Jump to
S1C2
Energy calculated at B3LYP/3-21G
| | hartrees |
| Energy at 0K | -340.499229 |
| Energy at 298.15K | |
| HF Energy | -340.499229 |
| Nuclear repulsion energy | 240.168350 |
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/3-21G
| 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 |
3088 |
2979 |
37.80 |
|
|
|
| 2 |
A1 |
1910 |
1843 |
453.05 |
|
|
|
| 3 |
A1 |
1591 |
1535 |
2.48 |
|
|
|
| 4 |
A1 |
1376 |
1328 |
0.32 |
|
|
|
| 5 |
A1 |
1107 |
1068 |
182.47 |
|
|
|
| 6 |
A1 |
902 |
870 |
5.97 |
|
|
|
| 7 |
A1 |
762 |
736 |
30.61 |
|
|
|
| 8 |
A1 |
697 |
673 |
2.32 |
|
|
|
| 9 |
A2 |
3114 |
3005 |
0.00 |
|
|
|
| 10 |
A2 |
1268 |
1223 |
0.00 |
|
|
|
| 11 |
A2 |
1146 |
1105 |
0.00 |
|
|
|
| 12 |
A2 |
161i |
155i |
0.00 |
|
|
|
| 13 |
B1 |
3139 |
3029 |
41.96 |
|
|
|
| 14 |
B1 |
1253 |
1209 |
0.14 |
|
|
|
| 15 |
B1 |
872 |
841 |
0.35 |
|
|
|
| 16 |
B1 |
714 |
689 |
23.43 |
|
|
|
| 17 |
B1 |
124 |
120 |
4.02 |
|
|
|
| 18 |
B2 |
3080 |
2972 |
26.36 |
|
|
|
| 19 |
B2 |
1578 |
1523 |
1.40 |
|
|
|
| 20 |
B2 |
1407 |
1357 |
0.05 |
|
|
|
| 21 |
B2 |
1114 |
1075 |
4.37 |
|
|
|
| 22 |
B2 |
933 |
900 |
280.64 |
|
|
|
| 23 |
B2 |
726 |
701 |
4.16 |
|
|
|
| 24 |
B2 |
480 |
463 |
0.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16108.1 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 15542.7 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 B3LYP/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.897 |
| O2 |
0.000 |
0.000 |
2.095 |
| O3 |
0.000 |
1.162 |
0.060 |
| O4 |
0.000 |
-1.162 |
0.060 |
| C5 |
0.000 |
0.786 |
-1.323 |
| C6 |
0.000 |
-0.786 |
-1.323 |
| H7 |
-0.893 |
1.187 |
-1.807 |
| H8 |
0.893 |
1.187 |
-1.807 |
| H9 |
0.893 |
-1.187 |
-1.807 |
| H10 |
-0.893 |
-1.187 |
-1.807 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1982 | 1.4322 | 1.4322 | 2.3548 | 2.3548 | 3.0856 | 3.0856 | 3.0856 | 3.0856 |
O2 | 1.1982 | | 2.3440 | 2.3440 | 3.5072 | 3.5072 | 4.1759 | 4.1759 | 4.1759 | 4.1759 | O3 | 1.4322 | 2.3440 | | 2.3235 | 1.4322 | 2.3885 | 2.0697 | 2.0697 | 3.1305 | 3.1305 | O4 | 1.4322 | 2.3440 | 2.3235 | | 2.3885 | 1.4322 | 3.1305 | 3.1305 | 2.0697 | 2.0697 | C5 | 2.3548 | 3.5072 | 1.4322 | 2.3885 | | 1.5725 | 1.0922 | 1.0922 | 2.2195 | 2.2195 | C6 | 2.3548 | 3.5072 | 2.3885 | 1.4322 | 1.5725 | | 2.2195 | 2.2195 | 1.0922 | 1.0922 | H7 | 3.0856 | 4.1759 | 2.0697 | 3.1305 | 1.0922 | 2.2195 | | 1.7855 | 2.9705 | 2.3740 | H8 | 3.0856 | 4.1759 | 2.0697 | 3.1305 | 1.0922 | 2.2195 | 1.7855 | | 2.3740 | 2.9705 | H9 | 3.0856 | 4.1759 | 3.1305 | 2.0697 | 2.2195 | 1.0922 | 2.9705 | 2.3740 | | 1.7855 | H10 | 3.0856 | 4.1759 | 3.1305 | 2.0697 | 2.2195 | 1.0922 | 2.3740 | 2.9705 | 1.7855 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.590 |
