Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -342.334980 |
| Energy at 298.15K | |
| HF Energy | -342.334980 |
| Nuclear repulsion energy | 239.471982 |
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/LANL2DZ
| 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 |
3107 |
2986 |
61.88 |
|
|
|
| 2 |
A1 |
1820 |
1750 |
573.23 |
|
|
|
| 3 |
A1 |
1555 |
1495 |
0.03 |
|
|
|
| 4 |
A1 |
1383 |
1330 |
1.08 |
|
|
|
| 5 |
A1 |
1115 |
1072 |
190.11 |
|
|
|
| 6 |
A1 |
941 |
905 |
14.65 |
|
|
|
| 7 |
A1 |
753 |
724 |
34.25 |
|
|
|
| 8 |
A1 |
685 |
658 |
0.53 |
|
|
|
| 9 |
A2 |
3151 |
3029 |
0.00 |
|
|
|
| 10 |
A2 |
1240 |
1192 |
0.00 |
|
|
|
| 11 |
A2 |
1158 |
1113 |
0.00 |
|
|
|
| 12 |
A2 |
150i |
144i |
0.00 |
|
|
|
| 13 |
B1 |
3175 |
3051 |
47.29 |
|
|
|
| 14 |
B1 |
1242 |
1194 |
0.98 |
|
|
|
| 15 |
B1 |
866 |
832 |
0.06 |
|
|
|
| 16 |
B1 |
693 |
666 |
30.24 |
|
|
|
| 17 |
B1 |
140 |
134 |
5.78 |
|
|
|
| 18 |
B2 |
3097 |
2977 |
23.68 |
|
|
|
| 19 |
B2 |
1544 |
1484 |
5.22 |
|
|
|
| 20 |
B2 |
1399 |
1345 |
0.01 |
|
|
|
| 21 |
B2 |
1114 |
1070 |
6.50 |
|
|
|
| 22 |
B2 |
915 |
879 |
317.35 |
|
|
|
| 23 |
B2 |
722 |
694 |
9.09 |
|
|
|
| 24 |
B2 |
463 |
445 |
0.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16063.6 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15440.3 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/LANL2DZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.902 |
| O2 |
0.000 |
0.000 |
2.113 |
| O3 |
0.000 |
1.159 |
0.055 |
| O4 |
0.000 |
-1.159 |
0.055 |
| C5 |
0.000 |
0.784 |
-1.330 |
| C6 |
0.000 |
-0.784 |
-1.330 |
| H7 |
-0.894 |
1.198 |
-1.806 |
| H8 |
0.894 |
1.198 |
-1.806 |
| H9 |
0.894 |
-1.198 |
-1.806 |
| H10 |
-0.894 |
-1.198 |
-1.806 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.2111 | 1.4351 | 1.4351 | 2.3657 | 2.3657 | 3.0923 | 3.0923 | 3.0923 | 3.0923 |
O2 | 1.2111 | | 2.3617 | 2.3617 | 3.5313 | 3.5313 | 4.1936 | 4.1936 | 4.1936 | 4.1936 | O3 | 1.4351 | 2.3617 | | 2.3172 | 1.4351 | 2.3857 | 2.0642 | 2.0642 | 3.1325 | 3.1325 | O4 | 1.4351 | 2.3617 | 2.3172 | | 2.3857 | 1.4351 | 3.1325 | 3.1325 | 2.0642 | 2.0642 | C5 | 2.3657 | 3.5313 | 1.4351 | 2.3857 | | 1.5674 | 1.0934 | 1.0934 | 2.2250 | 2.2250 | C6 | 2.3657 | 3.5313 | 2.3857 | 1.4351 | 1.5674 | | 2.2250 | 2.2250 | 1.0934 | 1.0934 | H7 | 3.0923 | 4.1936 | 2.0642 | 3.1325 | 1.0934 | 2.2250 | | 1.7870 | 2.9889 | 2.3958 | H8 | 3.0923 | 4.1936 | 2.0642 | 3.1325 | 1.0934 | 2.2250 | 1.7870 | | 2.3958 | 2.9889 | H9 | 3.0923 | 4.1936 | 3.1325 | 2.0642 | 2.2250 | 1.0934 | 2.9889 | 2.3958 | | 1.7870 | H10 | 3.0923 | 4.1936 | 3.1325 | 2.0642 | 2.2250 | 1.0934 | 2.3958 | 2.9889 | 1.7870 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
