527 | H4 | 2.6648 | 1.3527 | 3.7749 | | 4.5034 | H5 | 2.6648 | 3.7749 | 1.3527 | 4.5034 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
98.251 |
|
S1 |
S3 |
H5 |
98.251 |
S2 |
S1 |
S3 |
108.503 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.055 |
|
|
|
2 |
S |
-0.065 |
|
|
|
3 |
S |
-0.065 |
|
|
|
4 |
H |
0.092 |
|
|
|
5 |
H |
0.092 |
|
|
|
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 |
-0.718 |
0.718 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-38.184 |
-4.374 |
0.000 |
y |
-4.374 |
-40.807 |
0.000 |
z |
0.000 |
0.000 |
-42.877 |
|
Traceless |
| x | y | z |
x |
3.658 |
-4.374 |
0.000 |
y |
-4.374 |
-0.277 |
0.000 |
z |
0.000 |
0.000 |
-3.382 |
|
Polar |
3z2-r2 | -6.764 |
x2-y2 | 2.623 |
xy | -4.374 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.906 |
-0.536 |
0.000 |
y |
-0.536 |
12.022 |
0.000 |
z |
0.000 |
0.000 |
6.586 |
<r2> (average value of r
2) Å
2
<r2> |
146.271 |
(<r2>)1/2 |
12.094 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G**
| hartrees |
Energy at 0K | -1195.851499 |
Energy at 298.15K | -1195.853750 |
HF Energy | -1195.851499 |
Nuclear repulsion energy | 191.447600 |
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/6-311G**
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' |
2626 |
2539 |
9.87 |
|
|
|
2 |
A' |
860 |
832 |
4.96 |
|
|
|
3 |
A' |
452 |
437 |
0.60 |
|
|
|
4 |
A' |
339 |
328 |
22.23 |
|
|
|
5 |
A' |
196 |
189 |
0.15 |
|
|
|
6 |
A" |
2627 |
2540 |
0.39 |
|
|
|
7 |
A" |
850 |
822 |
7.21 |
|
|
|
8 |
A" |
429 |
414 |
42.62 |
|
|
|
9 |
A" |
311 |
301 |
9.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4344.6 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 4200.4 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/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
-0.054 |
0.844 |
0.000 |
S2 |
-0.054 |
-0.390 |
1.712 |
S3 |
-0.054 |
-0.390 |
-1.712 |
H4 |
1.286 |
-0.518 |
1.857 |
H5 |
1.286 |
-0.518 |
-1.857 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.1098 | 2.1098 | 2.6637 | 2.6637 |
S2 | 2.1098 | | 3.4233 | 1.3531 | 3.8136 | S3 | 2.1098 | 3.4233 | | 3.8136 | 1.3531 | H4 | 2.6637 | 1.3531 | 3.8136 | | 3.7135 | H5 | 2.6637 | 3.8136 | 1.3531 | 3.7135 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
98.191 |
|
S1 |
S3 |
H5 |
98.191 |
S2 |
S1 |
S3 |
108.445 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.058 |
|
|
|
2 |
S |
-0.057 |
|
|
|
3 |
S |
-0.057 |
|
|
|
4 |
H |
0.085 |
|
|
|
5 |
H |
0.085 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.054 |
-0.618 |
0.000 |
2.145 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-38.421 |
-1.512 |
0.000 |
y |
-1.512 |
-43.020 |
0.000 |
z |
0.000 |
0.000 |
-40.525 |
|
Traceless |
| x | y | z |
x |
3.351 |
-1.512 |
0.000 |
y |
-1.512 |
-3.547 |
0.000 |
z |
0.000 |
0.000 |
0.196 |
|
Polar |
3z2-r2 | 0.392 |
x2-y2 | 4.599 |
xy | -1.512 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.886 |
-0.267 |
0.000 |
y |
-0.267 |
6.562 |
0.000 |
z |
0.000 |
0.000 |
12.039 |
<r2> (average value of r
2) Å
2
<r2> |
146.271 |
(<r2>)1/2 |
12.094 |