Jump to
S1C2
Energy calculated at M06-2X/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -342.405698 |
| Energy at 298.15K | |
| HF Energy | -342.405698 |
| Nuclear repulsion energy | 246.705974 |
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 M06-2X/aug-cc-pVTZ
| 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 |
3083 |
2947 |
51.11 |
|
|
|
| 2 |
A1 |
1976 |
1888 |
709.94 |
|
|
|
| 3 |
A1 |
1558 |
1489 |
1.54 |
|
|
|
| 4 |
A1 |
1406 |
1344 |
0.03 |
|
|
|
| 5 |
A1 |
1248 |
1192 |
258.86 |
|
|
|
| 6 |
A1 |
961 |
919 |
8.10 |
|
|
|
| 7 |
A1 |
859 |
821 |
39.21 |
|
|
|
| 8 |
A1 |
735 |
702 |
0.92 |
|
|
|
| 9 |
A2 |
3113 |
2975 |
0.00 |
|
|
|
| 10 |
A2 |
1270 |
1213 |
0.00 |
|
|
|
| 11 |
A2 |
1174 |
1122 |
0.00 |
|
|
|
| 12 |
A2 |
187i |
179i |
0.00 |
|
|
|
| 13 |
B1 |
3134 |
2995 |
26.75 |
|
|
|
| 14 |
B1 |
1281 |
1224 |
3.02 |
|
|
|
| 15 |
B1 |
852 |
814 |
0.83 |
|
|
|
| 16 |
B1 |
788 |
753 |
26.84 |
|
|
|
| 17 |
B1 |
138 |
132 |
1.63 |
|
|
|
| 18 |
B2 |
3078 |
2942 |
14.46 |
|
|
|
| 19 |
B2 |
1546 |
1477 |
6.24 |
|
|
|
| 20 |
B2 |
1426 |
1362 |
16.00 |
|
|
|
| 21 |
B2 |
1234 |
1180 |
4.67 |
|
|
|
| 22 |
B2 |
1071 |
1024 |
309.75 |
|
|
|
| 23 |
B2 |
761 |
728 |
0.84 |
|
|
|
| 24 |
B2 |
518 |
495 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16511.4 cm
-1
Scaled (by 0.9557) Zero Point Vibrational Energy (zpe) 15779.9 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 M06-2X/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.865 |
| O2 |
0.000 |
0.000 |
2.040 |
| O3 |
0.000 |
1.123 |
0.057 |
| O4 |
0.000 |
-1.123 |
0.057 |
| C5 |
0.000 |
0.773 |
-1.281 |
| C6 |
0.000 |
-0.773 |
-1.281 |
| H7 |
-0.886 |
1.183 |
-1.764 |
| H8 |
0.886 |
1.183 |
-1.764 |
| H9 |
0.886 |
-1.183 |
-1.764 |
| H10 |
-0.886 |
-1.183 |
-1.764 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1758 | 1.3834 | 1.3834 | 2.2807 | 2.2807 | 3.0155 | 3.0155 | 3.0155 | 3.0155 |
O2 | 1.1758 | | 2.2792 | 2.2792 | 3.4103 | 3.4103 | 4.0812 | 4.0812 | 4.0812 | 4.0812 | O3 | 1.3834 | 2.2792 | | 2.2469 | 1.3834 | 2.3215 | 2.0261 | 2.0261 | 3.0696 | 3.0696 | O4 | 1.3834 | 2.2792 | 2.2469 | | 2.3215 | 1.3834 | 3.0696 | 3.0696 | 2.0261 | 2.0261 | C5 | 2.2807 | 3.4103 | 1.3834 | 2.3215 | | 1.5468 | 1.0892 | 1.0892 | 2.2016 | 2.2016 | C6 | 2.2807 | 3.4103 | 2.3215 | 1.3834 | 1.5468 | | 2.2016 | 2.2016 | 1.0892 | 1.0892 | H7 | 3.0155 | 4.0812 | 2.0261 | 3.0696 | 1.0892 | 2.2016 | | 1.7725 | 2.9568 | 2.3667 | H8 | 3.0155 | 4.0812 | 2.0261 | 3.0696 | 1.0892 | 2.2016 | 1.7725 | | 2.3667 | 2.9568 | H9 | 3.0155 | 4.0812 | 3.0696 | 2.0261 | 2.2016 | 1.0892 | 2.9568 | 2.3667 | | 1.7725 | H10 | 3.0155 | 4.0812 | 3.0696 | 2.0261 | 2.2016 | 1.0892 | 2.3667 | 2.9568 | 1.7725 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
