Jump to
S1C2
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -194.358643 |
| Energy at 298.15K | -194.367579 |
| Nuclear repulsion energy | 130.809960 |
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 mPW1PW91/6-311G**
| 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' |
3909 |
3739 |
28.78 |
|
|
|
| 2 |
A' |
3131 |
2996 |
33.53 |
|
|
|
| 3 |
A' |
3062 |
2929 |
31.41 |
|
|
|
| 4 |
A' |
3049 |
2917 |
26.58 |
|
|
|
| 5 |
A' |
2984 |
2854 |
62.84 |
|
|
|
| 6 |
A' |
1532 |
1466 |
4.52 |
|
|
|
| 7 |
A' |
1511 |
1446 |
5.66 |
|
|
|
| 8 |
A' |
1497 |
1432 |
0.81 |
|
|
|
| 9 |
A' |
1469 |
1406 |
1.81 |
|
|
|
| 10 |
A' |
1415 |
1354 |
1.81 |
|
|
|
| 11 |
A' |
1354 |
1296 |
11.10 |
|
|
|
| 12 |
A' |
1272 |
1217 |
54.38 |
|
|
|
| 13 |
A' |
1117 |
1068 |
23.64 |
|
|
|
| 14 |
A' |
1088 |
1041 |
69.84 |
|
|
|
| 15 |
A' |
1062 |
1016 |
12.54 |
|
|
|
| 16 |
A' |
899 |
860 |
6.43 |
|
|
|
| 17 |
A' |
462 |
442 |
10.91 |
|
|
|
| 18 |
A' |
271 |
259 |
4.03 |
|
|
|
| 19 |
A" |
3123 |
2987 |
70.16 |
|
|
|
| 20 |
A" |
3097 |
2963 |
2.54 |
|
|
|
| 21 |
A" |
3014 |
2884 |
55.86 |
|
|
|
| 22 |
A" |
1502 |
1437 |
8.76 |
|
|
|
| 23 |
A" |
1326 |
1269 |
0.10 |
|
|
|
| 24 |
A" |
1273 |
1218 |
0.13 |
|
|
|
| 25 |
A" |
1190 |
1139 |
1.32 |
|
|
|
| 26 |
A" |
905 |
866 |
3.08 |
|
|
|
| 27 |
A" |
774 |
740 |
1.18 |
|
|
|
| 28 |
A" |
278 |
266 |
119.44 |
|
|
|
| 29 |
A" |
231 |
221 |
3.26 |
|
|
|
| 30 |
A" |
128 |
122 |
4.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 23961.0 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 22923.5 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 mPW1PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.440 |
1.231 |
0.000 |
| C2 |
0.000 |
0.736 |
0.000 |
| C3 |
0.097 |
-0.775 |
0.000 |
| O4 |
1.467 |
-1.128 |
0.000 |
| H5 |
-1.481 |
2.321 |
0.000 |
| H6 |
-1.982 |
0.880 |
0.882 |
| H7 |
-1.982 |
0.880 |
-0.882 |
| H8 |
0.534 |
1.113 |
0.877 |
| H9 |
0.534 |
1.113 |
-0.877 |
| H10 |
-0.416 |
-1.175 |
0.887 |
| H11 |
-0.416 |
-1.175 |
-0.887 |
| H12 |
1.528 |
-2.084 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
H12 |
| C1 | | 1.5223 | 2.5264 | 3.7437 | 1.0914 | 1.0935 | 1.0935 | 2.1625 | 2.1625 | 2.7613 | 2.7613 | 4.4486 |
