Jump to
S1C2
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -477.837214 |
| Energy at 298.15K | |
| HF Energy | -477.837214 |
| Nuclear repulsion energy | 107.888883 |
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 HSEh1PBE/6-311+G(3df,2p)
| 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' |
3124 |
3124 |
19.66 |
|
|
|
| 2 |
A' |
3069 |
3069 |
18.32 |
|
|
|
| 3 |
A' |
3048 |
3048 |
18.13 |
|
|
|
| 4 |
A' |
2707 |
2707 |
1.93 |
|
|
|
| 5 |
A' |
1498 |
1498 |
3.57 |
|
|
|
| 6 |
A' |
1484 |
1484 |
3.30 |
|
|
|
| 7 |
A' |
1409 |
1409 |
4.63 |
|
|
|
| 8 |
A' |
1294 |
1294 |
27.04 |
|
|
|
| 9 |
A' |
1118 |
1118 |
1.28 |
|
|
|
| 10 |
A' |
1005 |
1005 |
3.81 |
|
|
|
| 11 |
A' |
862 |
862 |
0.89 |
|
|
|
| 12 |
A' |
693 |
693 |
1.02 |
|
|
|
| 13 |
A' |
302 |
302 |
2.00 |
|
|
|
| 14 |
A" |
3135 |
3135 |
20.45 |
|
|
|
| 15 |
A" |
3110 |
3110 |
0.38 |
|
|
|
| 16 |
A" |
1488 |
1488 |
10.53 |
|
|
|
| 17 |
A" |
1266 |
1266 |
0.44 |
|
|
|
| 18 |
A" |
1043 |
1043 |
0.35 |
|
|
|
| 19 |
A" |
787 |
787 |
3.65 |
|
|
|
| 20 |
A" |
251 |
251 |
0.68 |
|
|
|
| 21 |
A" |
153 |
153 |
14.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16421.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16421.5 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.509 |
0.678 |
0.000 |
| C2 |
0.000 |
0.827 |
0.000 |
| S3 |
-0.753 |
-0.829 |
0.000 |
| H4 |
1.985 |
1.660 |
0.000 |
| H5 |
1.851 |
0.136 |
0.883 |
| H6 |
1.851 |
0.136 |
-0.883 |
| H7 |
-0.332 |
1.369 |
0.885 |
| H8 |
-0.332 |
1.369 |
-0.885 |
| H9 |
-2.036 |
-0.437 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5164 | 2.7177 | 1.0912 | 1.0911 | 1.0911 | 2.1567 | 2.1567 | 3.7158 |
C2 | 1.5164 | | 1.8190 | 2.1523 | 2.1644 | 2.1644 | 1.0898 | 1.0898 | 2.3960 | S3 | 2.7177 | 1.8190 | | 3.6997 | 2.9143 | 2.9143 | 2.4064 | 2.4064 | 1.3416 | H4 | 1.0912 | 2.1523 | 3.6997 | | 1.7662 | 1.7662 | 2.4972 | 2.4972 | 4.5341 | H5 | 1.0911 | 2.1644 | 2.9143 | 1.7662 | | 1.7664 | 2.5074 | 3.0684 | 4.0271 | H6 | 1.0911 | 2.1644 | 2.9143 | 1.7662 | 1.7664 | | 3.0684 | 2.5074 | 4.0271 | H7 | 2.1567 | 1.0898 | 2.4064 | 2.4972 | 2.5074 | 3.0684 | | 1.7706 | 2.6353 | H8 | 2.1567 | 1.0898 | 2.4064 | 2.4972 | 3.0684 | 2.5074 | 1.7706 | | 2.6353 | H9 | 3.7158 | 2.3960 | 1.3416 | 4.5341 | 4.0271 | 4.0271 | 2.6353 | 2.6353 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
108.799 |
|
C1 |
C2 |
H7 |
110.626 |
| C1 |
C2 |
H8 |
110.626 |
|
C2 |
C1 |
H4 |
110.190 |
| C2 |
C1 |
H5 |
111.164 |
|
C2 |
C1 |
H6 |