111.043 |
|
C1 |
O4 |
C6 |
111.043 |
| O2 |
C1 |
O3 |
125.699 |
|
O2 |
C1 |
O4 |
125.699 |
| O3 |
C1 |
O4 |
108.602 |
|
O3 |
C5 |
C6 |
104.656 |
| O3 |
C5 |
H7 |
109.480 |
|
O3 |
C5 |
H8 |
109.480 |
| O4 |
C6 |
C5 |
104.656 |
|
O4 |
C6 |
H9 |
109.480 |
| O4 |
C6 |
H10 |
109.480 |
|
C5 |
C6 |
H9 |
112.107 |
| C5 |
C6 |
H10 |
112.107 |
|
C6 |
C5 |
H7 |
112.107 |
| C6 |
C5 |
H8 |
112.107 |
|
H7 |
C5 |
H8 |
108.908 |
| H9 |
C6 |
H10 |
108.908 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.482 |
|
|
|
| 2 |
O |
-0.608 |
|
|
|
| 3 |
O |
-0.227 |
|
|
|
| 4 |
O |
-0.227 |
|
|
|
| 5 |
C |
-0.256 |
|
|
|
| 6 |
C |
-0.256 |
|
|
|
| 7 |
H |
0.273 |
|
|
|
| 8 |
H |
0.273 |
|
|
|
| 9 |
H |
0.273 |
|
|
|
| 10 |
H |
0.273 |
|
|
|
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 |
-4.919 |
4.919 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.295 |
0.000 |
0.000 |
| y |
0.000 |
-36.412 |
0.000 |
| z |
0.000 |
0.000 |
-36.434 |
|
| Traceless |
| | x | y | z |
| x |
4.128 |
0.000 |
0.000 |
| y |
0.000 |
-2.047 |
0.000 |
| z |
0.000 |
0.000 |
-2.081 |
|
| Polar |
| 3z2-r2 | -4.162 |
| x2-y2 | 4.117 |
| 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 |
5.051 |
0.000 |
0.000 |
| y |
0.000 |
6.276 |
0.000 |
| z |
0.000 |
0.000 |
8.225 |
<r2> (average value of r
2) Å
2
| <r2> |
127.982 |
| (<r2>)1/2 |
11.313 |
Jump to
S1C1
Energy calculated at M06-2X/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -342.406286 |
| Energy at 298.15K | -342.412691 |
| HF Energy | -342.406286 |
| Nuclear repulsion energy | 247.230370 |
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 M06-2X/aug-cc-pVTZ
| 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 |
3151 |
3011 |
14.40 |
|
|
|
| 2 |
A |
3068 |
2933 |
28.10 |
|
|
|
| 3 |
A |
1979 |
1891 |
694.49 |
|
|
|
| 4 |
A |
1552 |
1483 |
1.80 |
|
|
|
| 5 |
A |
1412 |
1349 |
2.42 |
|
|
|
| 6 |
A |
1277 |
1220 |
33.03 |
|
|
|
| 7 |
A |
1244 |
1189 |
192.68 |
|
|
|
| 8 |
A |
1167 |
1116 |
27.32 |
|
|
|
| 9 |
A |
966 |
923 |
2.97 |
|
|
|
| 10 |
A |
856 |
818 |
43.10 |
|
|
|
| 11 |
A |
733 |
700 |
1.14 |
|
|
|
| 12 |
A |
117 |
112 |
0.34 |
|
|
|
| 13 |
B |
3160 |
3020 |
14.55 |
|
|
|
| 14 |
B |
3075 |
2939 |
31.32 |
|
|
|
| 15 |
B |
1543 |
1475 |
6.87 |
|
|
|
| 16 |
B |
1420 |
1357 |
14.23 |
|
|
|
| 17 |
B |
1287 |
1230 |
6.60 |
|
|
|
| 18 |
B |
1213 |
1159 |
3.91 |
|
|
|
| 19 |
B |
1066 |
1019 |
294.96 |
|
|
|
| 20 |
B |
905 |
865 |
6.06 |
|
|
|
| 21 |
B |
794 |
759 |
27.12 |
|
|
|
| 22 |
B |
695 |
664 |
0.59 |
|
|
|
| 23 |
B |
518 |
495 |
0.04 |
|
|
|
| 24 |
B |
144 |
137 |
1.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16670.3 cm
-1