111.022 |
|
C1 |
O4 |
C6 |
111.022 |
| O2 |
C1 |
O3 |
126.165 |
|
O2 |
C1 |
O4 |
126.165 |
| O3 |
C1 |
O4 |
107.670 |
|
O3 |
C5 |
C6 |
105.143 |
| O3 |
C5 |
H7 |
108.690 |
|
O3 |
C5 |
H8 |
108.690 |
| O4 |
C6 |
C5 |
105.143 |
|
O4 |
C6 |
H9 |
108.690 |
| O4 |
C6 |
H10 |
108.690 |
|
C5 |
C6 |
H9 |
112.259 |
| C5 |
C6 |
H10 |
112.259 |
|
C6 |
C5 |
H7 |
112.259 |
| C6 |
C5 |
H8 |
112.259 |
|
H7 |
C5 |
H8 |
109.602 |
| H9 |
C6 |
H10 |
109.602 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.339 |
|
|
|
| 2 |
O |
-0.190 |
|
|
|
| 3 |
O |
-0.272 |
|
|
|
| 4 |
O |
-0.272 |
|
|
|
| 5 |
C |
-0.259 |
|
|
|
| 6 |
C |
-0.259 |
|
|
|
| 7 |
H |
0.228 |
|
|
|
| 8 |
H |
0.228 |
|
|
|
| 9 |
H |
0.228 |
|
|
|
| 10 |
H |
0.228 |
|
|
|
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 |
-5.770 |
5.770 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.239 |
0.000 |
0.000 |
| y |
0.000 |
-38.255 |
0.000 |
| z |
0.000 |
0.000 |
-35.717 |
|
| Traceless |
| | x | y | z |
| x |
4.746 |
0.000 |
0.000 |
| y |
0.000 |
-4.277 |
0.000 |
| z |
0.000 |
0.000 |
-0.469 |
|
| Polar |
| 3z2-r2 | -0.939 |
| x2-y2 | 6.016 |
| 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 |
3.843 |
0.000 |
0.000 |
| y |
0.000 |
5.119 |
0.000 |
| z |
0.000 |
0.000 |
7.625 |
<r2> (average value of r
2) Å
2
| <r2> |
134.812 |
| (<r2>)1/2 |
11.611 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -342.335293 |
| Energy at 298.15K | -342.341383 |
| HF Energy | -342.335293 |
| Nuclear repulsion energy | 239.771755 |
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/LANL2DZ
| 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 |
3165 |
3042 |
10.85 |
|
|
|
| 2 |
A |
3095 |
2974 |
43.78 |
|
|
|
| 3 |
A |
1823 |
1753 |
562.05 |
|
|
|
| 4 |
A |
1546 |
1486 |
0.01 |
|
|
|
| 5 |
A |
1386 |
1332 |
0.03 |
|
|
|
| 6 |
A |
1241 |
1193 |
14.38 |
|
|
|
| 7 |
A |
1164 |
1118 |
11.41 |
|
|
|
| 8 |
A |
1102 |
1059 |
164.69 |
|
|
|
| 9 |
A |
945 |
908 |
11.71 |
|
|
|
| 10 |
A |
749 |
720 |
36.05 |
|
|
|
| 11 |
A |
682 |
656 |
0.79 |
|
|
|
| 12 |
A |
83 |
80 |
0.67 |
|
|
|
| 13 |
B |
3182 |
3058 |
35.95 |
|
|
|
| 14 |
B |
3093 |
2973 |
38.47 |
|
|
|
| 15 |
B |
1539 |
1480 |
6.72 |
|
|
|
| 16 |
B |
1397 |
1343 |
0.18 |
|
|
|
| 17 |
B |
1241 |
1193 |
1.75 |
|
|
|
| 18 |
B |
1101 |
1059 |
6.49 |
|
|
|
| 19 |
B |
924 |
888 |
213.05 |
|
|
|
| 20 |
B |
872 |
838 |
97.93 |
|
|
|
| 21 |
B |
700 |
673 |
28.79 |
|
|
|
| 22 |
B |
684 |
658 |
6.38 |
|
|
|
| 23 |
B |
463 |
445 |
0.95 |
|
|
|
| 24 |
B |
146 |
140 |
5.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16160.9 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15533.8 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/LANL2DZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.899 |
