Jump to
S1C2
Energy calculated at PBEPBE/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -342.076599 |
| Energy at 298.15K | |
| HF Energy | -342.076599 |
| Nuclear repulsion energy | 243.040435 |
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/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 |
A1 |
2986 |
2968 |
65.54 |
|
|
|
| 2 |
A1 |
1848 |
1837 |
575.32 |
|
|
|
| 3 |
A1 |
1476 |
1467 |
0.41 |
|
|
|
| 4 |
A1 |
1334 |
1326 |
0.01 |
|
|
|
| 5 |
A1 |
1141 |
1134 |
200.89 |
|
|
|
| 6 |
A1 |
933 |
927 |
9.75 |
|
|
|
| 7 |
A1 |
791 |
786 |
38.34 |
|
|
|
| 8 |
A1 |
694 |
690 |
0.39 |
|
|
|
| 9 |
A2 |
3016 |
2998 |
0.00 |
|
|
|
| 10 |
A2 |
1200 |
1193 |
0.00 |
|
|
|
| 11 |
A2 |
1120 |
1113 |
0.00 |
|
|
|
| 12 |
A2 |
167i |
166i |
0.00 |
|
|
|
| 13 |
B1 |
3039 |
3020 |
38.76 |
|
|
|
| 14 |
B1 |
1214 |
1206 |
1.40 |
|
|
|
| 15 |
B1 |
832 |
827 |
0.19 |
|
|
|
| 16 |
B1 |
715 |
710 |
14.38 |
|
|
|
| 17 |
B1 |
146 |
145 |
1.44 |
|
|
|
| 18 |
B2 |
2980 |
2961 |
22.87 |
|
|
|
| 19 |
B2 |
1466 |
1457 |
4.20 |
|
|
|
| 20 |
B2 |
1334 |
1326 |
10.58 |
|
|
|
| 21 |
B2 |
1132 |
1125 |
1.11 |
|
|
|
| 22 |
B2 |
983 |
977 |
276.42 |
|
|
|
| 23 |
B2 |
717 |
712 |
5.21 |
|
|
|
| 24 |
B2 |
478 |
475 |
0.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15702.7 cm
-1
Scaled (by 0.9939) Zero Point Vibrational Energy (zpe) 15606.9 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 PBEPBE/aug-cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.873 |
| O2 |
0.000 |
0.000 |
2.072 |
| O3 |
0.000 |
1.145 |
0.057 |
| O4 |
0.000 |
-1.145 |
0.057 |
| C5 |
0.000 |
0.777 |
-1.299 |
| C6 |
0.000 |
-0.777 |
-1.299 |
| H7 |
-0.900 |
1.198 |
-1.787 |
| H8 |
0.900 |
1.198 |
-1.787 |
| H9 |
0.900 |
-1.198 |
-1.787 |
| H10 |
-0.900 |
-1.198 |
-1.787 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1988 | 1.4057 | 1.4057 | 2.3076 | 2.3076 | 3.0531 | 3.0531 | 3.0531 | 3.0531 |
O2 | 1.1988 | | 2.3172 | 2.3172 | 3.4600 | 3.4600 | 4.1397 | 4.1397 | 4.1397 | 4.1397 | O3 | 1.4057 | 2.3172 | | 2.2893 | 1.4057 | 2.3525 | 2.0527 | 2.0527 | 3.1145 | 3.1145 | O4 | 1.4057 | 2.3172 | 2.2893 | | 2.3525 | 1.4057 | 3.1145 | 3.1145 | 2.0527 | 2.0527 | C5 | 2.3076 | 3.4600 | 1.4057 | 2.3525 | | 1.5543 | 1.1066 | 1.1066 | 2.2247 | 2.2247 | C6 | 2.3076 | 3.4600 | 2.3525 | 1.4057 | 1.5543 | | 2.2247 | 2.2247 | 1.1066 | 1.1066 | H7 | 3.0531 | 4.1397 | 2.0527 | 3.1145 | 1.1066 | 2.2247 | | 1.7996 | 2.9970 | 2.3966 | H8 | 3.0531 | 4.1397 | 2.0527 | 3.1145 | 1.1066 | 2.2247 | 1.7996 | | 2.3966 | 2.9970 | H9 | 3.0531 | 4.1397 | 3.1145 | 2.0527 | 2.2247 | 1.1066 | 2.9970 | 2.3966 | | 1.7996 | H10 | 3.0531 | 4.1397 | 3.1145 | 2.0527 | 2.2247 | 1.1066 | 2.3966 | 2.9970 | 1.7996 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.327 |
