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S1C2
S1C3
Vibrational Frequencies calculated at B1B95/6-31+G**
Geometric Data calculated at B1B95/6-31+G**
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C3
Vibrational Frequencies calculated at B1B95/6-31+G**
Geometric Data calculated at B1B95/6-31+G**
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -268.253446 |
| Energy at 298.15K | -268.261704 |
| Nuclear repulsion energy | 195.052681 |
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 B1B95/6-31+G**
| 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 |
3158 |
3021 |
21.08 |
|
|
|
| 2 |
A |
3120 |
2985 |
26.19 |
|
|
|
| 3 |
A |
3117 |
2982 |
51.03 |
|
|
|
| 4 |
A |
3055 |
2923 |
55.75 |
|
|
|
| 5 |
A |
3025 |
2894 |
50.62 |
|
|
|
| 6 |
A |
2992 |
2862 |
109.10 |
|
|
|
| 7 |
A |
1547 |
1480 |
2.11 |
|
|
|
| 8 |
A |
1523 |
1457 |
1.36 |
|
|
|
| 9 |
A |
1506 |
1440 |
3.24 |
|
|
|
| 10 |
A |
1426 |
1364 |
10.28 |
|
|
|
| 11 |
A |
1383 |
1323 |
2.07 |
|
|
|
| 12 |
A |
1345 |
1287 |
1.01 |
|
|
|
| 13 |
A |
1271 |
1215 |
8.20 |
|
|
|
| 14 |
A |
1240 |
1186 |
14.47 |
|
|
|
| 15 |
A |
1204 |
1151 |
80.35 |
|
|
|
| 16 |
A |
1186 |
1134 |
57.53 |
|
|
|
| 17 |
A |
1154 |
1104 |
39.13 |
|
|
|
| 18 |
A |
1135 |
1086 |
52.93 |
|
|
|
| 19 |
A |
1090 |
1043 |
36.18 |
|
|
|
| 20 |
A |
1005 |
961 |
33.87 |
|
|
|
| 21 |
A |
973 |
931 |
36.62 |
|
|
|
| 22 |
A |
959 |
917 |
35.30 |
|
|
|
| 23 |
A |
896 |
857 |
18.11 |
|
|
|
| 24 |
A |
734 |
702 |
0.28 |
|
|
|
| 25 |
A |
650 |
622 |
4.98 |
|
|
|
| 26 |
A |
277 |
265 |
7.75 |
|
|
|
| 27 |
A |
47 |
45 |
10.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20507.6 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 19617.5 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 B1B95/6-31+G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.182 |
-0.083 |
0.101 |
| C2 |
-1.027 |
-0.650 |
-0.118 |
| C3 |
-0.843 |
0.828 |
0.195 |
| O4 |
0.286 |
-1.177 |
0.026 |
| O5 |
0.473 |
1.065 |
-0.273 |
| H6 |
1.554 |
0.003 |
1.135 |
| H7 |
2.012 |
-0.224 |
-0.596 |
| H8 |
-1.377 |
-0.804 |
-1.145 |
| H9 |
-0.909 |
1.021 |
1.275 |
| H10 |
-1.525 |
1.491 |
-0.337 |
| H11 |
-1.700 |
-1.161 |
0.575 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
O5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 2.2916 | 2.2231 | 1.4162 | 1.4007 | 1.1015 | 1.0924 | 2.9364 | 2.6404 | 3.1620 | 3.1132 |