111.164 |
| C2 |
S3 |
H9 |
97.440 |
|
S3 |
C2 |
H7 |
109.051 |
| S3 |
C2 |
H8 |
109.051 |
|
H4 |
C1 |
H5 |
108.060 |
| H4 |
C1 |
H6 |
108.060 |
|
H5 |
C1 |
H6 |
108.085 |
| H7 |
C2 |
H8 |
108.656 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.329 |
|
|
|
| 2 |
C |
-0.243 |
|
|
|
| 3 |
S |
-0.323 |
|
|
|
| 4 |
H |
0.133 |
|
|
|
| 5 |
H |
0.155 |
|
|
|
| 6 |
H |
0.155 |
|
|
|
| 7 |
H |
0.149 |
|
|
|
| 8 |
H |
0.149 |
|
|
|
| 9 |
H |
0.153 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.104 |
1.675 |
0.000 |
1.678 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.006 |
-0.271 |
0.000 |
| y |
-0.271 |
-28.250 |
0.000 |
| z |
0.000 |
0.000 |
-29.092 |
|
| Traceless |
| | x | y | z |
| x |
3.666 |
-0.271 |
0.000 |
| y |
-0.271 |
-1.202 |
0.000 |
| z |
0.000 |
0.000 |
-2.464 |
|
| Polar |
| 3z2-r2 | -4.928 |
| x2-y2 | 3.245 |
| xy | -0.271 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.667 |
0.911 |
0.000 |
| y |
0.911 |
7.303 |
0.000 |
| z |
0.000 |
0.000 |
6.313 |
<r2> (average value of r
2) Å
2
| <r2> |
82.745 |
| (<r2>)1/2 |
9.096 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -477.838141 |
| Energy at 298.15K | |
| HF Energy | -477.838141 |
| Nuclear repulsion energy | 107.588238 |
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 HSEh1PBE/6-311+G(3df,2p)
| 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 |
3136 |
3136 |
21.02 |
12.30 |
0.75 |
0.86 |
| 2 |
A |
3114 |
3114 |
14.73 |
71.55 |
0.71 |
0.83 |
| 3 |
A |
3106 |
3106 |
11.91 |
105.36 |
0.69 |
0.82 |
| 4 |
A |
3069 |
3069 |
11.01 |
125.11 |
0.09 |
0.16 |
| 5 |
A |
3041 |
3041 |
24.26 |
178.09 |
0.04 |
0.08 |
| 6 |
A |
2709 |
2709 |
1.78 |
108.14 |
0.22 |
0.36 |
| 7 |
A |
1493 |
1493 |
3.50 |
2.89 |
0.75 |
0.86 |
| 8 |
A |
1485 |
1485 |
11.40 |
4.91 |
0.74 |
0.85 |
| 9 |
A |
1472 |
1472 |
2.08 |
7.62 |
0.71 |
0.83 |
| 10 |
A |
1407 |
1407 |
5.22 |
0.45 |
0.75 |
0.86 |
| 11 |
A |
1303 |
1303 |
16.03 |
1.78 |
0.34 |
0.50 |
| 12 |
A |
1278 |
1278 |
3.42 |
1.66 |
0.75 |
0.86 |
| 13 |
A |
1123 |
1123 |
6.11 |
3.21 |
0.32 |
0.48 |
| 14 |
A |
1072 |
1072 |
0.50 |
3.90 |
0.20 |
0.34 |
| 15 |
A |
995 |
995 |
6.75 |
3.36 |
0.74 |
0.85 |
| 16 |
A |
875 |
875 |
5.81 |
1.55 |
0.30 |
0.46 |
| 17 |
A |
737 |
737 |
1.97 |
3.11 |
0.20 |
0.33 |
| 18 |
A |
674 |
674 |
2.67 |
10.38 |
0.20 |
0.33 |
| 19 |
A |
330 |
330 |
1.37 |
1.17 |
0.21 |
0.34 |
| 20 |
A |
260 |
260 |
2.50 |
0.21 |
0.42 |
0.59 |
| 21 |
A |
223 |
223 |
11.89 |
0.52 |
0.66 |
0.80 |