C2 | 1.5223 | | 1.5135 | 2.3725 | 2.1699 | 2.1745 | 2.1745 | 1.0938 | 1.0938 | 2.1477 | 2.1477 | 3.2068 | C3 | 2.5264 | 1.5135 | | 1.4151 | 3.4751 | 2.8001 | 2.8001 | 2.1270 | 2.1270 | 1.1001 | 1.1001 | 1.9392 | O4 | 3.7437 | 2.3725 | 1.4151 | | 4.5383 | 4.0881 | 4.0881 | 2.5821 | 2.5821 | 2.0818 | 2.0818 | 0.9572 | H5 | 1.0914 | 2.1699 | 3.4751 | 4.5383 | | 1.7623 | 1.7623 | 2.5077 | 2.5077 | 3.7617 | 3.7617 | 5.3348 | H6 | 1.0935 | 2.1745 | 2.8001 | 4.0881 | 1.7623 | | 1.7647 | 2.5265 | 3.0788 | 2.5846 | 3.1322 | 4.6779 | H7 | 1.0935 | 2.1745 | 2.8001 | 4.0881 | 1.7623 | 1.7647 | | 3.0788 | 2.5265 | 3.1322 | 2.5846 | 4.6779 | H8 | 2.1625 | 1.0938 | 2.1270 | 2.5821 | 2.5077 | 2.5265 | 3.0788 | | 1.7541 | 2.4779 | 3.0416 | 3.4611 | H9 | 2.1625 | 1.0938 | 2.1270 | 2.5821 | 2.5077 | 3.0788 | 2.5265 | 1.7541 | | 3.0416 | 2.4779 | 3.4611 | H10 | 2.7613 | 2.1477 | 1.1001 | 2.0818 | 3.7617 | 2.5846 | 3.1322 | 2.4779 | 3.0416 | | 1.7737 | 2.3212 | H11 | 2.7613 | 2.1477 | 1.1001 | 2.0818 | 3.7617 | 3.1322 | 2.5846 | 3.0416 | 2.4779 | 1.7737 | | 2.3212 | H12 | 4.4486 | 3.2068 | 1.9392 | 0.9572 | 5.3348 | 4.6779 | 4.6779 | 3.4611 | 3.4611 | 2.3212 | 2.3212 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
112.648 |
|
C1 |
C2 |
H8 |
110.430 |
| C1 |
C2 |
H9 |
110.430 |
|
C2 |
C1 |
H5 |
111.170 |
| C2 |
C1 |
H6 |
111.414 |
|
C2 |
C1 |
H7 |
111.414 |
| C2 |
C3 |
O4 |
108.162 |
|
C2 |
C3 |
H10 |
109.498 |
| C2 |
C3 |
H11 |
109.498 |
|
C3 |
C2 |
H8 |
108.252 |
| C3 |
C2 |
H9 |
108.252 |
|
C3 |
O4 |
H12 |
108.101 |
| O4 |
C3 |
H10 |
111.110 |
|
O4 |
C3 |
H11 |
111.110 |
| H5 |
C1 |
H6 |
107.526 |
|
H5 |
C1 |
H7 |
107.526 |
| H6 |
C1 |
H7 |
107.590 |
|
H8 |
C2 |
H9 |
106.609 |
| H10 |
C3 |
H11 |
107.447 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.346 |
|
|
|
| 2 |
C |
-0.292 |
|
|
|
| 3 |
C |
-0.014 |
|
|
|
| 4 |
O |
-0.407 |
|
|
|
| 5 |
H |
0.127 |
|
|
|
| 6 |
H |
0.117 |
|
|
|
| 7 |
H |
0.117 |
|
|
|
| 8 |
H |
0.132 |
|
|
|
| 9 |
H |
0.132 |
|
|
|
| 10 |
H |
0.097 |
|
|
|
| 11 |
H |
0.097 |
|
|
|
| 12 |
H |
0.240 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.104 |
-1.030 |
0.000 |
1.509 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.325 |
-1.053 |
0.000 |
| y |
-1.053 |
-21.715 |
0.000 |
| z |
0.000 |
0.000 |
-26.473 |
|
| Traceless |
| | x | y | z |
| x |
-5.231 |
-1.053 |
0.000 |
| y |
-1.053 |
6.184 |
0.000 |
| z |
0.000 |
0.000 |
-0.953 |
|
| Polar |
| 3z2-r2 | -1.906 |
| x2-y2 | -7.610 |
| xy | -1.053 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.099 |
-0.532 |
0.000 |
| y |
-0.532 |
6.284 |
0.000 |
| z |
0.000 |
0.000 |
5.238 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -194.358993 |
| Energy at 298.15K | |
| HF Energy | -194.358993 |
| Nuclear repulsion energy | 133.110008 |
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 mPW1PW91/6-311G**
| 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 |
