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S1C2
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Vibrational Frequencies calculated at B1B95/3-21G
Geometric Data calculated at B1B95/3-21G
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C3
Vibrational Frequencies calculated at B1B95/3-21G
Geometric Data calculated at B1B95/3-21G
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -266.755708 |
| Energy at 298.15K | -266.763865 |
| Nuclear repulsion energy | 191.107422 |
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 B1B95/3-21G
| 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 |
3180 |
3042 |
28.21 |
|
|
|
| 2 |
A |
3175 |
3037 |
9.02 |
|
|
|
| 3 |
A |
3108 |
2973 |
65.24 |
|
|
|
| 4 |
A |
3072 |
2939 |
56.65 |
|
|
|
| 5 |
A |
3065 |
2932 |
0.49 |
|
|
|
| 6 |
A |
3054 |
2922 |
99.37 |
|
|
|
| 7 |
A |
1597 |
1528 |
4.66 |
|
|
|
| 8 |
A |
1552 |
1485 |
0.43 |
|
|
|
| 9 |
A |
1549 |
1482 |
2.75 |
|
|
|
| 10 |
A |
1413 |
1352 |
0.26 |
|
|
|
| 11 |
A |
1382 |
1322 |
7.90 |
|
|
|
| 12 |
A |
1340 |
1282 |
2.58 |
|
|
|
| 13 |
A |
1251 |
1197 |
7.15 |
|
|
|
| 14 |
A |
1214 |
1161 |
1.01 |
|
|
|
| 15 |
A |
1183 |
1132 |
28.60 |
|
|
|
| 16 |
A |
1135 |
1085 |
0.60 |
|
|
|
| 17 |
A |
1114 |
1066 |
13.06 |
|
|
|
| 18 |
A |
1087 |
1040 |
131.19 |
|
|
|
| 19 |
A |
1033 |
988 |
20.92 |
|
|
|
| 20 |
A |
946 |
905 |
8.63 |
|
|
|
| 21 |
A |
935 |
895 |
0.19 |
|
|
|
| 22 |
A |
934 |
894 |
14.04 |
|
|
|
| 23 |
A |
872 |
834 |
42.53 |
|
|
|
| 24 |
A |
692 |
662 |
0.10 |
|
|
|
| 25 |
A |
615 |
589 |
6.62 |
|
|
|
| 26 |
A |
266 |
255 |
1.02 |
|
|
|
| 27 |
A |
48 |
46 |
25.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20405.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 19521.9 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 B1B95/3-21G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.235 |
0.000 |
0.001 |
| C2 |
0.966 |
0.730 |
-0.219 |
| C3 |
0.965 |
-0.731 |
0.220 |
| O4 |
-0.377 |
1.162 |
0.178 |
| O5 |
-0.378 |
-1.161 |
-0.180 |
| H6 |
-1.850 |
-0.083 |
0.900 |
| H7 |
-1.853 |
0.083 |
-0.897 |
| H8 |
1.107 |
0.806 |
-1.302 |
| H9 |
1.104 |
-0.807 |
1.303 |
| H10 |
1.680 |
-1.358 |
-0.310 |
| H11 |
1.680 |
1.356 |
0.312 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
O5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 2.3290 | 2.3285 | 1.4550 | 1.4548 | 1.0930 | 1.0929 | 2.7985 | 2.7965 | 3.2305 | 3.2304 |
