Jump to
S1C2
Energy calculated at B3LYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -342.534153 |
| Energy at 298.15K | |
| HF Energy | -342.534153 |
| Nuclear repulsion energy | 245.474857 |
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 B3LYP/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 |
3050 |
2951 |
63.53 |
|
|
|
| 2 |
A1 |
1910 |
1848 |
653.92 |
|
|
|
| 3 |
A1 |
1551 |
1501 |
1.16 |
|
|
|
| 4 |
A1 |
1395 |
1350 |
0.05 |
|
|
|
| 5 |
A1 |
1185 |
1146 |
242.40 |
|
|
|
| 6 |
A1 |
943 |
912 |
9.21 |
|
|
|
| 7 |
A1 |
820 |
794 |
41.00 |
|
|
|
| 8 |
A1 |
722 |
699 |
0.96 |
|
|
|
| 9 |
A2 |
3069 |
2969 |
0.00 |
|
|
|
| 10 |
A2 |
1260 |
1219 |
0.00 |
|
|
|
| 11 |
A2 |
1171 |
1133 |
0.00 |
|
|
|
| 12 |
A2 |
163i |
157i |
0.00 |
|
|
|
| 13 |
B1 |
3093 |
2992 |
39.61 |
|
|
|
| 14 |
B1 |
1270 |
1229 |
2.35 |
|
|
|
| 15 |
B1 |
862 |
834 |
0.43 |
|
|
|
| 16 |
B1 |
763 |
738 |
22.23 |
|
|
|
| 17 |
B1 |
146 |
141 |
1.53 |
|
|
|
| 18 |
B2 |
3043 |
2944 |
21.54 |
|
|
|
| 19 |
B2 |
1540 |
1490 |
4.50 |
|
|
|
| 20 |
B2 |
1414 |
1368 |
10.79 |
|
|
|
| 21 |
B2 |
1176 |
1138 |
0.63 |
|
|
|
| 22 |
B2 |
1018 |
985 |
302.08 |
|
|
|
| 23 |
B2 |
745 |
720 |
4.85 |
|
|
|
| 24 |
B2 |
504 |
487 |
0.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16242.2 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 15714.4 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 B3LYP/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.870 |
| O2 |
0.000 |
0.000 |
2.051 |
| O3 |
0.000 |
1.131 |
0.058 |
| O4 |
0.000 |
-1.131 |
0.058 |
| C5 |
0.000 |
0.775 |
-1.288 |
| C6 |
0.000 |
-0.775 |
-1.288 |
| H7 |
-0.886 |
1.187 |
-1.772 |
| H8 |
0.886 |
1.187 |
-1.772 |
| H9 |
0.886 |
-1.187 |
-1.772 |
| H10 |
-0.886 |
-1.187 |
-1.772 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1805 | 1.3924 | 1.3924 | 2.2935 | 2.2935 | 3.0288 | 3.0288 | 3.0288 | 3.0288 |
O2 | 1.1805 | | 2.2914 | 2.2914 | 3.4278 | 3.4278 | 4.0993 | 4.0993 | 4.0993 | 4.0993 | O3 | 1.3924 | 2.2914 | | 2.2615 | 1.3924 | 2.3331 | 2.0333 | 2.0333 | 3.0829 | 3.0829 | O4 | 1.3924 | 2.2914 | 2.2615 | | 2.3331 | 1.3924 | 3.0829 | 3.0829 | 2.0333 | 2.0333 | C5 | 2.2935 | 3.4278 | 1.3924 | 2.3331 | | 1.5498 | 1.0902 | 1.0902 | 2.2065 | 2.2065 | C6 | 2.2935 | 3.4278 | 2.3331 | 1.3924 | 1.5498 | | 2.2065 | 2.2065 | 1.0902 | 1.0902 | H7 | 3.0288 | 4.0993 | 2.0333 | 3.0829 | 1.0902 | 2.2065 | | 1.7719 | 2.9629 | 2.3746 | H8 | 3.0288 | 4.0993 | 2.0333 | 3.0829 | 1.0902 | 2.2065 | 1.7719 | | 2.3746 | 2.9629 | H9 | 3.0288 | 4.0993 | 3.0829 | 2.0333 | 2.2065 | 1.0902 | 2.9629 | 2.3746 | | 1.7719 | H10 | 3.0288 | 4.0993 | 3.0829 | 2.0333 | 2.2065 | 1.0902 | 2.3746 | 2.9629 | 1.7719 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.891 |