3911 |
3742 |
31.70 |
102.56 |
0.30 |
0.46 |
| 2 |
A |
3147 |
3010 |
25.02 |
41.23 |
0.75 |
0.86 |
| 3 |
A |
3122 |
2987 |
49.79 |
58.33 |
0.59 |
0.74 |
| 4 |
A |
3091 |
2958 |
20.95 |
94.50 |
0.72 |
0.84 |
| 5 |
A |
3055 |
2922 |
44.31 |
139.63 |
0.06 |
0.11 |
| 6 |
A |
3052 |
2920 |
32.52 |
112.14 |
0.04 |
0.07 |
| 7 |
A |
3021 |
2890 |
50.99 |
94.93 |
0.75 |
0.86 |
| 8 |
A |
2986 |
2857 |
67.44 |
116.84 |
0.11 |
0.20 |
| 9 |
A |
1527 |
1460 |
3.11 |
5.63 |
0.68 |
0.81 |
| 10 |
A |
1513 |
1447 |
8.45 |
6.02 |
0.75 |
0.86 |
| 11 |
A |
1497 |
1432 |
8.64 |
13.80 |
0.75 |
0.86 |
| 12 |
A |
1478 |
1414 |
3.60 |
12.02 |
0.73 |
0.84 |
| 13 |
A |
1462 |
1399 |
1.89 |
1.82 |
0.18 |
0.30 |
| 14 |
A |
1414 |
1353 |
5.54 |
1.31 |
0.71 |
0.83 |
| 15 |
A |
1382 |
1322 |
0.76 |
1.24 |
0.73 |
0.84 |
| 16 |
A |
1333 |
1275 |
24.12 |
11.05 |
0.74 |
0.85 |
| 17 |
A |
1281 |
1225 |
1.72 |
7.09 |
0.74 |
0.85 |
| 18 |
A |
1256 |
1202 |
37.92 |
2.97 |
0.54 |
0.70 |
| 19 |
A |
1167 |
1116 |
7.26 |
0.59 |
0.19 |
0.32 |
| 20 |
A |
1139 |
1090 |
18.46 |
3.96 |
0.59 |
0.74 |
| 21 |
A |
1085 |
1038 |
38.04 |
2.61 |
0.70 |
0.82 |
| 22 |
A |
1002 |
959 |
43.14 |
3.76 |
0.75 |
0.86 |
| 23 |
A |
931 |
891 |
2.55 |
0.23 |
0.67 |
0.80 |
| 24 |
A |
882 |
844 |
2.49 |
9.08 |
0.16 |
0.27 |
| 25 |
A |
778 |
744 |
0.71 |
0.45 |
0.62 |
0.77 |
| 26 |
A |
480 |
460 |
8.45 |
0.21 |
0.48 |
0.65 |
| 27 |
A |
329 |
314 |
8.22 |
0.32 |
0.44 |
0.61 |
| 28 |
A |
255 |
244 |
113.33 |
3.52 |
0.74 |
0.85 |
| 29 |
A |
225 |
216 |
2.04 |
0.08 |
0.56 |
0.72 |
| 30 |
A |
151 |
144 |
6.85 |
0.14 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 23975.2 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 22937.1 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 mPW1PW91/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.532 |
-0.513 |
0.128 |
| C2 |
-0.630 |
0.641 |
-0.286 |
| C3 |
0.767 |
0.541 |
0.291 |
| O4 |
1.374 |
-0.633 |
-0.219 |
| H5 |
-2.517 |
-0.435 |
-0.338 |
| H6 |
-1.677 |
-0.530 |
1.212 |
| H7 |
-1.090 |
-1.466 |
-0.165 |
| H8 |
-0.546 |
0.677 |
-1.377 |
| H9 |
-1.065 |
1.596 |
0.028 |
| H10 |
0.708 |
0.508 |
1.389 |
| H11 |
1.345 |
1.433 |
0.014 |
| H12 |
2.230 |
-0.731 |
0.196 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
H12 |
| C1 | | 1.5225 | 2.5346 | 2.9290 | 1.0920 | 1.0939 | 1.0905 | 2.1578 | 2.1627 | 2.7671 | 3.4759 | 3.7694 |