C2 | 2.2916 | | 1.5220 | 1.4226 | 2.2845 | 2.9427 | 3.1057 | 1.0957 | 2.1791 | 2.2091 | 1.0927 | C3 | 2.2231 | 1.5220 | | 2.3077 | 1.4176 | 2.7036 | 3.1436 | 2.1782 | 1.0991 | 1.0897 | 2.1987 | O4 | 1.4162 | 1.4226 | 2.3077 | | 2.2701 | 2.0570 | 2.0669 | 2.0677 | 2.7972 | 3.2451 | 2.0607 | O5 | 1.4007 | 2.2845 | 1.4176 | 2.2701 | | 2.0681 | 2.0327 | 2.7710 | 2.0762 | 2.0439 | 3.2248 | H6 | 1.1015 | 2.9427 | 2.7036 | 2.0570 | 2.0681 | | 1.8040 | 3.7999 | 2.6689 | 3.7226 | 3.5008 | H7 | 1.0924 | 3.1057 | 3.1436 | 2.0669 | 2.0327 | 1.8040 | | 3.4816 | 3.6852 | 3.9386 | 4.0030 | H8 | 2.9364 | 1.0957 | 2.1782 | 2.0677 | 2.7710 | 3.7999 | 3.4816 | | 3.0673 | 2.4377 | 1.7863 | H9 | 2.6404 | 2.1791 | 1.0991 | 2.7972 | 2.0762 | 2.6689 | 3.6852 | 3.0673 | | 1.7888 | 2.4244 | H10 | 3.1620 | 2.2091 | 1.0897 | 3.2451 | 2.0439 | 3.7226 | 3.9386 | 2.4377 | 1.7888 | | 2.8104 | H11 | 3.1132 | 1.0927 | 2.1987 | 2.0607 | 3.2248 | 3.5008 | 4.0030 | 1.7863 | 2.4244 | 2.8104 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O4 |
C2 |
107.660 |
|
C1 |
O5 |
C3 |
104.148 |
| C2 |
C3 |
O5 |
101.940 |
|
C2 |
C3 |
H9 |
111.457 |
| C2 |
C3 |
H10 |
114.510 |
|
C3 |
C2 |
O4 |
103.148 |
| C3 |
C2 |
H8 |
111.590 |
|
C3 |
C2 |
H11 |
113.453 |
| O4 |
C1 |
O5 |
107.392 |
|
O4 |
C1 |
H6 |
108.941 |
| O4 |
C1 |
H7 |
110.294 |
|
O4 |
C2 |
H8 |
109.699 |
| O4 |
C2 |
H11 |
109.323 |
|
O5 |
C1 |
H6 |
110.926 |
| O5 |
C1 |
H7 |
108.608 |
|
O5 |
C3 |
H9 |
110.536 |
| O5 |
C3 |
H10 |
108.501 |
|
H6 |
C1 |
H7 |
110.627 |
| H8 |
C2 |
H11 |
109.424 |
|
H9 |
C3 |
H10 |
109.614 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.075 |
|
|
|
| 2 |
C |
-0.103 |
|
|
|
| 3 |
C |
-0.129 |
|
|
|
| 4 |
O |
-0.387 |
|
|
|
| 5 |
O |
-0.356 |
|
|
|
| 6 |
H |
0.132 |
|
|
|
| 7 |
H |
0.146 |
|
|
|
| 8 |
H |
0.153 |
|
|
|
| 9 |
H |
0.151 |
|
|
|
| 10 |
H |
0.164 |
|
|
|
| 11 |
H |
0.153 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.275 |
0.417 |
0.613 |
1.475 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.888 |
-0.805 |
0.315 |
| y |
-0.805 |
-34.927 |
0.996 |
| z |
0.315 |
0.996 |
-29.861 |
|
| Traceless |
| | x | y | z |
| x |
6.507 |
-0.805 |
0.315 |
| y |
-0.805 |
-7.053 |
0.996 |
| z |
0.315 |
0.996 |
0.546 |
|
| Polar |
| 3z2-r2 | 1.093 |
| x2-y2 | 9.040 |
| xy | -0.805 |
| xz | 0.315 |
| yz | 0.996 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.873 |
-0.070 |
0.069 |
| y |
-0.070 |
5.768 |
0.081 |
| z |
0.069 |
0.081 |
5.632 |
<r2> (average value of r
2) Å
2
| <r2> |
92.878 |
| (<r2>)1/2 |
9.637 |