Jump to
S1C2
Energy calculated at B1B95/aug-cc-pVDZ
| hartrees |
Energy at 0K | -454.755880 |
Energy at 298.15K | -454.759632 |
HF Energy | -454.755880 |
Nuclear repulsion energy | 57.435499 |
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/aug-cc-pVDZ
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' |
3543 |
3393 |
6.25 |
|
|
|
2 |
A' |
2674 |
2562 |
9.53 |
|
|
|
3 |
A' |
1601 |
1533 |
12.64 |
|
|
|
4 |
A' |
1026 |
983 |
8.96 |
|
|
|
5 |
A' |
875 |
838 |
36.34 |
|
|
|
6 |
A' |
664 |
636 |
68.81 |
|
|
|
7 |
A" |
3643 |
3489 |
24.20 |
|
|
|
8 |
A" |
1121 |
1073 |
0.60 |
|
|
|
9 |
A" |
431 |
413 |
46.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7788.1 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 7460.2 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/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.014 |
1.114 |
0.000 |
S2 |
0.014 |
-0.620 |
0.000 |
H3 |
-1.331 |
-0.778 |
0.000 |
H4 |
0.502 |
1.449 |
0.823 |
H5 |
0.502 |
1.449 |
-0.823 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7341 | 2.3215 | 1.0136 | 1.0136 |
S2 | 1.7341 | | 1.3544 | 2.2798 | 2.2798 | H3 | 2.3215 | 1.3544 | | 2.9997 | 2.9997 | H4 | 1.0136 | 2.2798 | 2.9997 | | 1.6455 | H5 | 1.0136 | 2.2798 | 2.9997 | 1.6455 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
96.698 |
|
S2 |
N1 |
H4 |
109.318 |
S2 |
N1 |
H5 |
109.318 |
|
H4 |
N1 |
H5 |
108.531 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.341 |
|
|
|
2 |
S |
0.250 |
|
|
|
3 |
H |
0.077 |
|
|
|
4 |
H |
0.007 |
|
|
|
5 |
H |
0.007 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.521 |
0.888 |
0.000 |
1.030 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.301 |
3.492 |
0.000 |
y |
3.492 |
-19.303 |
0.000 |
z |
0.000 |
0.000 |
-20.453 |
|
Traceless |
| x | y | z |
x |
0.577 |
3.492 |
0.000 |
y |
3.492 |
0.574 |
0.000 |
z |
0.000 |
0.000 |
-1.151 |
|
Polar |
3z2-r2 | -2.301 |
x2-y2 | 0.002 |
xy | 3.492 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.471 |
0.307 |
0.000 |
y |
0.307 |
5.676 |
0.000 |
z |
0.000 |
0.000 |
4.332 |
<r2> (average value of r
2) Å
2
<r2> |
35.576 |
(<r2>)1/2 |
5.965 |
Jump to
S1C1
Energy calculated at B1B95/aug-cc-pVDZ
| hartrees |
Energy at 0K | -454.755255 |
Energy at 298.15K | -454.759049 |
HF Energy | -454.755255 |
Nuclear repulsion energy | 57.628426 |
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/aug-cc-pVDZ
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' |
3545 |
3396 |
2.78 |
|
|
|
2 |
A' |
2596 |
2487 |
31.21 |
|
|
|
3 |
A' |
1588 |
1521 |
12.78 |
|
|
|
4 |
A' |
997 |
955 |
20.28 |
|
|
|
5 |
A' |
877 |
840 |
18.43 |
|
|
|
6 |
A' |
630 |
604 |
107.35 |
|
|
|
7 |
A" |
3657 |
3503 |
24.14 |
|
|
|
8 |
A" |
1105 |
1059 |
0.95 |
|
|
|
9 |
A" |
511 |
490 |
2.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7753.5 cm
-1
Scaled (by 0.9579) Zero Point Vibrational Energy (zpe) 7427.1 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/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.085 |
1.106 |
0.000 |
S2 |
0.085 |
-0.613 |
0.000 |
H3 |
-1.247 |
-0.904 |
0.000 |
H4 |
-0.353 |
1.487 |
0.830 |
H5 |
-0.353 |
1.487 |
-0.830 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7186 | 2.4105 | 1.0125 | 1.0125 |
S2 | 1.7186 | | 1.3628 | 2.2996 | 2.2996 | H3 | 2.4105 | 1.3628 | | 2.6835 | 2.6835 | H4 | 1.0125 | 2.2996 | 2.6835 | | 1.6596 | H5 | 1.0125 | 2.2996 | 2.6835 | 1.6596 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
102.322 |
|
S2 |
N1 |
H4 |
112.099 |
S2 |
N1 |
H5 |
112.099 |
|
H4 |
N1 |
H5 |
110.071 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.304 |
|
|
|
2 |
S |
0.298 |
|
|
|
3 |
H |
0.017 |
|
|
|
4 |
H |
-0.005 |
|
|
|
5 |
H |
-0.005 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.972 |
0.989 |
0.000 |
2.206 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.145 |
-1.214 |
0.000 |
y |
-1.214 |
-18.597 |
0.000 |
z |
0.000 |
0.000 |
-20.383 |
|
Traceless |
| x | y | z |
x |
-0.655 |
-1.214 |
0.000 |
y |
-1.214 |
1.667 |
0.000 |
z |
0.000 |
0.000 |
-1.012 |
|
Polar |
3z2-r2 | -2.025 |
x2-y2 | -1.548 |
xy | -1.214 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.491 |
0.230 |
0.000 |
y |
0.230 |
5.616 |
0.000 |
z |
0.000 |
0.000 |
4.329 |
<r2> (average value of r
2) Å
2
<r2> |
35.461 |
(<r2>)1/2 |
5.955 |