C2 | 2.3290 | | 1.5250 | 1.4654 | 2.3200 | 3.1372 | 2.9704 | 1.0951 | 2.1675 | 2.2081 | 1.0884 | C3 | 2.3285 | 1.5250 | | 2.3203 | 1.4654 | 2.9677 | 3.1384 | 2.1674 | 1.0951 | 1.0884 | 2.2081 | O4 | 1.4550 | 1.4654 | 2.3203 | | 2.3504 | 2.0591 | 2.1209 | 2.1262 | 2.7084 | 3.2888 | 2.0710 | O5 | 1.4548 | 2.3200 | 1.4654 | 2.3504 | | 2.1208 | 2.0589 | 2.7081 | 2.1263 | 2.0709 | 3.2886 | H6 | 1.0930 | 3.1372 | 2.9677 | 2.0591 | 2.1208 | | 1.8051 | 3.7928 | 3.0684 | 3.9434 | 3.8577 | H7 | 1.0929 | 2.9704 | 3.1384 | 2.1209 | 2.0589 | 1.8051 | | 3.0737 | 3.7919 | 3.8601 | 3.9455 | H8 | 2.7985 | 1.0951 | 2.1674 | 2.1262 | 2.7081 | 3.7928 | 3.0737 | | 3.0643 | 2.4483 | 1.7990 | H9 | 2.7965 | 2.1675 | 1.0951 | 2.7084 | 2.1263 | 3.0684 | 3.7919 | 3.0643 | | 1.7991 | 2.4483 | H10 | 3.2305 | 2.2081 | 1.0884 | 3.2888 | 2.0709 | 3.9434 | 3.8601 | 2.4483 | 1.7991 | | 2.7842 | H11 | 3.2304 | 1.0884 | 2.2081 | 2.0710 | 3.2886 | 3.8577 | 3.9455 | 1.7990 | 2.4483 | 2.7842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O4 |
C2 |
105.782 |
|
C1 |
O5 |
C3 |
105.759 |
| C2 |
C3 |
O5 |
101.739 |
|
C2 |
C3 |
H9 |
110.562 |
| C2 |
C3 |
H10 |
114.291 |
|
C3 |
C2 |
O4 |
101.757 |
| C3 |
C2 |
H8 |
110.558 |
|
C3 |
C2 |
H11 |
114.285 |
| O4 |
C1 |
O5 |
107.753 |
|
O4 |
C1 |
H6 |
106.971 |
| O4 |
C1 |
H7 |
111.909 |
|
O4 |
C2 |
H8 |
111.460 |
| O4 |
C2 |
H11 |
107.451 |
|
O5 |
C1 |
H6 |
111.912 |
| O5 |
C1 |
H7 |
106.966 |
|
O5 |
C3 |
H9 |
111.464 |
| O5 |
C3 |
H10 |
107.449 |
|
H6 |
C1 |
H7 |
111.332 |
| H8 |
C2 |
H11 |
110.956 |
|
H9 |
C3 |
H10 |
110.960 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.064 |
|
|
|
| 2 |
C |
-0.208 |
|
|
|
| 3 |
C |
-0.208 |
|
|
|
| 4 |
O |
-0.491 |
|
|
|
| 5 |
O |
-0.491 |
|
|
|
| 6 |
H |
0.216 |
|
|
|
| 7 |
H |
0.216 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
| 9 |
H |
0.219 |
|
|
|
| 10 |
H |
0.232 |
|
|
|
| 11 |
H |
0.232 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.324 |
-0.003 |
0.004 |
1.324 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.818 |
-0.004 |
-0.002 |
| y |
-0.004 |
-34.958 |
-1.243 |
| z |
-0.002 |
-1.243 |
-29.252 |
|
| Traceless |
| | x | y | z |
| x |
7.287 |
-0.004 |
-0.002 |
| y |
-0.004 |
-7.923 |
-1.243 |
| z |
-0.002 |
-1.243 |
0.636 |
|
| Polar |
| 3z2-r2 | 1.272 |
| x2-y2 | 10.140 |
| xy | -0.004 |
| xz | -0.002 |
| yz | -1.243 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.140 |
-0.000 |
-0.000 |
| y |
-0.000 |
4.479 |
-0.055 |
| z |
-0.000 |
-0.055 |
4.579 |
<r2> (average value of r
2) Å
2
| <r2> |
95.368 |
| (<r2>)1/2 |
9.766 |