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Vibrational Frequencies calculated at B3PW91/aug-cc-pVDZ
Geometric Data calculated at B3PW91/aug-cc-pVDZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C3
Vibrational Frequencies calculated at B3PW91/aug-cc-pVDZ
Geometric Data calculated at B3PW91/aug-cc-pVDZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B3PW91/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -268.284282 |
| Energy at 298.15K | -268.292569 |
| Nuclear repulsion energy | 194.168958 |
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 B3PW91/aug-cc-pVDZ
| 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 |
3140 |
3029 |
24.03 |
|
|
|
| 2 |
A |
3119 |
3008 |
32.95 |
|
|
|
| 3 |
A |
3096 |
2986 |
34.37 |
|
|
|
| 4 |
A |
3048 |
2940 |
58.97 |
|
|
|
| 5 |
A |
3014 |
2908 |
51.59 |
|
|
|
| 6 |
A |
2958 |
2853 |
114.90 |
|
|
|
| 7 |
A |
1524 |
1470 |
1.80 |
|
|
|
| 8 |
A |
1508 |
1454 |
0.87 |
|
|
|
| 9 |
A |
1493 |
1440 |
2.70 |
|
|
|
| 10 |
A |
1402 |
1352 |
5.33 |
|
|
|
| 11 |
A |
1363 |
1315 |
0.08 |
|
|
|
| 12 |
A |
1329 |
1282 |
0.95 |
|
|
|
| 13 |
A |
1261 |
1217 |
6.27 |
|
|
|
| 14 |
A |
1222 |
1178 |
3.78 |
|
|
|
| 15 |
A |
1197 |
1155 |
4.45 |
|
|
|
| 16 |
A |
1179 |
1138 |
89.11 |
|
|
|
| 17 |
A |
1144 |
1104 |
26.06 |
|
|
|
| 18 |
A |
1113 |
1074 |
84.36 |
|
|
|
| 19 |
A |
1071 |
1033 |
36.22 |
|
|
|
| 20 |
A |
995 |
960 |
23.11 |
|
|
|
| 21 |
A |
969 |
935 |
34.29 |
|
|
|
| 22 |
A |
945 |
912 |
56.66 |
|
|
|
| 23 |
A |
867 |
836 |
9.69 |
|
|
|
| 24 |
A |
739 |
713 |
0.42 |
|
|
|
| 25 |
A |
684 |
660 |
5.29 |
|
|
|
| 26 |
A |
277 |
267 |
11.07 |
|
|
|
| 27 |
A |
55 |
53 |
4.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20355.2 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 19634.7 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 B3PW91/aug-cc-pVDZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.173 |
-0.084 |
0.147 |
| C2 |
-1.032 |
-0.667 |
-0.052 |
| C3 |
-0.850 |
0.844 |
0.149 |
| O4 |
0.303 |
-1.179 |
-0.066 |
| O5 |
0.490 |
1.069 |
-0.272 |
| H6 |
1.433 |
-0.012 |
1.223 |
| H7 |
2.076 |
-0.208 |
-0.464 |
| H8 |
-1.507 |
-0.908 |
-1.014 |
| H9 |
-0.971 |
1.127 |
1.209 |
| H10 |
-1.514 |
1.458 |
-0.469 |
| H11 |
-1.606 |
-1.133 |
0.762 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
O5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 2.2894 | 2.2258 | 1.4153 | 1.4044 | 1.1090 | 1.0971 | 3.0351 | 2.6816 | 3.1590 | 3.0337 |
