Jump to
S1C2
Energy calculated at BLYP/6-31G*
| hartrees |
Energy at 0K | -554.065840 |
Energy at 298.15K | |
HF Energy | -554.065840 |
Nuclear repulsion energy | 196.052165 |
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 BLYP/6-31G*
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 |
3170 |
3144 |
17.27 |
|
|
|
2 |
A |
3097 |
3072 |
3.49 |
|
|
|
3 |
A |
3086 |
3061 |
12.73 |
|
|
|
4 |
A |
1626 |
1612 |
4.31 |
|
|
|
5 |
A |
1406 |
1394 |
8.95 |
|
|
|
6 |
A |
1295 |
1285 |
0.04 |
|
|
|
7 |
A |
1042 |
1033 |
0.72 |
|
|
|
8 |
A |
938 |
930 |
0.00 |
|
|
|
9 |
A |
833 |
827 |
0.00 |
|
|
|
10 |
A |
685 |
680 |
0.36 |
|
|
|
11 |
A |
591 |
587 |
0.00 |
|
|
|
12 |
A |
391 |
388 |
0.90 |
|
|
|
13 |
A |
171 |
169 |
0.13 |
|
|
|
14 |
A |
51i |
50i |
0.00 |
|
|
|
15 |
B |
3170 |
3144 |
1.19 |
|
|
|
16 |
B |
3097 |
3071 |
3.18 |
|
|
|
17 |
B |
3087 |
3062 |
0.18 |
|
|
|
18 |
B |
1604 |
1591 |
130.56 |
|
|
|
19 |
B |
1397 |
1386 |
18.36 |
|
|
|
20 |
B |
1261 |
1251 |
15.86 |
|
|
|
21 |
B |
1012 |
1004 |
25.58 |
|
|
|
22 |
B |
948 |
940 |
47.73 |
|
|
|
23 |
B |
835 |
828 |
63.52 |
|
|
|
24 |
B |
691 |
685 |
42.19 |
|
|
|
25 |
B |
526 |
521 |
17.87 |
|
|
|
26 |
B |
380 |
377 |
3.88 |
|
|
|
27 |
B |
32i |
32i |
0.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18126.6 cm
-1
Scaled (by 0.9919) Zero Point Vibrational Energy (zpe) 17979.8 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 BLYP/6-31G*
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.626 |
C2 |
0.001 |
1.388 |
-0.495 |
C3 |
-0.001 |
-1.388 |
-0.495 |
C4 |
0.000 |
2.677 |
-0.100 |
C5 |
0.000 |
-2.677 |
-0.100 |
H6 |
0.036 |
1.118 |
-1.556 |
H7 |
-0.036 |
-1.118 |
-1.556 |
H8 |
-0.037 |
3.480 |
-0.839 |
H9 |
0.006 |
2.977 |
0.952 |
H10 |
0.037 |
-3.480 |
-0.839 |
H11 |
-0.006 |
-2.977 |
0.952 |
Atom - Atom Distances (Å)
|
S1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
S1 | | 1.7843 | 1.7843 | 2.7735 | 2.7735 | 2.4519 | 2.4519 | 3.7763 | 2.9951 | 3.7763 | 2.9951 |
C2 | 1.7843 | | 2.7760 | 1.3479 | 4.0839 | 1.0953 | 2.7211 | 2.1206 | 2.1492 | 4.8803 | 4.5988 | C3 | 1.7843 | 2.7760 | | 4.0839 | 1.3479 | 2.7211 | 1.0953 | 4.8803 | 4.5988 | 2.1206 | 2.1492 | C4 | 2.7735 | 1.3479 | 4.0839 | | 5.3535 | 2.1335 | 4.0641 | 1.0925 | 1.0938 | 6.2011 | 5.7511 | C5 | 2.7735 | 4.0839 | 1.3479 | 5.3535 | | 4.0641 | 2.1335 | 6.2011 | 5.7511 | 1.0925 | 1.0938 | H6 | 2.4519 | 1.0953 | 2.7211 | 2.1335 | 4.0641 | | 2.2362 | 2.4698 | 3.1220 | 4.6530 | 4.8018 | H7 | 2.4519 | 2.7211 | 1.0953 | 4.0641 | 2.1335 | 2.2362 | | 4.6530 | 4.8018 | 2.4698 | 3.1220 | H8 | 3.7763 | 2.1206 | 4.8803 | 1.0925 | 6.2011 | 2.4698 | 4.6530 | | 1.8609 | 6.9604 | 6.7012 | H9 | 2.9951 | 2.1492 | 4.5988 | 1.0938 | 5.7511 | 3.1220 | 4.8018 | 1.8609 | | 6.7012 | 5.9547 | H10 | 3.7763 | 4.8803 | 2.1206 | 6.2011 | 1.0925 | 4.6530 | 2.4698 | 6.9604 | 6.7012 | | 1.8609 | H11 | 2.9951 | 4.5988 | 2.1492 | 5.7511 | 1.0938 | 4.8018 | 3.1220 | 6.7012 | 5.9547 | 1.8609 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
