Jump to
S1C2
Energy calculated at B1B95/3-21G*
| hartrees |
Energy at 0K | -452.555988 |
Energy at 298.15K | -452.559658 |
HF Energy | -452.555988 |
Nuclear repulsion energy | 58.780457 |
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 B1B95/3-21G*
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' |
3571 |
3410 |
6.45 |
|
|
|
2 |
A' |
2510 |
2397 |
120.02 |
|
|
|
3 |
A' |
1675 |
1599 |
4.28 |
|
|
|
4 |
A' |
1065 |
1017 |
21.09 |
|
|
|
5 |
A' |
915 |
874 |
39.64 |
|
|
|
6 |
A' |
334 |
319 |
394.65 |
|
|
|
7 |
A" |
3699 |
3532 |
30.64 |
|
|
|
8 |
A" |
1079 |
1030 |
19.14 |
|
|
|
9 |
A" |
697 |
666 |
0.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7771.9 cm
-1
Scaled (by 0.9549) Zero Point Vibrational Energy (zpe) 7421.4 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 B1B95/3-21G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.053 |
1.056 |
0.000 |
S2 |
0.053 |
-0.601 |
0.000 |
H3 |
-1.272 |
-0.917 |
0.000 |
H4 |
0.022 |
1.572 |
0.865 |
H5 |
0.022 |
1.572 |
-0.865 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.6575 | 2.3773 | 1.0081 | 1.0081 |
S2 | 1.6575 | | 1.3627 | 2.3399 | 2.3399 | H3 | 2.3773 | 1.3627 | | 2.9364 | 2.9364 | H4 | 1.0081 | 2.3399 | 2.9364 | | 1.7306 | H5 | 1.0081 | 2.3399 | 2.9364 | 1.7306 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
103.408 |
|
S2 |
N1 |
H4 |
120.806 |
S2 |
N1 |
H5 |
120.806 |
|
H4 |
N1 |
H5 |
118.261 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.795 |
|
|
|
2 |
S |
0.066 |
|
|
|
3 |
H |
0.078 |
|
|
|
4 |
H |
0.326 |
|
|
|
5 |
H |
0.326 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.965 |
1.693 |
0.000 |
1.949 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.247 |
0.911 |
0.000 |
y |
0.911 |
-16.534 |
0.000 |
z |
0.000 |
0.000 |
-19.456 |
|
Traceless |
| x | y | z |
x |
-2.252 |
0.911 |
0.000 |
y |
0.911 |
3.317 |
0.000 |
z |
0.000 |
0.000 |
-1.065 |
|
Polar |
3z2-r2 | -2.131 |
x2-y2 | -3.713 |
xy | 0.911 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.584 |
0.554 |
0.000 |
y |
0.554 |
3.635 |
0.000 |
z |
0.000 |
0.000 |
2.213 |
<r2> (average value of r
2) Å
2
<r2> |
34.272 |
(<r2>)1/2 |
5.854 |
Jump to
S1C1
Energy calculated at B1B95/3-21G*
| hartrees |
Energy at 0K | -452.555988 |
Energy at 298.15K | -452.559658 |
HF Energy | -452.555988 |
Nuclear repulsion energy | 58.779568 |
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 B1B95/3-21G*
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' |
3571 |
3410 |
6.49 |
|
|
|
2 |
A' |
2510 |
2397 |
119.85 |
|
|
|
3 |
A' |
1675 |
1599 |
4.30 |
|
|
|
4 |
A' |
1065 |
1017 |
20.97 |
|
|
|
5 |
A' |
915 |
873 |
39.72 |
|
|
|
6 |
A' |
334 |
319 |
394.61 |
|
|
|
7 |
A" |
3699 |
3532 |
30.69 |
|
|
|
8 |
A" |
1079 |
1030 |
19.16 |
|
|
|
9 |
A" |
697 |
666 |
0.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7771.8 cm
-1
Scaled (by 0.9549) Zero Point Vibrational Energy (zpe) 7421.3 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 B1B95/3-21G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.053 |
1.056 |
0.000 |
S2 |
0.053 |
-0.601 |
0.000 |
H3 |
-1.272 |
-0.917 |
0.000 |
H4 |
0.023 |
1.572 |
0.865 |
H5 |
0.023 |
1.572 |
-0.865 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.6576 | 2.3771 | 1.0081 | 1.0081 |
S2 | 1.6576 | | 1.3626 | 2.3399 | 2.3399 | H3 | 2.3771 | 1.3626 | | 2.9368 | 2.9368 | H4 | 1.0081 | 2.3399 | 2.9368 | | 1.7308 | H5 | 1.0081 | 2.3399 | 2.9368 | 1.7308 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
103.393 |
|
S2 |
N1 |
H4 |
120.803 |
S2 |
N1 |
H5 |
120.803 |
|
H4 |
N1 |
H5 |
118.280 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.795 |
|
|
|
2 |
S |
0.066 |
|
|
|
3 |
H |
0.078 |
|
|
|
4 |
H |
0.326 |
|
|
|
5 |
H |
0.326 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.959 |
1.693 |
0.000 |
1.946 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.246 |
0.922 |
0.000 |
y |
0.922 |
-16.535 |
0.000 |
z |
0.000 |
0.000 |
-19.455 |
|
Traceless |
| x | y | z |
x |
-2.251 |
0.922 |
0.000 |
y |
0.922 |
3.316 |
0.000 |
z |
0.000 |
0.000 |
-1.065 |
|
Polar |
3z2-r2 | -2.130 |
x2-y2 | -3.711 |
xy | 0.922 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.584 |
0.554 |
0.000 |
y |
0.554 |
3.635 |
0.000 |
z |
0.000 |
0.000 |
2.213 |
<r2> (average value of r
2) Å
2
<r2> |
34.272 |
(<r2>)1/2 |
5.854 |