Scaled (by 0.9557) Zero Point Vibrational Energy (zpe) 15931.8 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 M06-2X/aug-cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.860 |
| O2 |
0.000 |
0.000 |
2.036 |
| O3 |
0.000 |
1.123 |
0.048 |
| O4 |
0.000 |
-1.123 |
0.048 |
| C5 |
0.187 |
0.744 |
-1.272 |
| C6 |
-0.187 |
-0.744 |
-1.272 |
| H7 |
-0.453 |
1.341 |
-1.917 |
| H8 |
1.230 |
0.899 |
-1.555 |
| H9 |
0.453 |
-1.341 |
-1.917 |
| H10 |
-1.230 |
-0.899 |
-1.555 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1755 | 1.3863 | 1.3863 | 2.2661 | 2.2661 | 3.1173 | 2.8555 | 3.1173 | 2.8555 |
O2 | 1.1755 | | 2.2833 | 2.2833 | 3.3956 | 3.3956 | 4.1987 | 3.9004 | 4.1987 | 3.9004 | O3 | 1.3863 | 2.2833 | | 2.2469 | 1.3863 | 2.2942 | 2.0285 | 2.0329 | 3.1842 | 2.8586 | O4 | 1.3863 | 2.2833 | 2.2469 | | 2.2942 | 1.3863 | 3.1842 | 2.8586 | 2.0285 | 2.0329 | C5 | 2.2661 | 3.3956 | 1.3863 | 2.2942 | | 1.5335 | 1.0871 | 1.0919 | 2.1979 | 2.1876 | C6 | 2.2661 | 3.3956 | 2.2942 | 1.3863 | 1.5335 | | 2.1979 | 2.1876 | 1.0871 | 1.0919 | H7 | 3.1173 | 4.1987 | 2.0285 | 3.1842 | 1.0871 | 2.1979 | | 1.7771 | 2.8299 | 2.3981 | H8 | 2.8555 | 3.9004 | 2.0329 | 2.8586 | 1.0919 | 2.1876 | 1.7771 | | 2.3981 | 3.0470 | H9 | 3.1173 | 4.1987 | 3.1842 | 2.0285 | 2.1979 | 1.0871 | 2.8299 | 2.3981 | | 1.7771 | H10 | 2.8555 | 3.9004 | 2.8586 | 2.0329 | 2.1876 | 1.0919 | 2.3981 | 3.0470 | 1.7771 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.629 |
|
C1 |
O4 |
C6 |
109.629 |
| O2 |
C1 |
O3 |
125.869 |
|
O2 |
C1 |
O4 |
125.869 |
| O3 |
C1 |
O4 |
108.263 |
|
O3 |
C5 |
C6 |
103.466 |
| O3 |
C5 |
H7 |
109.601 |
|
O3 |
C5 |
H8 |
109.653 |
| O4 |
C6 |
C5 |
103.466 |
|
O4 |
C6 |
H9 |
109.601 |
| O4 |
C6 |
H10 |
109.653 |
|
C5 |
C6 |
H9 |
112.907 |
| C5 |
C6 |
H10 |
111.761 |
|
C6 |
C5 |
H7 |
112.907 |
| C6 |
C5 |
H8 |
111.761 |
|
H7 |
C5 |
H8 |
109.288 |
| H9 |
C6 |
H10 |
109.288 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.515 |
|
|
|
| 2 |
O |
-0.625 |
|
|
|
| 3 |
O |
-0.247 |
|
|
|
| 4 |
O |
-0.247 |
|
|
|
| 5 |
C |
-0.284 |
|
|
|
| 6 |
C |
-0.284 |
|
|
|
| 7 |
H |
0.296 |
|
|
|
| 8 |
H |
0.290 |
|
|
|
| 9 |
H |
0.296 |
|
|
|
| 10 |
H |
0.290 |
|
|
|
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 |
-4.880 |
4.880 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.390 |
0.268 |
0.000 |
| y |
0.268 |
-36.445 |
0.000 |
| z |
0.000 |
0.000 |
-36.225 |
|
| Traceless |
| | x | y | z |
| x |
3.945 |
0.268 |
0.000 |
| y |
0.268 |
-2.138 |
0.000 |
| z |
0.000 |
0.000 |
-1.808 |
|
| Polar |
| 3z2-r2 | -3.615 |
| x2-y2 | 4.055 |
| xy | 0.268 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.169 |
0.144 |
0.000 |
| y |
0.144 |
6.218 |
0.000 |
| z |
0.000 |
0.000 |
8.194 |
<r2> (average value of r
2) Å
2
| <r2> |
127.007 |
| (<r2>)1/2 |
11.270 |