Jump to
S1C2
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -342.115180 |
| Energy at 298.15K | |
| HF Energy | -342.115180 |
| Nuclear repulsion energy | 243.761961 |
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 PBEPBE/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 |
A1 |
2979 |
2952 |
60.67 |
|
|
|
| 2 |
A1 |
1886 |
1869 |
547.07 |
|
|
|
| 3 |
A1 |
1495 |
1482 |
0.96 |
|
|
|
| 4 |
A1 |
1340 |
1327 |
0.23 |
|
|
|
| 5 |
A1 |
1142 |
1132 |
206.11 |
|
|
|
| 6 |
A1 |
922 |
914 |
7.85 |
|
|
|
| 7 |
A1 |
796 |
789 |
33.64 |
|
|
|
| 8 |
A1 |
700 |
693 |
0.69 |
|
|
|
| 9 |
A2 |
3001 |
2974 |
0.00 |
|
|
|
| 10 |
A2 |
1205 |
1194 |
0.00 |
|
|
|
| 11 |
A2 |
1123 |
1113 |
0.00 |
|
|
|
| 12 |
A2 |
171i |
169i |
0.00 |
|
|
|
| 13 |
B1 |
3025 |
2997 |
49.89 |
|
|
|
| 14 |
B1 |
1223 |
1212 |
0.89 |
|
|
|
| 15 |
B1 |
832 |
824 |
0.23 |
|
|
|
| 16 |
B1 |
721 |
714 |
15.66 |
|
|
|
| 17 |
B1 |
145 |
143 |
1.72 |
|
|
|
| 18 |
B2 |
2972 |
2945 |
30.45 |
|
|
|
| 19 |
B2 |
1483 |
1469 |
3.76 |
|
|
|
| 20 |
B2 |
1352 |
1339 |
10.74 |
|
|
|
| 21 |
B2 |
1135 |
1125 |
0.15 |
|
|
|
| 22 |
B2 |
981 |
972 |
299.75 |
|
|
|
| 23 |
B2 |
721 |
715 |
6.28 |
|
|
|
| 24 |
B2 |
489 |
484 |
0.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15747.1 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 15603.8 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 PBEPBE/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.872 |
| O2 |
0.000 |
0.000 |
2.063 |
| O3 |
0.000 |
1.142 |
0.059 |
| O4 |
0.000 |
-1.142 |
0.059 |
| C5 |
0.000 |
0.778 |
-1.295 |
| C6 |
0.000 |
-0.778 |
-1.295 |
| H7 |
-0.895 |
1.194 |
-1.784 |
| H8 |
0.895 |
1.194 |
-1.784 |
| H9 |
0.895 |
-1.194 |
-1.784 |
| H10 |
-0.895 |
-1.194 |
-1.784 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1909 | 1.4021 | 1.4021 | 2.3030 | 2.3030 | 3.0470 | 3.0470 | 3.0470 | 3.0470 |
O2 | 1.1909 | | 2.3069 | 2.3069 | 3.4475 | 3.4475 | 4.1267 | 4.1267 | 4.1267 | 4.1267 | O3 | 1.4021 | 2.3069 | | 2.2837 | 1.4021 | 2.3492 | 2.0494 | 2.0494 | 3.1070 | 3.1070 | O4 | 1.4021 | 2.3069 | 2.2837 | | 2.3492 | 1.4021 | 3.1070 | 3.1070 | 2.0494 | 2.0494 | C5 | 2.3030 | 3.4475 | 1.4021 | 2.3492 | | 1.5557 | 1.1014 | 1.1014 | 2.2200 | 2.2200 | C6 | 2.3030 | 3.4475 | 2.3492 | 1.4021 | 1.5557 | | 2.2200 | 2.2200 | 1.1014 | 1.1014 | H7 | 3.0470 | 4.1267 | 2.0494 | 3.1070 | 1.1014 | 2.2200 | | 1.7898 | 2.9843 | 2.3880 | H8 | 3.0470 | 4.1267 | 2.0494 | 3.1070 | 1.1014 | 2.2200 | 1.7898 | | 2.3880 | 2.9843 | H9 | 3.0470 | 4.1267 | 3.1070 | 2.0494 | 2.2200 | 1.1014 | 2.9843 | 2.3880 | | 1.7898 | H10 | 3.0470 | 4.1267 | 3.1070 | 2.0494 | 2.2200 | 1.1014 | 2.3880 | 2.9843 | 1.7898 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.427 |
