Jump to
S1C2
Energy calculated at B3LYP/6-311G*
| hartrees |
Energy at 0K | -454.760120 |
Energy at 298.15K | -454.763901 |
HF Energy | -454.760120 |
Nuclear repulsion energy | 57.327681 |
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 B3LYP/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' |
3522 |
3403 |
2.27 |
|
|
|
2 |
A' |
2575 |
2488 |
37.00 |
|
|
|
3 |
A' |
1698 |
1641 |
18.76 |
|
|
|
4 |
A' |
1042 |
1007 |
11.34 |
|
|
|
5 |
A' |
900 |
870 |
67.14 |
|
|
|
6 |
A' |
625 |
604 |
77.47 |
|
|
|
7 |
A" |
3613 |
3491 |
10.71 |
|
|
|
8 |
A" |
1166 |
1127 |
7.30 |
|
|
|
9 |
A" |
481 |
465 |
72.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7810.7 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 7547.5 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 B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.016 |
1.116 |
0.000 |
S2 |
0.016 |
-0.621 |
0.000 |
H3 |
-1.329 |
-0.797 |
0.000 |
H4 |
0.485 |
1.464 |
0.826 |
H5 |
0.485 |
1.464 |
-0.826 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7373 | 2.3377 | 1.0119 | 1.0119 |
S2 | 1.7373 | | 1.3557 | 2.2918 | 2.2918 | H3 | 2.3377 | 1.3557 | | 3.0138 | 3.0138 | H4 | 1.0119 | 2.2918 | 3.0138 | | 1.6519 | H5 | 1.0119 | 2.2918 | 3.0138 | 1.6519 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
97.425 |
|
S2 |
N1 |
H4 |
110.140 |
S2 |
N1 |
H5 |
110.140 |
|
H4 |
N1 |
H5 |
109.423 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.849 |
|
|
|
2 |
S |
-0.012 |
|
|
|
3 |
H |
0.152 |
|
|
|
4 |
H |
0.354 |
|
|
|
5 |
H |
0.354 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.594 |
0.958 |
0.000 |
1.127 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.481 |
3.842 |
0.000 |
y |
3.842 |
-19.213 |
0.000 |
z |
0.000 |
0.000 |
-20.761 |
|
Traceless |
| x | y | z |
x |
0.506 |
3.842 |
0.000 |
y |
3.842 |
0.908 |
0.000 |
z |
0.000 |
0.000 |
-1.414 |
|
Polar |
3z2-r2 | -2.827 |
x2-y2 | -0.268 |
xy | 3.842 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.327 |
0.463 |
0.000 |
y |
0.463 |
4.362 |
0.000 |
z |
0.000 |
0.000 |
2.579 |
<r2> (average value of r
2) Å
2
<r2> |
35.801 |
(<r2>)1/2 |
5.983 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G*
| hartrees |
Energy at 0K | -454.758920 |
Energy at 298.15K | -454.762735 |
HF Energy | -454.758920 |
Nuclear repulsion energy | 57.694460 |
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 B3LYP/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' |
3525 |
3407 |
1.32 |
|
|
|
2 |
A' |
2456 |
2373 |
104.56 |
|
|
|
3 |
A' |
1677 |
1620 |
10.49 |
|
|
|
4 |
A' |
1017 |
983 |
44.69 |
|
|
|
5 |
A' |
870 |
841 |
29.05 |
|
|
|
6 |
A' |
593 |
573 |
178.90 |
|
|
|
7 |
A" |
3627 |
3504 |
11.46 |
|
|
|
8 |
A" |
1145 |
1106 |
9.90 |
|
|
|
9 |
A" |
576 |
557 |
5.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7742.3 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 7481.4 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 B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.082 |
1.099 |
0.000 |
S2 |
0.082 |
-0.612 |
0.000 |
H3 |
-1.252 |
-0.929 |
0.000 |
H4 |
-0.314 |
1.510 |
0.835 |
H5 |
-0.314 |
1.510 |
-0.835 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7109 | 2.4276 | 1.0109 | 1.0109 |
S2 | 1.7109 | | 1.3706 | 2.3141 | 2.3141 | H3 | 2.4276 | 1.3706 | | 2.7435 | 2.7435 | H4 | 1.0109 | 2.3141 | 2.7435 | | 1.6690 | H5 | 1.0109 | 2.3141 | 2.7435 | 1.6690 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
103.407 |
|
S2 |
N1 |
H4 |
113.984 |
S2 |
N1 |
H5 |
113.984 |
|
H4 |
N1 |
H5 |
111.284 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.843 |
|
|
|
2 |
S |
0.039 |
|
|
|
3 |
H |
0.102 |
|
|
|
4 |
H |
0.351 |
|
|
|
5 |
H |
0.351 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.256 |
1.156 |
0.000 |
2.535 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.567 |
-1.138 |
0.000 |
y |
-1.138 |
-18.358 |
0.000 |
z |
0.000 |
0.000 |
-20.639 |
|
Traceless |
| x | y | z |
x |
-1.069 |
-1.138 |
0.000 |
y |
-1.138 |
2.246 |
0.000 |
z |
0.000 |
0.000 |
-1.177 |
|
Polar |
3z2-r2 | -2.354 |
x2-y2 | -2.210 |
xy | -1.138 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.332 |
0.284 |
0.000 |
y |
0.284 |
4.314 |
0.000 |
z |
0.000 |
0.000 |
2.572 |
<r2> (average value of r
2) Å
2
<r2> |
35.580 |
(<r2>)1/2 |
5.965 |