|
C1 |
O4 |
C6 |
110.590 |
| O2 |
C1 |
O3 |
125.790 |
|
O2 |
C1 |
O4 |
125.790 |
| O3 |
C1 |
O4 |
108.420 |
|
O3 |
C5 |
C6 |
105.200 |
| O3 |
C5 |
H7 |
109.408 |
|
O3 |
C5 |
H8 |
109.408 |
| O4 |
C6 |
C5 |
105.200 |
|
O4 |
C6 |
H9 |
109.408 |
| O4 |
C6 |
H10 |
109.408 |
|
C5 |
C6 |
H9 |
111.528 |
| C5 |
C6 |
H10 |
111.528 |
|
C6 |
C5 |
H7 |
111.528 |
| C6 |
C5 |
H8 |
111.528 |
|
H7 |
C5 |
H8 |
109.655 |
| H9 |
C6 |
H10 |
109.655 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.851 |
|
|
|
| 2 |
O |
-0.455 |
|
|
|
| 3 |
O |
-0.487 |
|
|
|
| 4 |
O |
-0.487 |
|
|
|
| 5 |
C |
-0.161 |
|
|
|
| 6 |
C |
-0.161 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.225 |
|
|
|
| 9 |
H |
0.225 |
|
|
|
| 10 |
H |
0.225 |
|
|
|
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 |
-4.898 |
4.898 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.019 |
0.000 |
0.000 |
| y |
0.000 |
-37.061 |
0.000 |
| z |
0.000 |
0.000 |
-34.733 |
|
| Traceless |
| | x | y | z |
| x |
3.878 |
0.000 |
0.000 |
| y |
0.000 |
-3.685 |
0.000 |
| z |
0.000 |
0.000 |
-0.193 |
|
| Polar |
| 3z2-r2 | -0.386 |
| x2-y2 | 5.042 |
| 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 |
3.581 |
0.000 |
0.000 |
| y |
0.000 |
4.593 |
0.000 |
| z |
0.000 |
0.000 |
7.066 |
<r2> (average value of r
2) Å
2
| <r2> |
133.519 |
| (<r2>)1/2 |
11.555 |
Jump to
S1C1
Energy calculated at B3LYP/3-21G
| | hartrees |
| Energy at 0K | -340.499893 |
| Energy at 298.15K | -340.506076 |
| HF Energy | -340.499893 |
| Nuclear repulsion energy | 240.715210 |
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/3-21G
| 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 |
3144 |
3033 |
10.58 |
|
|
|
| 2 |
A |
3068 |
2960 |
20.11 |
|
|
|
| 3 |
A |
1915 |
1848 |
436.60 |
|
|
|
| 4 |
A |
1578 |
1523 |
2.48 |
|
|
|
| 5 |
A |
1390 |
1341 |
5.54 |
|
|
|
| 6 |
A |
1262 |
1218 |
12.97 |
|
|
|
| 7 |
A |
1155 |
1115 |
5.37 |
|
|
|
| 8 |
A |
1091 |
1053 |
153.63 |
|
|
|
| 9 |
A |
915 |
883 |
3.38 |
|
|
|
| 10 |
A |
757 |
730 |
31.99 |
|
|
|
| 11 |
A |
694 |
670 |
3.10 |
|
|
|
| 12 |
A |
116 |
112 |
0.59 |
|
|
|
| 13 |
B |
3155 |
3044 |
25.86 |
|
|
|
| 14 |
B |
3073 |
2965 |
43.47 |
|
|
|
| 15 |
B |
1572 |
1517 |
2.39 |
|
|
|
| 16 |
B |
1406 |
1357 |
0.21 |
|
|
|
| 17 |
B |
1253 |
1209 |
0.82 |
|
|
|
| 18 |
B |
1097 |
1059 |
5.20 |
|
|
|
| 19 |
B |
949 |
916 |
164.31 |
|
|
|
| 20 |
B |
887 |
855 |
103.12 |
|
|
|
| 21 |
B |
724 |
698 |
24.78 |
|
|
|
| 22 |
B |
664 |
641 |
1.48 |
|
|
|
| 23 |
B |
479 |
463 |
0.90 |
|
|
|
| 24 |
B |
136 |
132 |
3.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16239.6 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 15669.6 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/3-21G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.892 |