|
C1 |
O4 |
C6 |
110.427 |
| O2 |
C1 |
O3 |
125.473 |
|
O2 |
C1 |
O4 |
125.473 |
| O3 |
C1 |
O4 |
109.055 |
|
O3 |
C5 |
C6 |
105.046 |
| O3 |
C5 |
H7 |
109.308 |
|
O3 |
C5 |
H8 |
109.308 |
| O4 |
C6 |
C5 |
105.046 |
|
O4 |
C6 |
H9 |
109.308 |
| O4 |
C6 |
H10 |
109.308 |
|
C5 |
C6 |
H9 |
112.199 |
| C5 |
C6 |
H10 |
112.199 |
|
C6 |
C5 |
H7 |
112.199 |
| C6 |
C5 |
H8 |
112.199 |
|
H7 |
C5 |
H8 |
108.682 |
| H9 |
C6 |
H10 |
108.682 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.422 |
|
|
|
| 2 |
O |
-0.272 |
|
|
|
| 3 |
O |
-0.270 |
|
|
|
| 4 |
O |
-0.270 |
|
|
|
| 5 |
C |
-0.086 |
|
|
|
| 6 |
C |
-0.086 |
|
|
|
| 7 |
H |
0.140 |
|
|
|
| 8 |
H |
0.140 |
|
|
|
| 9 |
H |
0.140 |
|
|
|
| 10 |
H |
0.140 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-4.673 |
4.673 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.209 |
0.000 |
0.000 |
| y |
0.000 |
-36.306 |
0.000 |
| z |
0.000 |
0.000 |
-35.566 |
|
| Traceless |
| | x | y | z |
| x |
3.726 |
0.000 |
0.000 |
| y |
0.000 |
-2.418 |
0.000 |
| z |
0.000 |
0.000 |
-1.308 |
|
| Polar |
| 3z2-r2 | -2.616 |
| x2-y2 | 4.097 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.456 |
0.000 |
0.000 |
| y |
0.000 |
5.545 |
0.000 |
| z |
0.000 |
0.000 |
7.853 |
<r2> (average value of r
2) Å
2
| <r2> |
130.241 |
| (<r2>)1/2 |
11.412 |
Jump to
S1C1
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -342.116051 |
| Energy at 298.15K | -342.122332 |
| HF Energy | -342.116051 |
| Nuclear repulsion energy | 244.372546 |
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 PBEPBE/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 |
3036 |
3008 |
21.11 |
|
|
|
| 2 |
A |
2951 |
2924 |
29.98 |
|
|
|
| 3 |
A |
1888 |
1871 |
531.36 |
|
|
|
| 4 |
A |
1481 |
1468 |
1.21 |
|
|
|
| 5 |
A |
1347 |
1335 |
4.22 |
|
|
|
| 6 |
A |
1212 |
1201 |
14.38 |
|
|
|
| 7 |
A |
1148 |
1138 |
105.30 |
|
|
|
| 8 |
A |
1102 |
1092 |
79.15 |
|
|
|
| 9 |
A |
927 |
919 |
3.30 |
|
|
|
| 10 |
A |
790 |
783 |
36.99 |
|
|
|
| 11 |
A |
697 |
691 |
0.94 |
|
|
|
| 12 |
A |
148 |
146 |
0.54 |
|
|
|
| 13 |
B |
3045 |
3017 |
27.65 |
|
|
|
| 14 |
B |
2959 |
2932 |
57.91 |
|
|
|
| 15 |
B |
1474 |
1461 |
5.54 |
|
|
|
| 16 |
B |
1346 |
1334 |
9.06 |
|
|
|
| 17 |
B |
1225 |
1214 |
3.97 |
|
|
|
| 18 |
B |
1112 |
1102 |
3.71 |
|
|
|
| 19 |
B |
978 |
969 |
252.70 |
|
|
|
| 20 |
B |
863 |
855 |
28.05 |
|
|
|
| 21 |
B |
731 |
724 |
16.83 |
|
|
|
| 22 |
B |
658 |
652 |
2.25 |
|
|
|
| 23 |
B |
489 |
484 |
0.68 |
|
|
|
| 24 |
B |
153 |
151 |
1.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15878.9 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 15734.4 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 PBEPBE/6-311G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.867 |
