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Vibrational Frequencies calculated at HF/6-311+G(3df,2p)
Geometric Data calculated at HF/6-311+G(3df,2p)
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C3
Vibrational Frequencies calculated at HF/6-311+G(3df,2p)
Geometric Data calculated at HF/6-311+G(3df,2p)
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C2
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -266.892724 |
| Energy at 298.15K | -266.901217 |
| Nuclear repulsion energy | 196.856655 |
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 HF/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 |
3257 |
2960 |
41.84 |
|
|
|
| 2 |
A |
3238 |
2942 |
52.98 |
|
|
|
| 3 |
A |
3228 |
2933 |
57.66 |
|
|
|
| 4 |
A |
3177 |
2887 |
56.66 |
|
|
|
| 5 |
A |
3150 |
2862 |
70.20 |
|
|
|
| 6 |
A |
3139 |
2852 |
108.11 |
|
|
|
| 7 |
A |
1692 |
1537 |
3.71 |
|
|
|
| 8 |
A |
1659 |
1508 |
1.05 |
|
|
|
| 9 |
A |
1645 |
1495 |
2.95 |
|
|
|
| 10 |
A |
1574 |
1430 |
12.10 |
|
|
|
| 11 |
A |
1519 |
1380 |
2.68 |
|
|
|
| 12 |
A |
1482 |
1347 |
2.12 |
|
|
|
| 13 |
A |
1381 |
1255 |
9.10 |
|
|
|
| 14 |
A |
1351 |
1228 |
21.86 |
|
|
|
| 15 |
A |
1325 |
1204 |
68.33 |
|
|
|
| 16 |
A |
1306 |
1186 |
127.59 |
|
|
|
| 17 |
A |
1264 |
1148 |
30.48 |
|
|
|
| 18 |
A |
1246 |
1132 |
97.99 |
|
|
|
| 19 |
A |
1206 |
1096 |
54.04 |
|
|
|
| 20 |
A |
1078 |
980 |
31.32 |
|
|
|
| 21 |
A |
1056 |
960 |
52.27 |
|
|
|
| 22 |
A |
1021 |
928 |
11.14 |
|
|
|
| 23 |
A |
962 |
874 |
13.28 |
|
|
|
| 24 |
A |
808 |
734 |
0.42 |
|
|
|
| 25 |
A |
722 |
656 |
5.95 |
|
|
|
| 26 |
A |
257 |
234 |
7.48 |
|
|
|
| 27 |
A |
68 |
62 |
11.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21906.2 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 19904.0 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 HF/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.183 |
-0.053 |
0.088 |
| C2 |
-0.999 |
-0.688 |
-0.101 |
| C3 |
-0.872 |
0.806 |
0.167 |
| O4 |
0.322 |
-1.146 |
0.025 |
| O5 |
0.440 |
1.068 |
-0.238 |
| H6 |
1.587 |
0.030 |
1.095 |
| H7 |
1.987 |
-0.164 |
-0.626 |
| H8 |
-1.360 |
-0.886 |
-1.104 |
| H9 |
-0.998 |
1.035 |
1.222 |
| H10 |
-1.549 |
1.415 |
-0.412 |
| H11 |
-1.633 |
-1.199 |
0.611 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
O5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 2.2807 | 2.2287 | 1.3938 | 1.3838 | 1.0876 | 1.0804 | 2.9298 | 2.6883 | 3.1419 | 3.0849 |
C2 | 2.2807 | | 1.5231 | 1.4038 | 2.2745 | 2.9381 | 3.0763 | 1.0838 | 2.1720 | 2.1959 | 1.0814 | C3 | 2.2287 | 1.5231 | | 2.2929 | 1.3978 | 2.7401 | 3.1211 | 2.1713 | 1.0869 | 1.0792 | 2.1900 | O4 | 1.3938 | 1.4038 | 2.2929 | | 2.2332 | 2.0322 | 2.0394 | 2.0421 | 2.8166 | 3.2021 | 2.0411 | O5 | 1.3838 | 2.2745 | 1.3978 | 2.2332 | | 2.0417 | 2.0152 | 2.7942 | 2.0499 | 2.0270 | 3.1869 | H6 | 1.0876 | 2.9381 | 2.7401 | 2.0322 | 2.0417 | | 1.7768 | 3.7891 | 2.7764 | 3.7448 | 3.4800 | H7 | 1.0804 | 3.0763 | 3.1211 | 2.0394 | 2.0152 | 1.7768 | | 3.4571 | 3.7096 | 3.8788 | 3.9622 | H8 | 2.9298 | 1.0838 | 2.1713 | 2.0421 | 2.7942 | 3.7891 | 3.4571 | | 3.0376 | 2.4100 | 1.7639 | H9 | 2.6883 | 2.1720 | 1.0869 | 2.8166 | 2.0499 | 2.7764 | 3.7096 | 3.0376 | | 1.7655 | 2.4010 | H10 | 3.1419 | 2.1959 | 1.0792 | 3.2021 | 2.0270 | 3.7448 | 3.8788 | 2.4100 | 1.7655 | | 2.8081 | H11 | 3.0849 | 1.0814 | 2.1900 | 2.0411 | 3.1869 | 3.4800 | 3.9622 | 1.7639 | 2.4010 | 2.8081 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O4 |
C2 |
109.226 |
|
C1 |
O5 |
C3 |
106.496 |
| C2 |
C3 |
O5 |
102.193 |
|
C2 |
C3 |
H9 |
111.551 |
| C2 |
C3 |
H10 |
114.003 |
|
C3 |
C2 |
O4 |
103.068 |
| C3 |
C2 |
H8 |
111.688 |
|
C3 |
C2 |
H11 |
113.368 |
| O4 |
C1 |
O5 |
107.032 |
|
O4 |
C1 |
H6 |
109.348 |
| O4 |
C1 |
H7 |
110.388 |
|
O4 |
C2 |
H8 |
109.688 |
| O4 |
C2 |
H11 |
109.754 |
|
O5 |
C1 |
H6 |
110.845 |
| O5 |
C1 |
H7 |
109.110 |
|
O5 |
C3 |
H9 |
110.549 |
| O5 |
C3 |
H10 |
109.158 |
|
H6 |
C1 |
H7 |
110.074 |
| H8 |
C2 |
H11 |
109.106 |
|
H9 |
C3 |
H10 |
109.188 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.684 |
|
|
|
| 2 |
C |
0.325 |
|
|
|
| 3 |
C |
0.086 |
|
|
|
| 4 |
O |
-0.895 |
|
|
|
| 5 |
O |
-0.869 |
|
|
|
| 6 |
H |
0.091 |
|
|
|
| 7 |
H |
0.108 |
|
|
|
| 8 |
H |
0.114 |
|
|
|
| 9 |
H |
0.118 |
|
|
|
| 10 |
H |
0.123 |
|
|
|
| 11 |
H |
0.115 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.252 |
0.281 |
0.552 |
1.397 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.970 |
-0.493 |
0.304 |
| y |
-0.493 |
-34.728 |
0.909 |
| z |
0.304 |
0.909 |
-29.473 |
|
| Traceless |
| | x | y | z |
| x |
6.130 |
-0.493 |
0.304 |
| y |
-0.493 |
-7.007 |
0.909 |
| z |
0.304 |
0.909 |
0.876 |
|
| Polar |
| 3z2-r2 | 1.753 |
| x2-y2 | 8.758 |
| xy | -0.493 |
| xz | 0.304 |
| yz | 0.909 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.584 |
-0.035 |
0.039 |
| y |
-0.035 |
5.618 |
0.072 |
| z |
0.039 |
0.072 |
5.331 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |