Jump to
S1C2
Energy calculated at B3LYP/3-21G
| hartrees |
Energy at 0K | -1189.866678 |
Energy at 298.15K | -1189.868647 |
HF Energy | -1189.866678 |
Nuclear repulsion energy | 178.947966 |
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/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 |
2450 |
2364 |
0.05 |
|
|
|
2 |
A |
797 |
769 |
0.06 |
|
|
|
3 |
A |
408 |
394 |
0.99 |
|
|
|
4 |
A |
275 |
265 |
41.91 |
|
|
|
5 |
A |
151 |
146 |
0.03 |
|
|
|
6 |
B |
2451 |
2365 |
38.43 |
|
|
|
7 |
B |
794 |
766 |
2.47 |
|
|
|
8 |
B |
394 |
380 |
24.19 |
|
|
|
9 |
B |
295 |
285 |
26.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4007.6 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 3867.0 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 B3LYP/3-21G
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.954 |
S2 |
0.000 |
1.809 |
-0.438 |
S3 |
0.000 |
-1.809 |
-0.438 |
H4 |
-1.365 |
1.855 |
-0.619 |
H5 |
1.365 |
-1.855 |
-0.619 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.2826 | 2.2826 | 2.7895 | 2.7895 |
S2 | 2.2826 | | 3.6171 | 1.3781 | 3.9143 | S3 | 2.2826 | 3.6171 | | 3.9143 | 1.3781 | H4 | 2.7895 | 1.3781 | 3.9143 | | 4.6075 | H5 | 2.7895 | 3.9143 | 1.3781 | 4.6075 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
96.132 |
|
S1 |
S3 |
H5 |
96.132 |
S2 |
S1 |
S3 |
104.803 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.041 |
|
|
|
2 |
S |
-0.090 |
|
|
|
3 |
S |
-0.090 |
|
|
|
4 |
H |
0.110 |
|
|
|
5 |
H |
0.110 |
|
|
|
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 |
-0.624 |
0.624 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-38.742 |
-5.337 |
0.000 |
y |
-5.337 |
-41.406 |
0.000 |
z |
0.000 |
0.000 |
-42.732 |
|
Traceless |
| x | y | z |
x |
3.327 |
-5.337 |
0.000 |
y |
-5.337 |
-0.669 |
0.000 |
z |
0.000 |
0.000 |
-2.658 |
|
Polar |
3z2-r2 | -5.316 |
x2-y2 | 2.664 |
xy | -5.337 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.152 |
-0.831 |
0.000 |
y |
-0.831 |
12.861 |
0.000 |
z |
0.000 |
0.000 |
5.929 |
<r2> (average value of r
2) Å
2
<r2> |
162.350 |
(<r2>)1/2 |
12.742 |
Jump to
S1C1
Energy calculated at B3LYP/3-21G
| hartrees |
Energy at 0K | -1189.865594 |
Energy at 298.15K | -1189.867521 |
HF Energy | -1189.865594 |
Nuclear repulsion energy | 178.754946 |
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/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' |
2438 |
2352 |
50.84 |
|
|
|
2 |
A' |
796 |
768 |
3.63 |
|
|
|
3 |
A' |
407 |
393 |
0.76 |
|
|
|
4 |
A' |
285 |
275 |
31.35 |
|
|
|
5 |
A' |
152 |
147 |
0.14 |
|
|
|
6 |
A" |
2437 |
2351 |
0.11 |
|
|
|
7 |
A" |
792 |
765 |
0.53 |
|
|
|
8 |
A" |
395 |
381 |
28.41 |
|
|
|
9 |
A" |
252 |
243 |
12.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3976.6 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 3837.0 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 B3LYP/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
-0.055 |
0.946 |
0.000 |
S2 |
-0.055 |
-0.440 |
1.814 |
S3 |
-0.055 |
-0.440 |
-1.814 |
H4 |
1.317 |
-0.532 |
1.932 |
H5 |
1.317 |
-0.532 |
-1.932 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.2828 | 2.2828 | 2.7926 | 2.7926 |
S2 | 2.2828 | | 3.6272 | 1.3797 | 3.9894 | S3 | 2.2828 | 3.6272 | | 3.9894 | 1.3797 | H4 | 2.7926 | 1.3797 | 3.9894 | | 3.8630 | H5 | 2.7926 | 3.9894 | 1.3797 | 3.8630 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
96.233 |
|
S1 |
S3 |
H5 |
96.233 |
S2 |
S1 |
S3 |
105.210 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.041 |
|
|
|
2 |
S |
-0.079 |
|
|
|
3 |
S |
-0.079 |
|
|
|
4 |
H |
0.100 |
|
|
|
5 |
H |
0.100 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.589 |
-0.451 |
0.000 |
2.628 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-39.100 |
-1.666 |
0.000 |
y |
-1.666 |
-42.990 |
0.000 |
z |
0.000 |
0.000 |
-40.867 |
|
Traceless |
| x | y | z |
x |
2.828 |
-1.666 |
0.000 |
y |
-1.666 |
-3.007 |
0.000 |
z |
0.000 |
0.000 |
0.178 |
|
Polar |
3z2-r2 | 0.356 |
x2-y2 | 3.890 |
xy | -1.666 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.141 |
-0.375 |
0.000 |
y |
-0.375 |
5.834 |
0.000 |
z |
0.000 |
0.000 |
13.001 |
<r2> (average value of r
2) Å
2
<r2> |
163.016 |
(<r2>)1/2 |
12.768 |