C2 | 2.2894 | | 1.5347 | 1.4299 | 2.3188 | 2.8513 | 3.1683 | 1.0995 | 2.1938 | 2.2190 | 1.1000 | C3 | 2.2258 | 1.5347 | | 2.3386 | 1.4224 | 2.6646 | 3.1691 | 2.2026 | 1.1040 | 1.0956 | 2.2032 | O4 | 1.4153 | 1.4299 | 2.3386 | | 2.2655 | 2.0741 | 2.0604 | 2.0611 | 2.9275 | 3.2283 | 2.0819 | O5 | 1.4044 | 2.3188 | 1.4224 | 2.2655 | | 2.0725 | 2.0453 | 2.9061 | 2.0811 | 2.0506 | 3.2110 | H6 | 1.1090 | 2.8513 | 2.6646 | 2.0741 | 2.0725 | | 1.8155 | 3.8014 | 2.6605 | 3.7029 | 3.2719 | H7 | 1.0971 | 3.1683 | 3.1691 | 2.0604 | 2.0453 | 1.8155 | | 3.6922 | 3.7234 | 3.9578 | 3.9896 | H8 | 3.0351 | 1.0995 | 2.2026 | 2.0611 | 2.9061 | 3.8014 | 3.6922 | | 3.0610 | 2.4282 | 1.7929 | H9 | 2.6816 | 2.1938 | 1.1040 | 2.9275 | 2.0811 | 2.6605 | 3.7234 | 3.0610 | | 1.7946 | 2.3895 | H10 | 3.1590 | 2.2190 | 1.0956 | 3.2283 | 2.0506 | 3.7029 | 3.9578 | 2.4282 | 1.7946 | | 2.8703 | H11 | 3.0337 | 1.1000 | 2.2032 | 2.0819 | 3.2110 | 3.2719 | 3.9896 | 1.7929 | 2.3895 | 2.8703 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O4 |
C2 |
107.159 |
|
C1 |
O5 |
C3 |
103.884 |
| C2 |
C3 |
O5 |
103.216 |
|
C2 |
C3 |
H9 |
111.437 |
| C2 |
C3 |
H10 |
114.003 |
|
C3 |
C2 |
O4 |
104.100 |
| C3 |
C2 |
H8 |
112.417 |
|
C3 |
C2 |
H11 |
112.433 |
| O4 |
C1 |
O5 |
106.922 |
|
O4 |
C1 |
H6 |
109.910 |
| O4 |
C1 |
H7 |
109.538 |
|
O4 |
C2 |
H8 |
108.440 |
| O4 |
C2 |
H11 |
110.076 |
|
O5 |
C1 |
H6 |
110.542 |
| O5 |
C1 |
H7 |
109.080 |
|
O5 |
C3 |
H9 |
110.283 |
| O5 |
C3 |
H10 |
108.350 |
|
H6 |
C1 |
H7 |
110.764 |
| H8 |
C2 |
H11 |
109.202 |
|
H9 |
C3 |
H10 |
109.345 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.226 |
|
|
|
| 2 |
C |
1.008 |
|
|
|
| 3 |
C |
0.833 |
|
|
|
| 4 |
O |
-0.640 |
|
|
|
| 5 |
O |
-0.607 |
|
|
|
| 6 |
H |
-0.273 |
|
|
|
| 7 |
H |
-0.332 |
|
|
|
| 8 |
H |
-0.322 |
|
|
|
| 9 |
H |
-0.313 |
|
|
|
| 10 |
H |
-0.307 |
|
|
|
| 11 |
H |
-0.273 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.180 |
0.352 |
0.762 |
1.448 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.293 |
-0.757 |
0.502 |
| y |
-0.757 |
-34.502 |
0.537 |
| z |
0.502 |
0.537 |
-29.825 |
|
| Traceless |
| | x | y | z |
| x |
5.871 |
-0.757 |
0.502 |
| y |
-0.757 |
-6.443 |
0.537 |
| z |
0.502 |
0.537 |
0.573 |
|
| Polar |
| 3z2-r2 | 1.145 |
| x2-y2 | 8.210 |
| xy | -0.757 |
| xz | 0.502 |
| yz | 0.537 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.495 |
-0.053 |
0.059 |
| y |
-0.053 |
6.419 |
0.072 |
| z |
0.059 |
0.072 |
5.987 |
<r2> (average value of r
2) Å
2
| <r2> |
93.661 |
| (<r2>)1/2 |
9.678 |