Jump to
S1C2
Energy calculated at B1B95/cc-pVTZ
| hartrees |
Energy at 0K | -454.784573 |
Energy at 298.15K | -454.788354 |
HF Energy | -454.784573 |
Nuclear repulsion energy | 58.035163 |
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 B1B95/cc-pVTZ
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' |
3557 |
3404 |
6.39 |
|
|
|
2 |
A' |
2672 |
2557 |
14.11 |
|
|
|
3 |
A' |
1629 |
1560 |
13.09 |
|
|
|
4 |
A' |
1047 |
1002 |
7.70 |
|
|
|
5 |
A' |
888 |
850 |
33.64 |
|
|
|
6 |
A' |
652 |
624 |
91.79 |
|
|
|
7 |
A" |
3653 |
3496 |
21.64 |
|
|
|
8 |
A" |
1134 |
1086 |
1.58 |
|
|
|
9 |
A" |
461 |
442 |
48.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7846.0 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 7509.4 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 B1B95/cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.015 |
1.099 |
0.000 |
S2 |
0.015 |
-0.613 |
0.000 |
H3 |
-1.319 |
-0.782 |
0.000 |
H4 |
0.485 |
1.444 |
0.822 |
H5 |
0.485 |
1.444 |
-0.822 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7118 | 2.3065 | 1.0076 | 1.0076 |
S2 | 1.7118 | | 1.3447 | 2.2641 | 2.2641 | H3 | 2.3065 | 1.3447 | | 2.9808 | 2.9808 | H4 | 1.0076 | 2.2641 | 2.9808 | | 1.6444 | H5 | 1.0076 | 2.2641 | 2.9808 | 1.6444 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
97.259 |
|
S2 |
N1 |
H4 |
110.014 |
S2 |
N1 |
H5 |
110.014 |
|
H4 |
N1 |
H5 |
109.378 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.349 |
|
|
|
2 |
S |
-0.107 |
|
|
|
3 |
H |
0.117 |
|
|
|
4 |
H |
0.169 |
|
|
|
5 |
H |
0.169 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.497 |
0.943 |
0.000 |
1.066 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.014 |
3.394 |
0.000 |
y |
3.394 |
-18.800 |
0.000 |
z |
0.000 |
0.000 |
-20.034 |
|
Traceless |
| x | y | z |
x |
0.403 |
3.394 |
0.000 |
y |
3.394 |
0.724 |
0.000 |
z |
0.000 |
0.000 |
-1.127 |
|
Polar |
3z2-r2 | -2.254 |
x2-y2 | -0.214 |
xy | 3.394 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.767 |
0.401 |
0.000 |
y |
0.401 |
4.812 |
0.000 |
z |
0.000 |
0.000 |
3.210 |
<r2> (average value of r
2) Å
2
<r2> |
34.854 |
(<r2>)1/2 |
5.904 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVTZ
| hartrees |
Energy at 0K | -454.784333 |
Energy at 298.15K | -454.788157 |
HF Energy | -454.784333 |
Nuclear repulsion energy | 58.253256 |
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 B1B95/cc-pVTZ
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' |
3556 |
3404 |
2.66 |
|
|
|
2 |
A' |
2587 |
2476 |
42.51 |
|
|
|
3 |
A' |
1616 |
1547 |
13.14 |
|
|
|
4 |
A' |
1019 |
976 |
21.77 |
|
|
|
5 |
A' |
894 |
856 |
15.47 |
|
|
|
6 |
A' |
623 |
596 |
136.00 |
|
|
|
7 |
A" |
3661 |
3504 |
21.61 |
|
|
|
8 |
A" |
1115 |
1067 |
1.90 |
|
|
|
9 |
A" |
546 |
523 |
2.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7808.8 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 7473.8 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 B1B95/cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.083 |
1.090 |
0.000 |
S2 |
0.083 |
-0.606 |
0.000 |
H3 |
-1.238 |
-0.902 |
0.000 |
H4 |
-0.334 |
1.481 |
0.829 |
H5 |
-0.334 |
1.481 |
-0.829 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.6952 | 2.3901 | 1.0068 | 1.0068 |
S2 | 1.6952 | | 1.3539 | 2.2837 | 2.2837 | H3 | 2.3901 | 1.3539 | | 2.6807 | 2.6807 | H4 | 1.0068 | 2.2837 | 2.6807 | | 1.6573 | H5 | 1.0068 | 2.2837 | 2.6807 | 1.6573 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
102.656 |
|
S2 |
N1 |
H4 |
112.899 |
S2 |
N1 |
H5 |
112.899 |
|
H4 |
N1 |
H5 |
110.777 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.343 |
|
|
|
2 |
S |
-0.085 |
|
|
|
3 |
H |
0.092 |
|
|
|
4 |
H |
0.168 |
|
|
|
5 |
H |
0.168 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.933 |
1.062 |
0.000 |
2.205 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.849 |
-1.060 |
0.000 |
y |
-1.060 |
-18.150 |
0.000 |
z |
0.000 |
0.000 |
-19.979 |
|
Traceless |
| x | y | z |
x |
-0.784 |
-1.060 |
0.000 |
y |
-1.060 |
1.764 |
0.000 |
z |
0.000 |
0.000 |
-0.980 |
|
Polar |
3z2-r2 | -1.960 |
x2-y2 | -1.699 |
xy | -1.060 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.748 |
0.215 |
0.000 |
y |
0.215 |
4.789 |
0.000 |
z |
0.000 |
0.000 |
3.207 |
<r2> (average value of r
2) Å
2
<r2> |
34.739 |
(<r2>)1/2 |
5.894 |