C2 | 1.5225 | | 1.5150 | 2.3756 | 2.1723 | 2.1708 | 2.1603 | 1.0945 | 1.0950 | 2.1490 | 2.1494 | 3.2091 | C3 | 2.5346 | 1.5150 | | 1.4163 | 3.4827 | 2.8229 | 2.7720 | 2.1267 | 2.1295 | 1.1003 | 1.0989 | 1.9413 | O4 | 2.9290 | 2.3756 | 1.4163 | | 3.8973 | 3.3714 | 2.6013 | 2.5963 | 3.3124 | 2.0811 | 2.0792 | 0.9570 | H5 | 1.0920 | 2.1723 | 3.4827 | 3.8973 | | 1.7654 | 1.7691 | 2.4903 | 2.5233 | 3.7784 | 4.3044 | 4.7861 | H6 | 1.0939 | 2.1708 | 2.8229 | 3.3714 | 1.7654 | | 1.7657 | 3.0726 | 2.5090 | 2.6081 | 3.7980 | 4.0423 | H7 | 1.0905 | 2.1603 | 2.7720 | 2.6013 | 1.7691 | 1.7657 | | 2.5220 | 3.0682 | 3.0902 | 3.7905 | 3.4197 | H8 | 2.1578 | 1.0945 | 2.1267 | 2.5963 | 2.4903 | 3.0726 | 2.5220 | | 1.7572 | 3.0420 | 2.4658 | 3.4876 | H9 | 2.1627 | 1.0950 | 2.1295 | 3.3124 | 2.5233 | 2.5090 | 3.0682 | 1.7572 | | 2.4855 | 2.4152 | 4.0369 | H10 | 2.7671 | 2.1490 | 1.1003 | 2.0811 | 3.7784 | 2.6081 | 3.0902 | 3.0420 | 2.4855 | | 1.7756 | 2.2966 | H11 | 3.4759 | 2.1494 | 1.0989 | 2.0792 | 4.3044 | 3.7980 | 3.7905 | 2.4658 | 2.4152 | 1.7756 | | 2.3453 | H12 | 3.7694 | 3.2091 | 1.9413 | 0.9570 | 4.7861 | 4.0423 | 3.4197 | 3.4876 | 4.0369 | 2.2966 | 2.3453 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
113.113 |
|
C1 |
C2 |
H8 |
110.004 |
| C1 |
C2 |
H9 |
110.367 |
|
C2 |
C1 |
H5 |
111.310 |
| C2 |
C1 |
H6 |
111.075 |
|
C2 |
C1 |
H7 |
110.437 |
| C2 |
C3 |
O4 |
108.224 |
|
C2 |
C3 |
H10 |
109.486 |
| C2 |
C3 |
H11 |
109.609 |
|
C3 |
C2 |
H8 |
108.089 |
| C3 |
C2 |
H9 |
108.283 |
|
C3 |
O4 |
H12 |
108.201 |
| O4 |
C3 |
H10 |
110.949 |
|
O4 |
C3 |
H11 |
110.884 |
| H5 |
C1 |
H6 |
107.732 |
|
H5 |
C1 |
H7 |
108.300 |
| H6 |
C1 |
H7 |
107.857 |
|
H8 |
C2 |
H9 |
106.754 |
| H10 |
C3 |
H11 |
107.679 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.335 |
|
|
|
| 2 |
C |
-0.293 |
|
|
|
| 3 |
C |
-0.034 |
|
|
|
| 4 |
O |
-0.406 |
|
|
|
| 5 |
H |
0.119 |
|
|
|
| 6 |
H |
0.110 |
|
|
|
| 7 |
H |
0.139 |
|
|
|
| 8 |
H |
0.133 |
|
|
|
| 9 |
H |
0.119 |
|
|
|
| 10 |
H |
0.099 |
|
|
|
| 11 |
H |
0.106 |
|
|
|
| 12 |
H |
0.242 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.785 |
0.873 |
1.017 |
1.554 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.712 |
-0.278 |
2.021 |
| y |
-0.278 |
-26.989 |
-0.603 |
| z |
2.021 |
-0.603 |
-26.692 |
|
| Traceless |
| | x | y | z |
| x |
4.128 |
-0.278 |
2.021 |
| y |
-0.278 |
-2.287 |
-0.603 |
| z |
2.021 |
-0.603 |
-1.841 |
|
| Polar |
| 3z2-r2 | -3.683 |
| x2-y2 | 4.277 |
| xy | -0.278 |
| xz | 2.021 |
| yz | -0.603 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.434 |
0.069 |
0.149 |
| y |
0.069 |
5.732 |
-0.006 |
| z |
0.149 |
-0.006 |
5.425 |
<r2> (average value of r
2) Å
2
| <r2> |
94.487 |
| (<r2>)1/2 |
9.720 |