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S1C2
S1C3
Vibrational Frequencies calculated at B1B95/6-311G**
Geometric Data calculated at B1B95/6-311G**
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C3
Vibrational Frequencies calculated at B1B95/6-311G**
Geometric Data calculated at B1B95/6-311G**
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -268.306329 |
| Energy at 298.15K | -268.314653 |
| Nuclear repulsion energy | 195.426239 |
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 B1B95/6-311G**
| 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 |
3142 |
3016 |
25.67 |
|
|
|
| 2 |
A |
3119 |
2994 |
40.83 |
|
|
|
| 3 |
A |
3092 |
2968 |
44.87 |
|
|
|
| 4 |
A |
3049 |
2927 |
56.75 |
|
|
|
| 5 |
A |
3007 |
2887 |
55.02 |
|
|
|
| 6 |
A |
2949 |
2832 |
121.11 |
|
|
|
| 7 |
A |
1541 |
1479 |
2.18 |
|
|
|
| 8 |
A |
1523 |
1463 |
1.69 |
|
|
|
| 9 |
A |
1504 |
1444 |
2.94 |
|
|
|
| 10 |
A |
1429 |
1372 |
9.97 |
|
|
|
| 11 |
A |
1377 |
1322 |
1.02 |
|
|
|
| 12 |
A |
1344 |
1290 |
0.36 |
|
|
|
| 13 |
A |
1280 |
1229 |
7.95 |
|
|
|
| 14 |
A |
1235 |
1186 |
3.93 |
|
|
|
| 15 |
A |
1210 |
1161 |
7.22 |
|
|
|
| 16 |
A |
1194 |
1146 |
100.11 |
|
|
|
| 17 |
A |
1152 |
1106 |
20.83 |
|
|
|
| 18 |
A |
1127 |
1082 |
93.64 |
|
|
|
| 19 |
A |
1083 |
1040 |
34.99 |
|
|
|
| 20 |
A |
1009 |
969 |
36.89 |
|
|
|
| 21 |
A |
973 |
934 |
47.30 |
|
|
|
| 22 |
A |
955 |
917 |
31.86 |
|
|
|
| 23 |
A |
876 |
841 |
12.24 |
|
|
|
| 24 |
A |
741 |
712 |
0.80 |
|
|
|
| 25 |
A |
671 |
644 |
4.96 |
|
|
|
| 26 |
A |
288 |
277 |
10.80 |
|
|
|
| 27 |
A |
62 |
60 |
3.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20465.6 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 19649.0 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 B1B95/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.159 |
-0.106 |
0.149 |
| C2 |
-0.819 |
0.857 |
0.162 |
| C3 |
-1.040 |
-0.639 |
-0.062 |
| O4 |
0.508 |
1.048 |
-0.289 |
| O5 |
0.274 |
-1.181 |
-0.058 |
| H6 |
2.061 |
-0.253 |
-0.444 |
| H7 |
1.409 |
-0.026 |
1.220 |
| H8 |
-0.900 |
1.115 |
1.226 |
| H9 |
-1.503 |
-0.844 |
-1.030 |
| H10 |
-1.644 |
-1.094 |
0.726 |
| H11 |
-1.479 |
1.499 |
-0.416 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
O5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
| C1 | | 2.1995 | 2.2724 | 1.3959 | 1.4082 | 1.0895 | 1.1025 | 2.6248 | 3.0039 | 3.0273 | 3.1392 |