| O2 |
0.000 |
0.000 |
2.090 |
| O3 |
0.000 |
1.163 |
0.048 |
| O4 |
0.000 |
-1.163 |
0.048 |
| C5 |
0.208 |
0.749 |
-1.312 |
| C6 |
-0.208 |
-0.749 |
-1.312 |
| H7 |
-0.415 |
1.356 |
-1.970 |
| H8 |
1.263 |
0.866 |
-1.578 |
| H9 |
0.415 |
-1.356 |
-1.970 |
| H10 |
-1.263 |
-0.866 |
-1.578 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1977 | 1.4368 | 1.4368 | 2.3378 | 2.3378 | 3.1942 | 2.9068 | 3.1942 | 2.9068 |
O2 | 1.1977 | | 2.3498 | 2.3498 | 3.4901 | 3.4901 | 4.3005 | 3.9752 | 4.3005 | 3.9752 | O3 | 1.4368 | 2.3498 | | 2.3252 | 1.4368 | 2.3557 | 2.0693 | 2.0804 | 3.2537 | 2.8906 | O4 | 1.4368 | 2.3498 | 2.3252 | | 2.3557 | 1.4368 | 3.2537 | 2.8906 | 2.0693 | 2.0804 | C5 | 2.3378 | 3.4901 | 1.4368 | 2.3557 | | 1.5550 | 1.0897 | 1.0945 | 2.2150 | 2.2004 | C6 | 2.3378 | 3.4901 | 2.3557 | 1.4368 | 1.5550 | | 2.2150 | 2.2004 | 1.0897 | 1.0945 | H7 | 3.1942 | 4.3005 | 2.0693 | 3.2537 | 1.0897 | 2.2150 | | 1.7909 | 2.8353 | 2.4100 | H8 | 2.9068 | 3.9752 | 2.0804 | 2.8906 | 1.0945 | 2.2004 | 1.7909 | | 2.4100 | 3.0624 | H9 | 3.1942 | 4.3005 | 3.2537 | 2.0693 | 2.2150 | 1.0897 | 2.8353 | 2.4100 | | 1.7909 | H10 | 2.9068 | 3.9752 | 2.8906 | 2.0804 | 2.2004 | 1.0945 | 2.4100 | 3.0624 | 1.7909 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.879 |
|
C1 |
O4 |
C6 |
108.879 |
| O2 |
C1 |
O3 |
125.987 |
|
O2 |
C1 |
O4 |
125.987 |
| O3 |
C1 |
O4 |
108.026 |
|
O3 |
C5 |
C6 |
103.808 |
| O3 |
C5 |
H7 |
109.201 |
|
O3 |
C5 |
H8 |
109.802 |
| O4 |
C6 |
C5 |
103.808 |
|
O4 |
C6 |
H9 |
109.201 |
| O4 |
C6 |
H10 |
109.802 |
|
C5 |
C6 |
H9 |
112.569 |
| C5 |
C6 |
H10 |
111.106 |
|
C6 |
C5 |
H7 |
112.569 |
| C6 |
C5 |
H8 |
111.106 |
|
H7 |
C5 |
H8 |
110.152 |
| H9 |
C6 |
H10 |
110.152 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.848 |
|
|
|
| 2 |
O |
-0.454 |
|
|
|
| 3 |
O |
-0.485 |
|
|
|
| 4 |
O |
-0.485 |
|
|
|
| 5 |
C |
-0.162 |
|
|
|
| 6 |
C |
-0.162 |
|
|
|
| 7 |
H |
0.227 |
|
|
|
| 8 |
H |
0.222 |
|
|
|
| 9 |
H |
0.227 |
|
|
|
| 10 |
H |
0.222 |
|
|
|
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 |
-4.830 |
4.830 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.061 |
0.240 |
0.000 |
| y |
0.240 |
-37.106 |
0.000 |
| z |
0.000 |
0.000 |
-34.561 |
|
| Traceless |
| | x | y | z |
| x |
3.773 |
0.240 |
0.000 |
| y |
0.240 |
-3.795 |
0.000 |
| z |
0.000 |
0.000 |
0.022 |
|
| Polar |
| 3z2-r2 | 0.045 |
| x2-y2 | 5.046 |
| xy | 0.240 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.664 |
0.124 |
0.000 |
| y |
0.124 |
4.527 |
0.000 |
| z |
0.000 |
0.000 |
7.037 |
<r2> (average value of r
2) Å
2
| <r2> |
132.359 |
| (<r2>)1/2 |
11.505 |