|
C1 |
O4 |
C6 |
110.327 |
| O2 |
C1 |
O3 |
125.482 |
|
O2 |
C1 |
O4 |
125.482 |
| O3 |
C1 |
O4 |
109.036 |
|
O3 |
C5 |
C6 |
105.155 |
| O3 |
C5 |
H7 |
109.002 |
|
O3 |
C5 |
H8 |
109.002 |
| O4 |
C6 |
C5 |
105.155 |
|
O4 |
C6 |
H9 |
109.002 |
| O4 |
C6 |
H10 |
109.002 |
|
C5 |
C6 |
H9 |
112.369 |
| C5 |
C6 |
H10 |
112.369 |
|
C6 |
C5 |
H7 |
112.369 |
| C6 |
C5 |
H8 |
112.369 |
|
H7 |
C5 |
H8 |
108.809 |
| H9 |
C6 |
H10 |
108.809 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.806 |
|
|
|
| 2 |
O |
-0.448 |
|
|
|
| 3 |
O |
-0.490 |
|
|
|
| 4 |
O |
-0.490 |
|
|
|
| 5 |
C |
1.036 |
|
|
|
| 6 |
C |
1.036 |
|
|
|
| 7 |
H |
-0.362 |
|
|
|
| 8 |
H |
-0.362 |
|
|
|
| 9 |
H |
-0.362 |
|
|
|
| 10 |
H |
-0.362 |
|
|
|
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 |
-4.803 |
4.803 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.705 |
0.000 |
0.000 |
| y |
0.000 |
-36.536 |
0.000 |
| z |
0.000 |
0.000 |
-36.689 |
|
| Traceless |
| | x | y | z |
| x |
3.908 |
0.000 |
0.000 |
| y |
0.000 |
-1.839 |
0.000 |
| z |
0.000 |
0.000 |
-2.069 |
|
| Polar |
| 3z2-r2 | -4.138 |
| x2-y2 | 3.831 |
| 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 |
5.418 |
0.000 |
0.000 |
| y |
0.000 |
6.909 |
0.000 |
| z |
0.000 |
0.000 |
9.149 |
<r2> (average value of r
2) Å
2
| <r2> |
131.260 |
| (<r2>)1/2 |
11.457 |
Jump to
S1C1
Energy calculated at PBEPBE/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -342.077274 |
| Energy at 298.15K | -342.083521 |
| HF Energy | -342.077274 |
| Nuclear repulsion energy | 243.555479 |
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/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 |
3047 |
3028 |
17.89 |
|
|
|
| 2 |
A |
2964 |
2946 |
37.60 |
|
|
|
| 3 |
A |
1851 |
1840 |
561.51 |
|
|
|
| 4 |
A |
1465 |
1456 |
0.56 |
|
|
|
| 5 |
A |
1337 |
1329 |
1.95 |
|
|
|
| 6 |
A |
1202 |
1195 |
14.68 |
|
|
|
| 7 |
A |
1144 |
1137 |
118.15 |
|
|
|
| 8 |
A |
1099 |
1092 |
65.77 |
|
|
|
| 9 |
A |
935 |
929 |
4.57 |
|
|
|
| 10 |
A |
785 |
780 |
41.20 |
|
|
|
| 11 |
A |
692 |
688 |
0.60 |
|
|
|
| 12 |
A |
133 |
132 |
0.36 |
|
|
|
| 13 |
B |
3057 |
3039 |
22.44 |
|
|
|
| 14 |
B |
2970 |
2952 |
45.11 |
|
|
|
| 15 |
B |
1457 |
1448 |
5.60 |
|
|
|
| 16 |
B |
1327 |
1319 |
8.69 |
|
|
|
| 17 |
B |
1214 |
1206 |
3.87 |
|
|
|
| 18 |
B |
1111 |
1104 |
2.61 |
|
|
|
| 19 |
B |
977 |
971 |
244.68 |
|
|
|
| 20 |
B |
858 |
853 |
20.30 |
|
|
|
| 21 |
B |
723 |
718 |
14.76 |
|
|
|
| 22 |
B |
663 |
659 |
1.95 |
|
|
|
| 23 |
B |
478 |
475 |
0.61 |
|
|
|
| 24 |
B |
153 |
152 |
1.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15820.2 cm
-1