C2 | 2.1995 | | 1.5287 | 1.4140 | 2.3229 | 3.1448 | 2.6191 | 1.0977 | 2.1872 | 2.1919 | 1.0879 | C3 | 2.2724 | 1.5287 | | 2.3007 | 1.4212 | 3.1476 | 2.8314 | 2.1811 | 1.0925 | 1.0927 | 2.2111 | O4 | 1.3959 | 1.4140 | 2.3007 | | 2.2538 | 2.0321 | 2.0602 | 2.0693 | 2.8589 | 3.2014 | 2.0412 | O5 | 1.4082 | 2.3229 | 1.4212 | 2.2538 | | 2.0502 | 2.0631 | 2.8810 | 2.0536 | 2.0736 | 3.2225 | H6 | 1.0895 | 3.1448 | 3.1476 | 2.0321 | 2.0502 | | 1.8019 | 3.6644 | 3.6595 | 3.9748 | 3.9496 | H7 | 1.1025 | 2.6191 | 2.8314 | 2.0602 | 2.0631 | 1.8019 | | 2.5755 | 3.7701 | 3.2714 | 3.6529 | H8 | 2.6248 | 1.0977 | 2.1811 | 2.0693 | 2.8810 | 3.6644 | 2.5755 | | 3.0486 | 2.3839 | 1.7835 | H9 | 3.0039 | 2.1872 | 1.0925 | 2.8589 | 2.0536 | 3.6595 | 3.7701 | 3.0486 | | 1.7801 | 2.4219 | H10 | 3.0273 | 2.1919 | 1.0927 | 3.2014 | 2.0736 | 3.9748 | 3.2714 | 2.3839 | 1.7801 | | 2.8382 | H11 | 3.1392 | 1.0879 | 2.2111 | 2.0412 | 3.2225 | 3.9496 | 3.6529 | 1.7835 | 2.4219 | 2.8382 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O4 |
C2 |
103.024 |
|
C1 |
O5 |
C3 |
106.862 |
| C2 |
C3 |
O5 |
103.834 |
|
C2 |
C3 |
H9 |
112.031 |
| C2 |
C3 |
H10 |
112.406 |
|
C3 |
C2 |
O4 |
102.785 |
| C3 |
C2 |
H8 |
111.227 |
|
C3 |
C2 |
H11 |
114.290 |
| O4 |
C1 |
O5 |
106.975 |
|
O4 |
C1 |
H6 |
109.073 |
| O4 |
C1 |
H7 |
110.548 |
|
O4 |
C2 |
H8 |
110.310 |
| O4 |
C2 |
H11 |
108.640 |
|
O5 |
C1 |
H6 |
109.679 |
| O5 |
C1 |
H7 |
109.913 |
|
O5 |
C3 |
H9 |
108.862 |
| O5 |
C3 |
H10 |
110.467 |
|
H6 |
C1 |
H7 |
110.579 |
| H8 |
C2 |
H11 |
109.373 |
|
H9 |
C3 |
H10 |
109.103 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.145 |
|
|
|
| 2 |
C |
-0.139 |
|
|
|
| 3 |
C |
-0.023 |
|
|
|
| 4 |
O |
-0.339 |
|
|
|
| 5 |
O |
-0.372 |
|
|
|
| 6 |
H |
0.124 |
|
|
|
| 7 |
H |
0.100 |
|
|
|
| 8 |
H |
0.128 |
|
|
|
| 9 |
H |
0.124 |
|
|
|
| 10 |
H |
0.115 |
|
|
|
| 11 |
H |
0.137 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.182 |
0.442 |
0.769 |
1.478 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.809 |
-0.950 |
0.504 |
| y |
-0.950 |
-34.168 |
0.565 |
| z |
0.504 |
0.565 |
-29.523 |
|
| Traceless |
| | x | y | z |
| x |
6.037 |
-0.950 |
0.504 |
| y |
-0.950 |
-6.502 |
0.565 |
| z |
0.504 |
0.565 |
0.465 |
|
| Polar |
| 3z2-r2 | 0.930 |
| x2-y2 | 8.359 |
| xy | -0.950 |
| xz | 0.504 |
| yz | 0.565 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.557 |
-0.110 |
0.077 |
| y |
-0.110 |
5.225 |
0.107 |
| z |
0.077 |
0.107 |
5.178 |
<r2> (average value of r
2) Å
2
| <r2> |
92.357 |
| (<r2>)1/2 |
9.610 |