Jump to
S1C2
Energy calculated at B2PLYP/aug-cc-pVDZ
| hartrees |
Energy at 0K | -454.545705 |
Energy at 298.15K | -454.549425 |
HF Energy | -454.434673 |
Nuclear repulsion energy | 56.883504 |
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 B2PLYP/aug-cc-pVDZ
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' |
3505 |
3505 |
5.51 |
|
|
|
2 |
A' |
2672 |
2672 |
7.94 |
|
|
|
3 |
A' |
1606 |
1606 |
12.23 |
|
|
|
4 |
A' |
1025 |
1025 |
10.87 |
|
|
|
5 |
A' |
884 |
884 |
44.59 |
|
|
|
6 |
A' |
658 |
658 |
48.58 |
|
|
|
7 |
A" |
3604 |
3604 |
21.17 |
|
|
|
8 |
A" |
1126 |
1126 |
0.45 |
|
|
|
9 |
A" |
397 |
397 |
48.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7738.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7738.2 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 B2PLYP/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.013 |
1.130 |
0.000 |
S2 |
0.013 |
-0.628 |
0.000 |
H3 |
-1.334 |
-0.776 |
0.000 |
H4 |
0.514 |
1.455 |
0.824 |
H5 |
0.514 |
1.455 |
-0.824 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7578 | 2.3343 | 1.0175 | 1.0175 |
S2 | 1.7578 | | 1.3553 | 2.2951 | 2.2951 | H3 | 2.3343 | 1.3553 | | 3.0123 | 3.0123 | H4 | 1.0175 | 2.2951 | 3.0123 | | 1.6475 | H5 | 1.0175 | 2.2951 | 3.0123 | 1.6475 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
96.298 |
|
S2 |
N1 |
H4 |
108.628 |
S2 |
N1 |
H5 |
108.628 |
|
H4 |
N1 |
H5 |
108.109 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.349 |
|
|
|
2 |
S |
0.292 |
|
|
|
3 |
H |
0.052 |
|
|
|
4 |
H |
0.003 |
|
|
|
5 |
H |
0.003 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.544 |
0.798 |
0.000 |
0.966 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.587 |
3.570 |
0.000 |
y |
3.570 |
-19.727 |
0.000 |
z |
0.000 |
0.000 |
-20.816 |
|
Traceless |
| x | y | z |
x |
0.685 |
3.570 |
0.000 |
y |
3.570 |
0.474 |
0.000 |
z |
0.000 |
0.000 |
-1.159 |
|
Polar |
3z2-r2 | -2.317 |
x2-y2 | 0.141 |
xy | 3.570 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.537 |
0.295 |
0.000 |
y |
0.295 |
5.820 |
0.000 |
z |
0.000 |
0.000 |
4.398 |
<r2> (average value of r
2) Å
2
<r2> |
36.269 |
(<r2>)1/2 |
6.022 |
Jump to
S1C1
Energy calculated at B2PLYP/aug-cc-pVDZ
| hartrees |
Energy at 0K | -454.544961 |
Energy at 298.15K | -454.548735 |
HF Energy | -454.434269 |
Nuclear repulsion energy | 57.081169 |
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 B2PLYP/aug-cc-pVDZ
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' |
3508 |
3508 |
2.25 |
|
|
|
2 |
A' |
2603 |
2603 |
28.94 |
|
|
|
3 |
A' |
1594 |
1594 |
13.11 |
|
|
|
4 |
A' |
1002 |
1002 |
22.96 |
|
|
|
5 |
A' |
871 |
871 |
25.81 |
|
|
|
6 |
A' |
635 |
635 |
83.29 |
|
|
|
7 |
A" |
3618 |
3618 |
21.15 |
|
|
|
8 |
A" |
1112 |
1112 |
0.68 |
|
|
|
9 |
A" |
483 |
483 |
2.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7711.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7711.9 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 B2PLYP/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.086 |
1.122 |
0.000 |
S2 |
0.086 |
-0.620 |
0.000 |
H3 |
-1.247 |
-0.907 |
0.000 |
H4 |
-0.369 |
1.491 |
0.830 |
H5 |
-0.369 |
1.491 |
-0.830 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7418 | 2.4275 | 1.0165 | 1.0165 |
S2 | 1.7418 | | 1.3635 | 2.3139 | 2.3139 | H3 | 2.4275 | 1.3635 | | 2.6853 | 2.6853 | H4 | 1.0165 | 2.3139 | 2.6853 | | 1.6606 | H5 | 1.0165 | 2.3139 | 2.6853 | 1.6606 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
102.148 |
|
S2 |
N1 |
H4 |
111.311 |
S2 |
N1 |
H5 |
111.311 |
|
H4 |
N1 |
H5 |
109.540 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.315 |
|
|
|
2 |
S |
0.341 |
|
|
|
3 |
H |
-0.007 |
|
|
|
4 |
H |
-0.010 |
|
|
|
5 |
H |
-0.010 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.019 |
0.888 |
0.000 |
2.205 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.442 |
-1.298 |
0.000 |
y |
-1.298 |
-19.024 |
0.000 |
z |
0.000 |
0.000 |
-20.747 |
|
Traceless |
| x | y | z |
x |
-0.556 |
-1.298 |
0.000 |
y |
-1.298 |
1.571 |
0.000 |
z |
0.000 |
0.000 |
-1.015 |
|
Polar |
3z2-r2 | -2.029 |
x2-y2 | -1.418 |
xy | -1.298 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.558 |
0.226 |
0.000 |
y |
0.226 |
5.736 |
0.000 |
z |
0.000 |
0.000 |
4.392 |
<r2> (average value of r
2) Å
2
<r2> |
36.143 |
(<r2>)1/2 |
6.012 |