C2 |
C4 |
124.027 |
|
S1 |
C2 |
H6 |
114.619 |
S1 |
C3 |
C5 |
124.027 |
|
S1 |
C3 |
H7 |
114.619 |
C2 |
S1 |
C3 |
102.132 |
|
C2 |
C4 |
H8 |
120.309 |
C2 |
C4 |
H9 |
122.989 |
|
C3 |
C5 |
H10 |
120.309 |
C3 |
C5 |
H11 |
122.989 |
|
C4 |
C2 |
H6 |
121.324 |
C5 |
C3 |
H7 |
121.324 |
|
H8 |
C4 |
H9 |
116.679 |
H10 |
C5 |
H11 |
116.679 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.203 |
|
|
|
2 |
C |
-0.211 |
|
|
|
3 |
C |
-0.211 |
|
|
|
4 |
C |
-0.306 |
|
|
|
5 |
C |
-0.306 |
|
|
|
6 |
H |
0.143 |
|
|
|
7 |
H |
0.143 |
|
|
|
8 |
H |
0.136 |
|
|
|
9 |
H |
0.137 |
|
|
|
10 |
H |
0.136 |
|
|
|
11 |
H |
0.137 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-1.147 |
1.147 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-41.639 |
-0.001 |
0.000 |
y |
-0.001 |
-33.378 |
0.000 |
z |
0.000 |
0.000 |
-35.044 |
|
Traceless |
| x | y | z |
x |
-7.428 |
-0.001 |
0.000 |
y |
-0.001 |
4.963 |
0.000 |
z |
0.000 |
0.000 |
2.464 |
|
Polar |
3z2-r2 | 4.929 |
x2-y2 | -8.261 |
xy | -0.001 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.751 |
-0.005 |
0.000 |
y |
-0.005 |
17.044 |
0.000 |
z |
0.000 |
0.000 |
7.765 |
<r2> (average value of r
2) Å
2
<r2> |
193.511 |
(<r2>)1/2 |
13.911 |
Jump to
S1C1
Energy calculated at BLYP/6-31G*
| hartrees |
Energy at 0K | -554.066751 |
Energy at 298.15K | -554.071995 |
HF Energy | -554.066751 |
Nuclear repulsion energy | 199.132811 |
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 BLYP/6-31G*
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 |
3170 |
3145 |
11.55 |
|
|
|
2 |
A |
3167 |
3141 |
9.06 |
|
|
|
3 |
A |
3104 |
3078 |
6.15 |
|
|
|
4 |
A |
3095 |
3070 |
8.48 |
|
|
|
5 |
A |
3089 |
3064 |
2.45 |
|
|
|
6 |
A |
3082 |
3058 |
3.67 |
|
|
|
7 |
A |
1615 |
1602 |
40.46 |
|
|
|
8 |
A |
1605 |
1592 |
25.76 |
|
|
|
9 |
A |
1401 |
1390 |
4.81 |
|
|
|
10 |
A |
1398 |
1386 |
9.40 |
|
|
|
11 |
A |
1282 |
1271 |
2.49 |
|
|
|
12 |
A |
1268 |
1257 |
10.66 |
|
|
|
13 |
A |
1038 |
1029 |
12.86 |
|
|
|
14 |
A |
1012 |
1004 |
7.26 |
|
|
|
15 |
A |
966 |
959 |
24.26 |
|
|
|
16 |
A |
951 |
943 |
33.91 |
|
|
|
17 |
A |
872 |
865 |
27.92 |
|
|
|
18 |
A |
838 |
831 |
32.53 |
|
|
|
19 |
A |
698 |
692 |
15.00 |
|
|
|
20 |
A |
653 |
648 |
4.75 |
|
|
|
21 |
A |
600 |
595 |
11.29 |
|
|
|
22 |
A |
582 |
577 |
10.63 |
|
|
|
23 |
A |
450 |
447 |
0.60 |
|
|
|
24 |
A |
354 |
351 |
0.51 |
|
|
|
25 |
A |
207 |
205 |
0.97 |
|
|
|
26 |
A |
145 |
144 |
4.33 |
|
|
|
27 |
A |
91 |
90 |
1.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18365.0 cm
-1
Scaled (by 0.9919) Zero Point Vibrational Energy (zpe) 18216.3 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 BLYP/6-31G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.027 |