Scaled (by 0.9939) Zero Point Vibrational Energy (zpe) 15723.7 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 PBEPBE/aug-cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.869 |
| O2 |
0.000 |
0.000 |
2.067 |
| O3 |
0.000 |
1.145 |
0.047 |
| O4 |
0.000 |
-1.145 |
0.047 |
| C5 |
0.193 |
0.746 |
-1.290 |
| C6 |
-0.193 |
-0.746 |
-1.290 |
| H7 |
-0.451 |
1.358 |
-1.946 |
| H8 |
1.255 |
0.902 |
-1.570 |
| H9 |
0.451 |
-1.358 |
-1.946 |
| H10 |
-1.255 |
-0.902 |
-1.570 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1984 | 1.4092 | 1.4092 | 2.2924 | 2.2924 | 3.1577 | 2.8869 | 3.1577 | 2.8869 |
O2 | 1.1984 | | 2.3219 | 2.3219 | 3.4447 | 3.4447 | 4.2607 | 3.9516 | 4.2607 | 3.9516 | O3 | 1.4092 | 2.3219 | | 2.2900 | 1.4092 | 2.3239 | 2.0546 | 2.0611 | 3.2316 | 2.8947 | O4 | 1.4092 | 2.3219 | 2.2900 | | 2.3239 | 1.4092 | 3.2316 | 2.8947 | 2.0546 | 2.0611 | C5 | 2.2924 | 3.4447 | 1.4092 | 2.3239 | | 1.5400 | 1.1041 | 1.1093 | 2.2188 | 2.2107 | C6 | 2.2924 | 3.4447 | 2.3239 | 1.4092 | 1.5400 | | 2.2188 | 2.2107 | 1.1041 | 1.1093 | H7 | 3.1577 | 4.2607 | 2.0546 | 3.2316 | 1.1041 | 2.2188 | | 1.8049 | 2.8624 | 2.4285 | H8 | 2.8869 | 3.9516 | 2.0611 | 2.8947 | 1.1093 | 2.2107 | 1.8049 | | 2.4285 | 3.0905 | H9 | 3.1577 | 4.2607 | 3.2316 | 2.0546 | 2.2188 | 1.1041 | 2.8624 | 2.4285 | | 1.8049 | H10 | 2.8869 | 3.9516 | 2.8947 | 2.0611 | 2.2107 | 1.1093 | 2.4285 | 3.0905 | 1.8049 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.847 |
|
C1 |
O4 |
C6 |
108.847 |
| O2 |
C1 |
O3 |
125.659 |
|
O2 |
C1 |
O4 |
125.659 |
| O3 |
C1 |
O4 |
108.682 |
|
O3 |
C5 |
C6 |
103.903 |
| O3 |
C5 |
H7 |
109.067 |
|
O3 |
C5 |
H8 |
109.262 |
| O4 |
C6 |
C5 |
103.903 |
|
O4 |
C6 |
H9 |
109.067 |
| O4 |
C6 |
H10 |
109.262 |
|
C5 |
C6 |
H9 |
113.066 |
| C5 |
C6 |
H10 |
112.086 |
|
C6 |
C5 |
H7 |
113.066 |
| C6 |
C5 |
H8 |
112.086 |
|
H7 |
C5 |
H8 |
109.262 |
| H9 |
C6 |
H10 |
109.262 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.817 |
|
|
|
| 2 |
O |
-0.458 |
|
|
|
| 3 |
O |
-0.497 |
|
|
|
| 4 |
O |
-0.497 |
|
|
|
| 5 |
C |
1.045 |
|
|
|
| 6 |
C |
1.045 |
|
|
|
| 7 |
H |
-0.338 |
|
|
|
| 8 |
H |
-0.390 |
|
|
|
| 9 |
H |
-0.338 |
|
|
|
| 10 |
H |
-0.390 |
|
|
|
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 |
-4.761 |
4.761 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.814 |
0.236 |
0.000 |
| y |
0.236 |
-36.564 |
0.000 |
| z |
0.000 |
0.000 |
-36.471 |
|
| Traceless |
| | x | y | z |
| x |
3.704 |
0.236 |
0.000 |
| y |
0.236 |
-1.922 |
0.000 |
| z |
0.000 |
0.000 |
-1.782 |
|
| Polar |
| 3z2-r2 | -3.563 |
| x2-y2 | 3.751 |
| xy | 0.236 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.564 |
0.186 |
0.000 |
| y |
0.186 |
6.840 |
0.000 |
| z |
0.000 |
0.000 |
9.101 |
<r2> (average value of r
2) Å
2
| <r2> |
130.235 |
| (<r2>)1/2 |
11.412 |