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S1C2
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Vibrational Frequencies calculated at B3LYP/LANL2DZ
Geometric Data calculated at B3LYP/LANL2DZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C3
Vibrational Frequencies calculated at B3LYP/LANL2DZ
Geometric Data calculated at B3LYP/LANL2DZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -268.307922 |
| Energy at 298.15K | -268.315971 |
| Nuclear repulsion energy | 189.584498 |
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 B3LYP/LANL2DZ
| 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 |
3176 |
3053 |
40.08 |
|
|
|
| 2 |
A |
3153 |
3031 |
40.02 |
|
|
|
| 3 |
A |
3152 |
3029 |
34.67 |
|
|
|
| 4 |
A |
3078 |
2959 |
49.12 |
|
|
|
| 5 |
A |
3056 |
2938 |
63.46 |
|
|
|
| 6 |
A |
3046 |
2928 |
112.80 |
|
|
|
| 7 |
A |
1543 |
1484 |
1.15 |
|
|
|
| 8 |
A |
1529 |
1470 |
0.87 |
|
|
|
| 9 |
A |
1521 |
1462 |
4.63 |
|
|
|
| 10 |
A |
1403 |
1349 |
0.31 |
|
|
|
| 11 |
A |
1365 |
1312 |
0.63 |
|
|
|
| 12 |
A |
1347 |
1295 |
1.42 |
|
|
|
| 13 |
A |
1234 |
1186 |
7.61 |
|
|
|
| 14 |
A |
1208 |
1161 |
3.77 |
|
|
|
| 15 |
A |
1165 |
1120 |
15.88 |
|
|
|
| 16 |
A |
1150 |
1105 |
5.12 |
|
|
|
| 17 |
A |
1113 |
1070 |
16.56 |
|
|
|
| 18 |
A |
1075 |
1033 |
115.41 |
|
|
|
| 19 |
A |
1015 |
976 |
30.02 |
|
|
|
| 20 |
A |
957 |
920 |
8.79 |
|
|
|
| 21 |
A |
906 |
871 |
32.86 |
|
|
|
| 22 |
A |
891 |
856 |
11.56 |
|
|
|
| 23 |
A |
837 |
805 |
56.08 |
|
|
|
| 24 |
A |
696 |
669 |
0.16 |
|
|
|
| 25 |
A |
645 |
620 |
6.58 |
|
|
|
| 26 |
A |
237 |
228 |
10.37 |
|
|
|
| 27 |
A |
32 |
31 |
24.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20266.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 19479.9 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 B3LYP/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.244 |
-0.041 |
0.080 |
| C2 |
-0.927 |
0.804 |
0.190 |
| C3 |
-1.035 |
-0.702 |
-0.129 |
| O4 |
0.443 |
1.129 |
-0.238 |
| O5 |
0.344 |
-1.200 |
0.048 |
| H6 |
2.018 |
-0.137 |
-0.686 |
| H7 |
1.674 |
0.034 |
1.090 |
| H8 |
-1.046 |
1.002 |
1.265 |
| H9 |
-1.350 |
-0.878 |
-1.165 |
| H10 |
-1.685 |
-1.248 |
0.560 |
| H11 |
-1.606 |
1.433 |
-0.388 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
O5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 2.3319 | 2.3819 | 1.4534 | 1.4677 | 1.0933 | 1.0998 | 2.7817 | 2.9965 | 3.2041 | 3.2424 |
