Jump to
S1C2
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -66.027619 |
Energy at 298.15K | -66.031274 |
HF Energy | -66.027619 |
Nuclear repulsion energy | 27.393629 |
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 HF/LANL2DZ
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' |
3836 |
3452 |
13.43 |
|
|
|
2 |
A' |
2679 |
2411 |
40.07 |
|
|
|
3 |
A' |
1768 |
1591 |
9.98 |
|
|
|
4 |
A' |
1085 |
976 |
7.99 |
|
|
|
5 |
A' |
849 |
764 |
41.45 |
|
|
|
6 |
A' |
434 |
390 |
361.90 |
|
|
|
7 |
A" |
3994 |
3594 |
43.49 |
|
|
|
8 |
A" |
1156 |
1040 |
10.59 |
|
|
|
9 |
A" |
512 |
461 |
65.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8156.2 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 7339.7 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.032 |
1.118 |
0.000 |
S2 |
0.032 |
-0.633 |
0.000 |
H3 |
-1.309 |
-0.829 |
0.000 |
H4 |
0.291 |
1.565 |
0.849 |
H5 |
0.291 |
1.565 |
-0.849 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7515 | 2.3639 | 0.9943 | 0.9943 |
S2 | 1.7515 | | 1.3545 | 2.3709 | 2.3709 | H3 | 2.3639 | 1.3545 | | 3.0022 | 3.0022 | H4 | 0.9943 | 2.3709 | 3.0022 | | 1.6989 | H5 | 0.9943 | 2.3709 | 3.0022 | 1.6989 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
98.308 |
|
S2 |
N1 |
H4 |
116.699 |
S2 |
N1 |
H5 |
116.699 |
|
H4 |
N1 |
H5 |
117.365 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.989 |
|
|
|
2 |
S |
0.177 |
|
|
|
3 |
H |
0.082 |
|
|
|
4 |
H |
0.365 |
|
|
|
5 |
H |
0.365 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.067 |
0.883 |
0.000 |
0.885 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.750 |
3.586 |
0.000 |
y |
3.586 |
-17.815 |
0.000 |
z |
0.000 |
0.000 |
-19.190 |
|
Traceless |
| x | y | z |
x |
-1.248 |
3.586 |
0.000 |
y |
3.586 |
1.655 |
0.000 |
z |
0.000 |
0.000 |
-0.408 |
|
Polar |
3z2-r2 | -0.816 |
x2-y2 | -1.935 |
xy | 3.586 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.730 |
0.596 |
0.000 |
y |
0.596 |
4.221 |
0.000 |
z |
0.000 |
0.000 |
1.429 |
<r2> (average value of r
2) Å
2
<r2> |
31.901 |
(<r2>)1/2 |
5.648 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -66.027619 |
Energy at 298.15K | -66.031271 |
HF Energy | -66.027619 |
Nuclear repulsion energy | 27.395764 |
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 HF/LANL2DZ
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' |
3837 |
3453 |
13.47 |
|
|
|
2 |
A' |
2679 |
2411 |
40.21 |
|
|
|
3 |
A' |
1768 |
1591 |
9.90 |
|
|
|
4 |
A' |
1085 |
977 |
7.91 |
|
|
|
5 |
A' |
849 |
764 |
41.13 |
|
|
|
6 |
A' |
431 |
388 |
363.92 |
|
|
|
7 |
A" |
3995 |
3595 |
43.53 |
|
|
|
8 |
A" |
1155 |
1039 |
10.69 |
|
|
|
9 |
A" |
512 |
461 |
65.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8155.3 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 7339.0 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.032 |
1.118 |
0.000 |
S2 |
0.032 |
-0.633 |
0.000 |
H3 |
-1.309 |
-0.829 |
0.000 |
H4 |
0.290 |
1.566 |
0.849 |
H5 |
0.290 |
1.566 |
-0.849 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7513 | 2.3636 | 0.9942 | 0.9942 |
S2 | 1.7513 | | 1.3545 | 2.3713 | 2.3713 | H3 | 2.3636 | 1.3545 | | 3.0018 | 3.0018 | H4 | 0.9942 | 2.3713 | 3.0018 | | 1.6987 | H5 | 0.9942 | 2.3713 | 3.0018 | 1.6987 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
98.303 |
|
S2 |
N1 |
H4 |
116.755 |
S2 |
N1 |
H5 |
116.755 |
|
H4 |
N1 |
H5 |
117.356 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.989 |
|
|
|
2 |
S |
0.177 |
|
|
|
3 |
H |
0.082 |
|
|
|
4 |
H |
0.365 |
|
|
|
5 |
H |
0.365 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.072 |
0.885 |
0.000 |
0.888 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.754 |
3.575 |
0.000 |
y |
3.575 |
-17.805 |
0.000 |
z |
0.000 |
0.000 |
-19.190 |
|
Traceless |
| x | y | z |
x |
-1.257 |
3.575 |
0.000 |
y |
3.575 |
1.668 |
0.000 |
z |
0.000 |
0.000 |
-0.410 |
|
Polar |
3z2-r2 | -0.821 |
x2-y2 | -1.950 |
xy | 3.575 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.730 |
0.595 |
0.000 |
y |
0.595 |
4.219 |
0.000 |
z |
0.000 |
0.000 |
1.429 |
<r2> (average value of r
2) Å
2
<r2> |
31.898 |
(<r2>)1/2 |
5.648 |