Jump to
S1C2
Energy calculated at wB97X-D/6-311G**
| hartrees |
Energy at 0K | -454.728985 |
Energy at 298.15K | -454.732780 |
HF Energy | -454.728985 |
Nuclear repulsion energy | 57.808164 |
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 wB97X-D/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' |
3572 |
3417 |
6.64 |
|
|
|
2 |
A' |
2723 |
2605 |
21.28 |
|
|
|
3 |
A' |
1653 |
1581 |
16.01 |
|
|
|
4 |
A' |
1059 |
1013 |
9.97 |
|
|
|
5 |
A' |
885 |
847 |
42.98 |
|
|
|
6 |
A' |
642 |
614 |
106.93 |
|
|
|
7 |
A" |
3670 |
3510 |
20.56 |
|
|
|
8 |
A" |
1153 |
1102 |
5.33 |
|
|
|
9 |
A" |
483 |
462 |
66.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7920.0 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 7575.5 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 wB97X-D/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.016 |
1.103 |
0.000 |
S2 |
0.016 |
-0.615 |
0.000 |
H3 |
-1.319 |
-0.796 |
0.000 |
H4 |
0.472 |
1.460 |
0.827 |
H5 |
0.472 |
1.460 |
-0.827 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7181 | 2.3215 | 1.0100 | 1.0100 |
S2 | 1.7181 | | 1.3477 | 2.2803 | 2.2803 | H3 | 2.3215 | 1.3477 | | 2.9974 | 2.9974 | H4 | 1.0100 | 2.2803 | 2.9974 | | 1.6548 | H5 | 1.0100 | 2.2803 | 2.9974 | 1.6548 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
97.711 |
|
S2 |
N1 |
H4 |
110.720 |
S2 |
N1 |
H5 |
110.720 |
|
H4 |
N1 |
H5 |
110.011 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.629 |
|
|
|
2 |
S |
0.043 |
|
|
|
3 |
H |
0.081 |
|
|
|
4 |
H |
0.253 |
|
|
|
5 |
H |
0.253 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.492 |
0.968 |
0.000 |
1.086 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.238 |
3.696 |
0.000 |
y |
3.696 |
-18.909 |
0.000 |
z |
0.000 |
0.000 |
-20.410 |
|
Traceless |
| x | y | z |
x |
0.422 |
3.696 |
0.000 |
y |
3.696 |
0.915 |
0.000 |
z |
0.000 |
0.000 |
-1.337 |
|
Polar |
3z2-r2 | -2.673 |
x2-y2 | -0.329 |
xy | 3.696 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.334 |
0.457 |
0.000 |
y |
0.457 |
4.291 |
0.000 |
z |
0.000 |
0.000 |
2.641 |
<r2> (average value of r
2) Å
2
<r2> |
35.221 |
(<r2>)1/2 |
5.935 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| hartrees |
Energy at 0K | -454.728105 |
Energy at 298.15K | -454.731936 |
HF Energy | -454.728105 |
Nuclear repulsion energy | |
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 wB97X-D/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' |
3576 |
3421 |
3.35 |
|
|
|
2 |
A' |
2586 |
2474 |
60.52 |
|
|
|
3 |
A' |
1636 |
1565 |
8.55 |
|
|
|
4 |
A' |
1039 |
994 |
38.98 |
|
|
|
5 |
A' |
888 |
849 |
19.24 |
|
|
|
6 |
A' |
610 |
584 |
177.24 |
|
|
|
7 |
A" |
3682 |
3522 |
20.81 |
|
|
|
8 |
A" |
1138 |
1088 |
6.50 |
|
|
|
9 |
A" |
563 |
539 |
3.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7859.9 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 7518.0 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 wB97X-D/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.081 |
1.091 |
0.000 |
S2 |
0.081 |
-0.608 |
0.000 |
H3 |
-1.242 |
-0.912 |
0.000 |
H4 |
-0.313 |
1.500 |
0.834 |
H5 |
-0.313 |
1.500 |
-0.834 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.6995 | 2.4008 | 1.0090 | 1.0090 |
S2 | 1.6995 | | 1.3577 | 2.3013 | 2.3013 | H3 | 2.4008 | 1.3577 | | 2.7159 | 2.7159 | H4 | 1.0090 | 2.3013 | 2.7159 | | 1.6682 | H5 | 1.0090 | 2.3013 | 2.7159 | 1.6682 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
102.921 |
|
S2 |
N1 |
H4 |
113.894 |
S2 |
N1 |
H5 |
113.894 |
|
H4 |
N1 |
H5 |
111.508 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.623 |
|
|
|
2 |
S |
0.088 |
|
|
|
3 |
H |
0.036 |
|
|
|
4 |
H |
0.250 |
|
|
|
5 |
H |
0.250 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.218 |
1.117 |
0.000 |
2.483 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.203 |
-1.010 |
0.000 |
y |
-1.010 |
-18.183 |
0.000 |
z |
0.000 |
0.000 |
-20.317 |
|
Traceless |
| x | y | z |
x |
-0.953 |
-1.010 |
0.000 |
y |
-1.010 |
2.077 |
0.000 |
z |
0.000 |
0.000 |
-1.124 |
|
Polar |
3z2-r2 | -2.247 |
x2-y2 | -2.020 |
xy | -1.010 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.321 |
0.256 |
0.000 |
y |
0.256 |
4.247 |
0.000 |
z |
0.000 |
0.000 |
2.644 |
<r2> (average value of r
2) Å
2
<r2> |
35.091 |
(<r2>)1/2 |
5.924 |