|
C1 |
O4 |
C6 |
110.891 |
| O2 |
C1 |
O3 |
125.699 |
|
O2 |
C1 |
O4 |
125.699 |
| O3 |
C1 |
O4 |
108.602 |
|
O3 |
C5 |
C6 |
104.808 |
| O3 |
C5 |
H7 |
109.377 |
|
O3 |
C5 |
H8 |
109.377 |
| O4 |
C6 |
C5 |
104.808 |
|
O4 |
C6 |
H9 |
109.377 |
| O4 |
C6 |
H10 |
109.377 |
|
C5 |
C6 |
H9 |
112.230 |
| C5 |
C6 |
H10 |
112.230 |
|
C6 |
C5 |
H7 |
112.230 |
| C6 |
C5 |
H8 |
112.230 |
|
H7 |
C5 |
H8 |
108.717 |
| H9 |
C6 |
H10 |
108.717 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.426 |
|
|
|
| 2 |
O |
-0.483 |
|
|
|
| 3 |
O |
-0.326 |
|
|
|
| 4 |
O |
-0.326 |
|
|
|
| 5 |
C |
-0.084 |
|
|
|
| 6 |
C |
-0.084 |
|
|
|
| 7 |
H |
0.219 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
| 9 |
H |
0.219 |
|
|
|
| 10 |
H |
0.219 |
|
|
|
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 |
-4.899 |
4.899 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.422 |
0.000 |
0.000 |
| y |
0.000 |
-36.547 |
0.000 |
| z |
0.000 |
0.000 |
-36.646 |
|
| Traceless |
| | x | y | z |
| x |
4.175 |
0.000 |
0.000 |
| y |
0.000 |
-2.013 |
0.000 |
| z |
0.000 |
0.000 |
-2.162 |
|
| Polar |
| 3z2-r2 | -4.324 |
| x2-y2 | 4.125 |
| 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 |
5.206 |
0.000 |
0.000 |
| y |
0.000 |
6.536 |
0.000 |
| z |
0.000 |
0.000 |
8.548 |
<r2> (average value of r
2) Å
2
| <r2> |
129.141 |
| (<r2>)1/2 |
11.364 |
Jump to
S1C1
Energy calculated at B3LYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -342.534557 |
| Energy at 298.15K | -342.540871 |
| HF Energy | -342.534557 |
| Nuclear repulsion energy | 245.885948 |
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 B3LYP/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 |
3094 |
2993 |
20.74 |
|
|
|
| 2 |
A |
3027 |
2929 |
34.86 |
|
|
|
| 3 |
A |
1913 |
1851 |
642.11 |
|
|
|
| 4 |
A |
1541 |
1491 |
1.38 |
|
|
|
| 5 |
A |
1398 |
1353 |
1.05 |
|
|
|
| 6 |
A |
1261 |
1220 |
15.50 |
|
|
|
| 7 |
A |
1191 |
1153 |
124.65 |
|
|
|
| 8 |
A |
1151 |
1114 |
98.86 |
|
|
|
| 9 |
A |
945 |
914 |
4.72 |
|
|
|
| 10 |
A |
817 |
790 |
44.04 |
|
|
|
| 11 |
A |
721 |
697 |
1.18 |
|
|
|
| 12 |
A |
98 |
95 |
0.31 |
|
|
|
| 13 |
B |
3105 |
3004 |
24.40 |
|
|
|
| 14 |
B |
3033 |
2934 |
41.01 |
|
|
|
| 15 |
B |
1533 |
1484 |
5.37 |
|
|
|
| 16 |
B |
1407 |
1362 |
9.41 |
|
|
|
| 17 |
B |
1270 |
1229 |
4.64 |
|
|
|
| 18 |
B |
1160 |
1123 |
2.43 |
|
|
|
| 19 |
B |
1015 |
982 |
276.58 |
|
|
|
| 20 |
B |
887 |
858 |
17.43 |
|
|
|
| 21 |
B |
768 |
743 |
22.20 |
|
|
|
| 22 |
B |
696 |
674 |
2.11 |
|
|
|
| 23 |
B |
504 |
487 |
0.47 |
|
|
|
| 24 |
B |
151 |
146 |
1.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16342.9 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 15811.8 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 B3LYP/aug-cc-pVTZ