C2 | 2.3319 | | 1.5429 | 1.4714 | 2.3770 | 3.2133 | 2.8572 | 1.0995 | 2.2005 | 2.2187 | 1.0918 | C3 | 2.3819 | 1.5429 | | 2.3555 | 1.4767 | 3.1545 | 3.0598 | 2.2017 | 1.0966 | 1.0940 | 2.2253 | O4 | 1.4534 | 1.4714 | 2.3555 | | 2.3488 | 2.0701 | 2.1158 | 2.1195 | 2.8464 | 3.2889 | 2.0764 | O5 | 1.4677 | 2.3770 | 1.4767 | 2.3488 | | 2.1148 | 2.0917 | 2.8746 | 2.1084 | 2.0932 | 3.3054 | H6 | 1.0933 | 3.2133 | 3.1545 | 2.0701 | 2.1148 | | 1.8168 | 3.8072 | 3.4821 | 4.0623 | 3.9606 | H7 | 1.0998 | 2.8572 | 3.0598 | 2.1158 | 2.0917 | 1.8168 | | 2.8923 | 3.8803 | 3.6336 | 3.8596 | H8 | 2.7817 | 1.0995 | 2.2017 | 2.1195 | 2.8746 | 3.8072 | 2.8923 | | 3.0870 | 2.4430 | 1.7980 | H9 | 2.9965 | 2.2005 | 1.0966 | 2.8464 | 2.1084 | 3.4821 | 3.8803 | 3.0870 | | 1.7961 | 2.4511 | H10 | 3.2041 | 2.2187 | 1.0940 | 3.2889 | 2.0932 | 4.0623 | 3.6336 | 2.4430 | 1.7961 | | 2.8456 | H11 | 3.2424 | 1.0918 | 2.2253 | 2.0764 | 3.3054 | 3.9606 | 3.8596 | 1.7980 | 2.4511 | 2.8456 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O4 |
C2 |
105.745 |
|
C1 |
O5 |
C3 |
107.986 |
| C2 |
C3 |
O5 |
103.823 |
|
C2 |
C3 |
H9 |
111.838 |
| C2 |
C3 |
H10 |
113.480 |
|
C3 |
C2 |
O4 |
102.758 |
| C3 |
C2 |
H8 |
111.765 |
|
C3 |
C2 |
H11 |
114.168 |
| O4 |
C1 |
O5 |
107.042 |
|
O4 |
C1 |
H6 |
107.917 |
| O4 |
C1 |
H7 |
111.171 |
|
O4 |
C2 |
H8 |
110.220 |
| O4 |
C2 |
H11 |
107.282 |
|
O5 |
C1 |
H6 |
110.483 |
| O5 |
C1 |
H7 |
108.260 |
|
O5 |
C3 |
H9 |
109.137 |
| O5 |
C3 |
H10 |
108.099 |
|
H6 |
C1 |
H7 |
111.867 |
| H8 |
C2 |
H11 |
110.274 |
|
H9 |
C3 |
H10 |
110.147 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.113 |
|
|
|
| 2 |
C |
-0.265 |
|
|
|
| 3 |
C |
-0.241 |
|
|
|
| 4 |
O |
-0.315 |
|
|
|
| 5 |
O |
-0.327 |
|
|
|
| 6 |
H |
0.220 |
|
|
|
| 7 |
H |
0.199 |
|
|
|
| 8 |
H |
0.199 |
|
|
|
| 9 |
H |
0.205 |
|
|
|
| 10 |
H |
0.211 |
|
|
|
| 11 |
H |
0.226 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.591 |
0.342 |
0.663 |
1.757 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.553 |
-0.457 |
0.346 |
| y |
-0.457 |
-36.372 |
1.268 |
| z |
0.346 |
1.268 |
-29.205 |
|
| Traceless |
| | x | y | z |
| x |
8.235 |
-0.457 |
0.346 |
| y |
-0.457 |
-9.493 |
1.268 |
| z |
0.346 |
1.268 |
1.258 |
|
| Polar |
| 3z2-r2 | 2.516 |
| x2-y2 | 11.819 |
| xy | -0.457 |
| xz | 0.346 |
| yz | 1.268 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.191 |
-0.048 |
0.023 |
| y |
-0.048 |
4.883 |
0.037 |
| z |
0.023 |
0.037 |
4.470 |
<r2> (average value of r
2) Å
2
| <r2> |
97.227 |
| (<r2>)1/2 |
9.860 |