Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G**
| hartrees |
Energy at 0K | -454.564573 |
Energy at 298.15K | -454.568361 |
HF Energy | -454.564573 |
Nuclear repulsion energy | 57.734658 |
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 HSEh1PBE/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' |
3560 |
3419 |
6.77 |
|
|
|
2 |
A' |
2664 |
2559 |
19.40 |
|
|
|
3 |
A' |
1646 |
1581 |
15.79 |
|
|
|
4 |
A' |
1044 |
1002 |
10.41 |
|
|
|
5 |
A' |
887 |
852 |
46.69 |
|
|
|
6 |
A' |
637 |
612 |
93.03 |
|
|
|
7 |
A" |
3657 |
3512 |
21.39 |
|
|
|
8 |
A" |
1147 |
1102 |
5.31 |
|
|
|
9 |
A" |
482 |
463 |
67.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7861.8 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 7550.5 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 HSEh1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.016 |
1.105 |
0.000 |
S2 |
0.016 |
-0.616 |
0.000 |
H3 |
-1.323 |
-0.795 |
0.000 |
H4 |
0.481 |
1.456 |
0.826 |
H5 |
0.481 |
1.456 |
-0.826 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7211 | 2.3243 | 1.0106 | 1.0106 |
S2 | 1.7211 | | 1.3510 | 2.2780 | 2.2780 | H3 | 2.3243 | 1.3510 | | 3.0001 | 3.0001 | H4 | 1.0106 | 2.2780 | 3.0001 | | 1.6521 | H5 | 1.0106 | 2.2780 | 3.0001 | 1.6521 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
97.604 |
|
S2 |
N1 |
H4 |
110.283 |
S2 |
N1 |
H5 |
110.283 |
|
H4 |
N1 |
H5 |
109.643 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.622 |
|
|
|
2 |
S |
0.029 |
|
|
|
3 |
H |
0.091 |
|
|
|
4 |
H |
0.251 |
|
|
|
5 |
H |
0.251 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.509 |
0.986 |
0.000 |
1.110 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.271 |
3.699 |
0.000 |
y |
3.699 |
-19.030 |
0.000 |
z |
0.000 |
0.000 |
-20.537 |
|
Traceless |
| x | y | z |
x |
0.512 |
3.699 |
0.000 |
y |
3.699 |
0.874 |
0.000 |
z |
0.000 |
0.000 |
-1.386 |
|
Polar |
3z2-r2 | -2.772 |
x2-y2 | -0.241 |
xy | 3.699 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.366 |
0.454 |
0.000 |
y |
0.454 |
4.344 |
0.000 |
z |
0.000 |
0.000 |
2.657 |
<r2> (average value of r
2) Å
2
<r2> |
35.321 |
(<r2>)1/2 |
5.943 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G**
| hartrees |
Energy at 0K | -454.563636 |
Energy at 298.15K | -454.567459 |
HF Energy | -454.563636 |
Nuclear repulsion energy | 58.037719 |
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 HSEh1PBE/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' |
3563 |
3422 |
3.17 |
|
|
|
2 |
A' |
2561 |
2459 |
64.36 |
|
|
|
3 |
A' |
1628 |
1563 |
8.50 |
|
|
|
4 |
A' |
1023 |
982 |
39.35 |
|
|
|
5 |
A' |
883 |
848 |
19.73 |
|
|
|
6 |
A' |
597 |
573 |
173.57 |
|
|
|
7 |
A" |
3670 |
3524 |
22.02 |
|
|
|
8 |
A" |
1129 |
1084 |
7.02 |
|
|
|
9 |
A" |
573 |
550 |
3.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7812.2 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 7502.8 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 HSEh1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.081 |
1.092 |
0.000 |
S2 |
0.081 |
-0.607 |
0.000 |
H3 |
-1.245 |
-0.921 |
0.000 |
H4 |
-0.315 |
1.500 |
0.834 |
H5 |
-0.315 |
1.500 |
-0.834 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.6990 | 2.4103 | 1.0096 | 1.0096 |
S2 | 1.6990 | | 1.3628 | 2.3008 | 2.3008 | H3 | 2.4103 | 1.3628 | | 2.7244 | 2.7244 | H4 | 1.0096 | 2.3008 | 2.7244 | | 1.6681 | H5 | 1.0096 | 2.3008 | 2.7244 | 1.6681 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
103.307 |
|
S2 |
N1 |
H4 |
113.860 |
S2 |
N1 |
H5 |
113.860 |
|
H4 |
N1 |
H5 |
111.397 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.616 |
|
|
|
2 |
S |
0.075 |
|
|
|
3 |
H |
0.045 |
|
|
|
4 |
H |
0.248 |
|
|
|
5 |
H |
0.248 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.203 |
1.156 |
0.000 |
2.487 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.293 |
-1.002 |
0.000 |
y |
-1.002 |
-18.226 |
0.000 |
z |
0.000 |
0.000 |
-20.428 |
|
Traceless |
| x | y | z |
x |
-0.965 |
-1.002 |
0.000 |
y |
-1.002 |
2.134 |
0.000 |
z |
0.000 |
0.000 |
-1.169 |
|
Polar |
3z2-r2 | -2.338 |
x2-y2 | -2.066 |
xy | -1.002 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.359 |
0.277 |
0.000 |
y |
0.277 |
4.312 |
0.000 |
z |
0.000 |
0.000 |
2.656 |
<r2> (average value of r
2) Å
2
<r2> |
35.156 |
(<r2>)1/2 |
5.929 |