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 |
2.047 |
| O3 |
0.000 |
1.131 |
0.050 |
| O4 |
0.000 |
-1.131 |
0.050 |
| C5 |
0.168 |
0.751 |
-1.282 |
| C6 |
-0.168 |
-0.751 |
-1.282 |
| H7 |
-0.500 |
1.334 |
-1.912 |
| H8 |
1.201 |
0.938 |
-1.587 |
| H9 |
0.500 |
-1.334 |
-1.912 |
| H10 |
-1.201 |
-0.938 |
-1.587 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1802 | 1.3949 | 1.3949 | 2.2819 | 2.2819 | 3.1225 | 2.8885 | 3.1225 | 2.8885 |
O2 | 1.1802 | | 2.2949 | 2.2949 | 3.4163 | 3.4163 | 4.2074 | 3.9407 | 4.2074 | 3.9407 | O3 | 1.3949 | 2.2949 | | 2.2614 | 1.3949 | 2.3110 | 2.0349 | 2.0394 | 3.1893 | 2.8985 | O4 | 1.3949 | 2.2949 | 2.2614 | | 2.3110 | 1.3949 | 3.1893 | 2.8985 | 2.0349 | 2.0394 | C5 | 2.2819 | 3.4163 | 1.3949 | 2.3110 | | 1.5385 | 1.0881 | 1.0927 | 2.2025 | 2.1952 | C6 | 2.2819 | 3.4163 | 2.3110 | 1.3949 | 1.5385 | | 2.2025 | 2.1952 | 1.0881 | 1.0927 | H7 | 3.1225 | 4.2074 | 2.0349 | 3.1893 | 1.0881 | 2.2025 | | 1.7758 | 2.8483 | 2.3992 | H8 | 2.8885 | 3.9407 | 2.0394 | 2.8985 | 1.0927 | 2.1952 | 1.7758 | | 2.3992 | 3.0470 | H9 | 3.1225 | 4.2074 | 3.1893 | 2.0349 | 2.2025 | 1.0881 | 2.8483 | 2.3992 | | 1.7758 | H10 | 2.8885 | 3.9407 | 2.8985 | 2.0394 | 2.1952 | 1.0927 | 2.3992 | 3.0470 | 1.7758 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.760 |
|
C1 |
O4 |
C6 |
109.760 |
| O2 |
C1 |
O3 |
125.844 |
|
O2 |
C1 |
O4 |
125.844 |
| O3 |
C1 |
O4 |
108.311 |
|
O3 |
C5 |
C6 |
103.855 |
| O3 |
C5 |
H7 |
109.452 |
|
O3 |
C5 |
H8 |
109.537 |
| O4 |
C6 |
C5 |
103.855 |
|
O4 |
C6 |
H9 |
109.452 |
| O4 |
C6 |
H10 |
109.537 |
|
C5 |
C6 |
H9 |
112.847 |
| C5 |
C6 |
H10 |
111.967 |
|
C6 |
C5 |
H7 |
112.847 |
| C6 |
C5 |
H8 |
111.967 |
|
H7 |
C5 |
H8 |
109.037 |
| H9 |
C6 |
H10 |
109.037 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.446 |
|
|
|
| 2 |
O |
-0.493 |
|
|
|
| 3 |
O |
-0.338 |
|
|
|
| 4 |
O |
-0.338 |
|
|
|
| 5 |
C |
-0.094 |
|
|
|
| 6 |
C |
-0.094 |
|
|
|
| 7 |
H |
0.243 |
|
|
|
| 8 |
H |
0.213 |
|
|
|
| 9 |
H |
0.243 |
|
|
|
| 10 |
H |
0.213 |
|
|
|
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 |
-4.867 |
4.867 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.506 |
0.223 |
0.000 |
| y |
0.223 |
-36.573 |
0.000 |
| z |
0.000 |
0.000 |
-36.472 |
|
| Traceless |
| | x | y | z |
| x |
4.017 |
0.223 |
0.000 |
| y |
0.223 |
-2.084 |
0.000 |
| z |
0.000 |
0.000 |
-1.933 |
|
| Polar |
| 3z2-r2 | -3.866 |
| x2-y2 | 4.067 |
| xy | 0.223 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.305 |
0.152 |
0.000 |
| y |
0.152 |
6.481 |
0.000 |
| z |
0.000 |
0.000 |
8.519 |
<r2> (average value of r
2) Å
2
| <r2> |
128.359 |
| (<r2>)1/2 |
11.330 |