| O2 |
0.000 |
0.000 |
2.109 |
| O3 |
0.000 |
1.160 |
0.048 |
| O4 |
0.000 |
-1.160 |
0.048 |
| C5 |
0.166 |
0.761 |
-1.324 |
| C6 |
-0.166 |
-0.761 |
-1.324 |
| H7 |
-0.521 |
1.342 |
-1.943 |
| H8 |
1.199 |
0.959 |
-1.629 |
| H9 |
0.521 |
-1.342 |
-1.943 |
| H10 |
-1.199 |
-0.959 |
-1.629 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.2106 | 1.4381 | 1.4381 | 2.3552 | 2.3552 | 3.1852 | 2.9573 | 3.1852 | 2.9573 |
O2 | 1.2106 | | 2.3651 | 2.3651 | 3.5205 | 3.5205 | 4.3001 | 4.0411 | 4.3001 | 4.0411 | O3 | 1.4381 | 2.3651 | | 2.3190 | 1.4381 | 2.3660 | 2.0656 | 2.0711 | 3.2393 | 2.9558 | O4 | 1.4381 | 2.3651 | 2.3190 | | 2.3660 | 1.4381 | 3.2393 | 2.9558 | 2.0656 | 2.0711 | C5 | 2.3552 | 3.5205 | 1.4381 | 2.3660 | | 1.5578 | 1.0919 | 1.0955 | 2.2211 | 2.2168 | C6 | 2.3552 | 3.5205 | 2.3660 | 1.4381 | 1.5578 | | 2.2211 | 2.2168 | 1.0919 | 1.0955 | H7 | 3.1852 | 4.3001 | 2.0656 | 3.2393 | 1.0919 | 2.2211 | | 1.7901 | 2.8799 | 2.4196 | H8 | 2.9573 | 4.0411 | 2.0711 | 2.9558 | 1.0955 | 2.2168 | 1.7901 | | 2.4196 | 3.0709 | H9 | 3.1852 | 4.3001 | 3.2393 | 2.0656 | 2.2211 | 1.0919 | 2.8799 | 2.4196 | | 1.7901 | H10 | 2.9573 | 4.0411 | 2.9558 | 2.0711 | 2.2168 | 1.0955 | 2.4196 | 3.0709 | 1.7901 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.933 |
|
C1 |
O4 |
C6 |
109.933 |
| O2 |
C1 |
O3 |
126.268 |
|
O2 |
C1 |
O4 |
126.268 |
| O3 |
C1 |
O4 |
107.463 |
|
O3 |
C5 |
C6 |
104.251 |
| O3 |
C5 |
H7 |
108.685 |
|
O3 |
C5 |
H8 |
108.914 |
| O4 |
C6 |
C5 |
104.251 |
|
O4 |
C6 |
H9 |
108.685 |
| O4 |
C6 |
H10 |
108.914 |
|
C5 |
C6 |
H9 |
112.731 |
| C5 |
C6 |
H10 |
112.163 |
|
C6 |
C5 |
H7 |
112.731 |
| C6 |
C5 |
H8 |
112.163 |
|
H7 |
C5 |
H8 |
109.847 |
| H9 |
C6 |
H10 |
109.847 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.338 |
|
|
|
| 2 |
O |
-0.185 |
|
|
|
| 3 |
O |
-0.274 |
|
|
|
| 4 |
O |
-0.274 |
|
|
|
| 5 |
C |
-0.258 |
|
|
|
| 6 |
C |
-0.258 |
|
|
|
| 7 |
H |
0.230 |
|
|
|
| 8 |
H |
0.225 |
|
|
|
| 9 |
H |
0.230 |
|
|
|
| 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 |
-5.717 |
5.717 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.266 |
0.325 |
0.000 |
| y |
0.325 |
-38.304 |
0.000 |
| z |
0.000 |
0.000 |
-35.582 |
|
| Traceless |
| | x | y | z |
| x |
4.678 |
0.325 |
0.000 |
| y |
0.325 |
-4.380 |
0.000 |
| z |
0.000 |
0.000 |
-0.297 |
|
| Polar |
| 3z2-r2 | -0.595 |
| x2-y2 | 6.039 |
| xy | 0.325 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.899 |
0.112 |
0.000 |
| y |
0.112 |
5.086 |
0.000 |
| z |
0.000 |
0.000 |
7.622 |
<r2> (average value of r
2) Å
2
| <r2> |
134.116 |
| (<r2>)1/2 |
11.581 |