Jump to
S1C2
Energy calculated at PBE1PBE/STO-3G
| hartrees |
Energy at 0K | -449.374124 |
Energy at 298.15K | -449.377714 |
HF Energy | -449.374124 |
Nuclear repulsion energy | 55.998167 |
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 PBE1PBE/STO-3G
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 |
3092 |
12.87 |
|
|
|
2 |
A' |
2992 |
2639 |
20.02 |
|
|
|
3 |
A' |
1868 |
1648 |
2.85 |
|
|
|
4 |
A' |
1183 |
1043 |
25.16 |
|
|
|
5 |
A' |
1046 |
923 |
14.17 |
|
|
|
6 |
A' |
815 |
719 |
7.72 |
|
|
|
7 |
A" |
3694 |
3259 |
16.42 |
|
|
|
8 |
A" |
1279 |
1128 |
2.22 |
|
|
|
9 |
A" |
267 |
235 |
65.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8324.9 cm
-1
Scaled (by 0.8821) Zero Point Vibrational Energy (zpe) 7343.4 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 PBE1PBE/STO-3G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.004 |
1.153 |
0.000 |
S2 |
0.004 |
-0.636 |
0.000 |
H3 |
-1.353 |
-0.725 |
0.000 |
H4 |
0.628 |
1.415 |
0.818 |
H5 |
0.628 |
1.415 |
-0.818 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7886 | 2.3167 | 1.0610 | 1.0610 |
S2 | 1.7886 | | 1.3599 | 2.2940 | 2.2940 | H3 | 2.3167 | 1.3599 | | 3.0280 | 3.0280 | H4 | 1.0610 | 2.2940 | 3.0280 | | 1.6353 | H5 | 1.0610 | 2.2940 | 3.0280 | 1.6353 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
93.757 |
|
S2 |
N1 |
H4 |
104.299 |
S2 |
N1 |
H5 |
104.299 |
|
H4 |
N1 |
H5 |
100.821 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.424 |
|
|
|
2 |
S |
0.118 |
|
|
|
3 |
H |
-0.004 |
|
|
|
4 |
H |
0.155 |
|
|
|
5 |
H |
0.155 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.929 |
0.022 |
0.000 |
0.929 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.557 |
3.233 |
0.000 |
y |
3.233 |
-18.207 |
0.000 |
z |
0.000 |
0.000 |
-17.476 |
|
Traceless |
| x | y | z |
x |
1.284 |
3.233 |
0.000 |
y |
3.233 |
-1.190 |
0.000 |
z |
0.000 |
0.000 |
-0.094 |
|
Polar |
3z2-r2 | -0.189 |
x2-y2 | 1.649 |
xy | 3.233 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.656 |
0.696 |
0.000 |
y |
0.696 |
2.347 |
0.000 |
z |
0.000 |
0.000 |
0.925 |
<r2> (average value of r
2) Å
2
<r2> |
35.132 |
(<r2>)1/2 |
5.927 |
Jump to
S1C1
Energy calculated at PBE1PBE/STO-3G
| hartrees |
Energy at 0K | -449.368821 |
Energy at 298.15K | -449.372521 |
HF Energy | -449.368821 |
Nuclear repulsion energy | 56.176421 |
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 PBE1PBE/STO-3G
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' |
3510 |
3096 |
10.47 |
|
|
|
2 |
A' |
2922 |
2578 |
58.18 |
|
|
|
3 |
A' |
1849 |
1631 |
12.68 |
|
|
|
4 |
A' |
1171 |
1033 |
27.97 |
|
|
|
5 |
A' |
1002 |
884 |
16.13 |
|
|
|
6 |
A' |
731 |
645 |
24.76 |
|
|
|
7 |
A" |
3714 |
3276 |
17.44 |
|
|
|
8 |
A" |
1264 |
1115 |
2.62 |
|
|
|
9 |
A" |
412 |
363 |
9.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8287.4 cm
-1
Scaled (by 0.8821) Zero Point Vibrational Energy (zpe) 7310.3 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 PBE1PBE/STO-3G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.097 |
1.144 |
0.000 |
S2 |
0.097 |
-0.631 |
0.000 |
H3 |
-1.258 |
-0.823 |
0.000 |
H4 |
-0.490 |
1.451 |
0.825 |
H5 |
-0.490 |
1.451 |
-0.825 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7750 | 2.3890 | 1.0583 | 1.0583 |
S2 | 1.7750 | | 1.3692 | 2.3153 | 2.3153 | H3 | 2.3890 | 1.3692 | | 2.5386 | 2.5386 | H4 | 1.0583 | 2.3153 | 2.5386 | | 1.6507 | H5 | 1.0583 | 2.3153 | 2.5386 | 1.6507 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
98.069 |
|
S2 |
N1 |
H4 |
106.870 |
S2 |
N1 |
H5 |
106.870 |
|
H4 |
N1 |
H5 |
102.502 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.430 |
|
|
|
2 |
S |
0.150 |
|
|
|
3 |
H |
-0.030 |
|
|
|
4 |
H |
0.155 |
|
|
|
5 |
H |
0.155 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.362 |
0.081 |
0.000 |
2.364 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-17.360 |
-1.788 |
0.000 |
y |
-1.788 |
-17.924 |
0.000 |
z |
0.000 |
0.000 |
-17.420 |
|
Traceless |
| x | y | z |
x |
0.312 |
-1.788 |
0.000 |
y |
-1.788 |
-0.535 |
0.000 |
z |
0.000 |
0.000 |
0.222 |
|
Polar |
3z2-r2 | 0.445 |
x2-y2 | 0.565 |
xy | -1.788 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.507 |
0.039 |
0.000 |
y |
0.039 |
2.342 |
0.000 |
z |
0.000 |
0.000 |
0.937 |
<r2> (average value of r
2) Å
2
<r2> |
35.036 |
(<r2>)1/2 |
5.919 |