-0.971 |
0.003 |
C2 |
1.104 |
0.418 |
0.333 |
C3 |
-1.596 |
-0.219 |
-0.007 |
C4 |
2.334 |
0.539 |
-0.197 |
C5 |
-1.908 |
1.085 |
-0.137 |
H6 |
0.719 |
1.127 |
1.075 |
H7 |
-2.374 |
-0.979 |
0.119 |
H8 |
3.001 |
1.343 |
0.127 |
H9 |
2.722 |
-0.159 |
-0.945 |
H10 |
-1.156 |
1.862 |
-0.294 |
H11 |
-2.952 |
1.404 |
-0.093 |
Atom - Atom Distances (Å)
|
S1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
S1 | | 1.7878 | 1.7886 | 2.7643 | 2.8264 | 2.4549 | 2.4042 | 3.7699 | 2.9696 | 3.0843 | 3.8117 |
C2 | 1.7878 | | 2.7941 | 1.3457 | 3.1199 | 1.0957 | 3.7538 | 2.1210 | 2.1411 | 2.7541 | 4.1959 | C3 | 1.7886 | 2.7941 | | 4.0069 | 1.3466 | 2.8877 | 1.0952 | 4.8567 | 4.4184 | 2.1459 | 2.1173 | C4 | 2.7643 | 1.3457 | 4.0069 | | 4.2777 | 2.1388 | 4.9572 | 1.0938 | 1.0934 | 3.7344 | 5.3583 | C5 | 2.8264 | 3.1199 | 1.3466 | 4.2777 | | 2.8933 | 2.1308 | 4.9228 | 4.8610 | 1.0925 | 1.0934 | H6 | 2.4549 | 1.0957 | 2.8877 | 2.1388 | 2.8933 | | 3.8618 | 2.4807 | 3.1215 | 2.4355 | 3.8626 | H7 | 2.4042 | 3.7538 | 1.0952 | 4.9572 | 2.1308 | 3.8618 | | 5.8552 | 5.2699 | 3.1181 | 2.4613 | H8 | 3.7699 | 2.1210 | 4.8567 | 1.0938 | 4.9228 | 2.4807 | 5.8552 | | 1.8661 | 4.2108 | 5.9580 | H9 | 2.9696 | 2.1411 | 4.4184 | 1.0934 | 4.8610 | 3.1215 | 5.2699 | 1.8661 | | 4.4209 | 5.9468 | H10 | 3.0843 | 2.7541 | 2.1459 | 3.7344 | 1.0925 | 2.4355 | 3.1181 | 4.2108 | 4.4209 | | 1.8644 | H11 | 3.8117 | 4.1959 | 2.1173 | 5.3583 | 1.0934 | 3.8626 | 2.4613 | 5.9580 | 5.9468 | 1.8644 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
C2 |
C4 |
123.202 |
|
S1 |
C2 |
H6 |
114.583 |
S1 |
C3 |
C5 |
128.156 |
|
S1 |
C3 |
H7 |
110.650 |
C2 |
S1 |
C3 |
102.753 |
|
C2 |
C4 |
H8 |
120.434 |
C2 |
C4 |
H9 |
122.432 |
|
C3 |
C5 |
H10 |
122.893 |
C3 |
C5 |
H11 |
120.041 |
|
C4 |
C2 |
H6 |
122.004 |
C5 |
C3 |
H7 |
121.193 |
|
H8 |
C4 |
H9 |
117.123 |
H10 |
C5 |
H11 |
117.065 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.170 |
|
|
|
2 |
C |
-0.216 |
|
|
|
3 |
C |
-0.225 |
|
|
|
4 |
C |
-0.284 |
|
|
|
5 |
C |
-0.295 |
|
|
|
6 |
H |
0.152 |
|
|
|
7 |
H |
0.149 |
|
|
|
8 |
H |
0.137 |
|
|
|
9 |
H |
0.143 |
|
|
|
10 |
H |
0.136 |
|
|
|
11 |
H |
0.134 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.094 |
0.938 |
0.230 |
0.970 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.838 |
1.461 |
-0.693 |
y |
1.461 |
-36.970 |
1.049 |
z |
-0.693 |
1.049 |
-40.086 |
|
Traceless |
| x | y | z |
x |
5.690 |
1.461 |
-0.693 |
y |
1.461 |
-0.507 |
1.049 |
z |
-0.693 |
1.049 |
-5.182 |
|
Polar |
3z2-r2 | -10.365 |
x2-y2 | 4.132 |
xy | 1.461 |
xz | -0.693 |
yz | 1.049 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
13.583 |
-0.008 |
-0.742 |
y |
-0.008 |
9.075 |
0.273 |
z |
-0.742 |
0.273 |
4.750 |
<r2> (average value of r
2) Å
2
<r2> |
170.526 |
(<r2>)1/2 |
13.059 |