Unscaled Zero Point Vibrational Energy (zpe) 16450.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16450.5 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.631 |
-0.347 |
-0.053 |
| C2 |
0.492 |
0.640 |
0.091 |
| S3 |
-1.157 |
-0.100 |
-0.080 |
| H4 |
2.594 |
0.165 |
0.018 |
| H5 |
1.597 |
-1.103 |
0.734 |
| H6 |
1.584 |
-0.862 |
-1.013 |
| H7 |
0.543 |
1.174 |
1.040 |
| H8 |
0.526 |
1.391 |
-0.700 |
| H9 |
-1.074 |
-0.927 |
0.973 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5146 | 2.7991 | 1.0931 | 1.0914 | 1.0902 | 2.1667 | 2.1593 | 2.9505 |
C2 | 1.5146 | | 1.8148 | 2.1566 | 2.1617 | 2.1606 | 1.0903 | 1.0914 | 2.3842 | S3 | 2.7991 | 1.8148 | | 3.7614 | 3.0416 | 2.9939 | 2.4013 | 2.3323 | 1.3421 | H4 | 1.0931 | 2.1566 | 3.7614 | | 1.7649 | 1.7714 | 2.5040 | 2.5089 | 3.9443 | H5 | 1.0914 | 2.1617 | 3.0416 | 1.7649 | | 1.7629 | 2.5282 | 3.0698 | 2.6870 | H6 | 1.0902 | 2.1606 | 2.9939 | 1.7714 | 1.7629 | | 3.0733 | 2.5091 | 3.3185 | H7 | 2.1667 | 1.0903 | 2.4013 | 2.5040 | 2.5282 | 3.0733 | | 1.7533 | 2.6521 | H8 | 2.1593 | 1.0914 | 2.3323 | 2.5089 | 3.0698 | 2.5091 | 1.7533 | | 3.2763 | H9 | 2.9505 | 2.3842 | 1.3421 | 3.9443 | 2.6870 | 3.3185 | 2.6521 | 3.2763 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
114.128 |
|
C1 |
C2 |
H7 |
111.524 |
| C1 |
C2 |
H8 |
110.860 |
|
C2 |
C1 |
H4 |
110.545 |
| C2 |
C1 |
H5 |
111.055 |
|
C2 |
C1 |
H6 |
111.042 |
| C2 |
S3 |
H9 |
96.949 |
|
S3 |
C2 |
H7 |
108.935 |
| S3 |
C2 |
H8 |
103.951 |
|
H4 |
C1 |
H5 |
107.793 |
| H4 |
C1 |
H6 |
108.463 |
|
H5 |
C1 |
H6 |
107.821 |
| H7 |
C2 |
H8 |
106.955 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.254 |
|
|
|
| 2 |
C |
-0.292 |
|
|
|
| 3 |
S |
-0.295 |
|
|
|
| 4 |
H |
0.130 |
|
|
|
| 5 |
H |
0.138 |
|
|
|
| 6 |
H |
0.147 |
|
|
|
| 7 |
H |
0.146 |
|
|
|
| 8 |
H |
0.142 |
|
|
|
| 9 |
H |
0.138 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.567 |
0.163 |
0.661 |
1.708 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.182 |
1.272 |
-0.628 |
| y |
1.272 |
-27.238 |
-1.718 |
| z |
-0.628 |
-1.718 |
-27.045 |
|
| Traceless |
| | x | y | z |
| x |
-2.040 |
1.272 |
-0.628 |
| y |
1.272 |
0.875 |
-1.718 |
| z |
-0.628 |
-1.718 |
1.165 |
|
| Polar |
| 3z2-r2 | 2.331 |
| x2-y2 | -1.944 |
| xy | 1.272 |
| xz | -0.628 |
| yz | -1.718 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.430 |
0.216 |
-0.063 |
| y |
0.216 |
6.707 |
0.042 |
| z |
-0.063 |
0.042 |
6.286 |
<r2> (average value of r
2) Å
2
| <r2> |
83.468 |
| (<r2>)1/2 |
9.136 |