| O2 |
0.000 |
0.000 |
2.058 |
| O3 |
0.000 |
1.142 |
0.047 |
| O4 |
0.000 |
-1.142 |
0.047 |
| C5 |
0.204 |
0.742 |
-1.285 |
| C6 |
-0.204 |
-0.742 |
-1.285 |
| H7 |
-0.415 |
1.360 |
-1.950 |
| H8 |
1.268 |
0.875 |
-1.552 |
| H9 |
0.415 |
-1.360 |
-1.950 |
| H10 |
-1.268 |
-0.875 |
-1.552 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1907 | 1.4058 | 1.4058 | 2.2852 | 2.2852 | 3.1555 | 2.8674 | 3.1555 | 2.8674 |
O2 | 1.1907 | | 2.3122 | 2.3122 | 3.4299 | 3.4299 | 4.2525 | 3.9242 | 4.2525 | 3.9242 | O3 | 1.4058 | 2.3122 | | 2.2842 | 1.4058 | 2.3164 | 2.0516 | 2.0579 | 3.2282 | 2.8691 | O4 | 1.4058 | 2.3122 | 2.2842 | | 2.3164 | 1.4058 | 3.2282 | 2.8691 | 2.0516 | 2.0579 | C5 | 2.2852 | 3.4299 | 1.4058 | 2.3164 | | 1.5389 | 1.0988 | 1.1046 | 2.2145 | 2.2027 | C6 | 2.2852 | 3.4299 | 2.3164 | 1.4058 | 1.5389 | | 2.2145 | 2.2027 | 1.0988 | 1.1046 | H7 | 3.1555 | 4.2525 | 2.0516 | 3.2282 | 1.0988 | 2.2145 | | 1.7957 | 2.8432 | 2.4250 | H8 | 2.8674 | 3.9242 | 2.0579 | 2.8691 | 1.1046 | 2.2027 | 1.7957 | | 2.4250 | 3.0808 | H9 | 3.1555 | 4.2525 | 3.2282 | 2.0516 | 2.2145 | 1.0988 | 2.8432 | 2.4250 | | 1.7957 | H10 | 2.8674 | 3.9242 | 2.8691 | 2.0579 | 2.2027 | 1.1046 | 2.4250 | 3.0808 | 1.7957 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.735 |
|
C1 |
O4 |
C6 |
108.735 |
| O2 |
C1 |
O3 |
125.667 |
|
O2 |
C1 |
O4 |
125.667 |
| O3 |
C1 |
O4 |
108.665 |
|
O3 |
C5 |
C6 |
103.649 |
| O3 |
C5 |
H7 |
109.381 |
|
O3 |
C5 |
H8 |
109.533 |
| O4 |
C6 |
C5 |
103.649 |
|
O4 |
C6 |
H9 |
109.381 |
| O4 |
C6 |
H10 |
109.533 |
|
C5 |
C6 |
H9 |
113.130 |
| C5 |
C6 |
H10 |
111.814 |
|
C6 |
C5 |
H7 |
113.130 |
| C6 |
C5 |
H8 |
111.814 |
|
H7 |
C5 |
H8 |
109.166 |
| H9 |
C6 |
H10 |
109.166 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.423 |
|
|
|
| 2 |
O |
-0.268 |
|
|
|
| 3 |
O |
-0.270 |
|
|
|
| 4 |
O |
-0.270 |
|
|
|
| 5 |
C |
-0.087 |
|
|
|
| 6 |
C |
-0.087 |
|
|
|
| 7 |
H |
0.140 |
|
|
|
| 8 |
H |
0.139 |
|
|
|
| 9 |
H |
0.140 |
|
|
|
| 10 |
H |
0.139 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-4.610 |
4.610 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.312 |
0.181 |
0.000 |
| y |
0.181 |
-36.308 |
0.000 |
| z |
0.000 |
0.000 |
-35.366 |
|
| Traceless |
| | x | y | z |
| x |
3.525 |
0.181 |
0.000 |
| y |
0.181 |
-2.470 |
0.000 |
| z |
0.000 |
0.000 |
-1.056 |
|
| Polar |
| 3z2-r2 | -2.111 |
| x2-y2 | 3.997 |
| xy | 0.181 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.582 |
0.183 |
0.000 |
| y |
0.183 |
5.492 |
0.000 |
| z |
0.000 |
0.000 |
7.810 |
<r2> (average value of r
2) Å
2
| <r2> |
129.060 |
| (<r2>)1/2 |
11.360 |