Jump to
S1C2
Energy calculated at B1B95/6-31G**
| | hartrees |
| Energy at 0K | -342.275683 |
| Energy at 298.15K | |
| HF Energy | -342.275683 |
| Nuclear repulsion energy | 246.588889 |
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 B1B95/6-31G**
| 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 |
3099 |
2959 |
53.33 |
|
|
|
| 2 |
A1 |
1989 |
1899 |
603.31 |
|
|
|
| 3 |
A1 |
1579 |
1508 |
3.76 |
|
|
|
| 4 |
A1 |
1418 |
1354 |
1.84 |
|
|
|
| 5 |
A1 |
1251 |
1194 |
243.50 |
|
|
|
| 6 |
A1 |
967 |
924 |
7.73 |
|
|
|
| 7 |
A1 |
861 |
823 |
30.79 |
|
|
|
| 8 |
A1 |
729 |
696 |
0.89 |
|
|
|
| 9 |
A2 |
3129 |
2987 |
0.00 |
|
|
|
| 10 |
A2 |
1269 |
1211 |
0.00 |
|
|
|
| 11 |
A2 |
1183 |
1129 |
0.00 |
|
|
|
| 12 |
A2 |
178i |
170i |
0.00 |
|
|
|
| 13 |
B1 |
3150 |
3008 |
47.71 |
|
|
|
| 14 |
B1 |
1286 |
1227 |
1.01 |
|
|
|
| 15 |
B1 |
871 |
832 |
0.83 |
|
|
|
| 16 |
B1 |
763 |
728 |
24.07 |
|
|
|
| 17 |
B1 |
142 |
136 |
1.73 |
|
|
|
| 18 |
B2 |
3093 |
2953 |
28.14 |
|
|
|
| 19 |
B2 |
1566 |
1495 |
3.00 |
|
|
|
| 20 |
B2 |
1431 |
1367 |
21.20 |
|
|
|
| 21 |
B2 |
1234 |
1178 |
8.78 |
|
|
|
| 22 |
B2 |
1083 |
1034 |
315.59 |
|
|
|
| 23 |
B2 |
758 |
723 |
0.43 |
|
|
|
| 24 |
B2 |
508 |
485 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16589.0 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 15839.2 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 B1B95/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.861 |
| O2 |
0.000 |
0.000 |
2.045 |
| O3 |
0.000 |
1.123 |
0.056 |
| O4 |
0.000 |
-1.123 |
0.056 |
| C5 |
0.000 |
0.772 |
-1.280 |
| C6 |
0.000 |
-0.772 |
-1.280 |
| H7 |
-0.886 |
1.186 |
-1.766 |
| H8 |
0.886 |
1.186 |
-1.766 |
| H9 |
0.886 |
-1.186 |
-1.766 |
| H10 |
-0.886 |
-1.186 |
-1.766 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1837 | 1.3818 | 1.3818 | 2.2758 | 2.2758 | 3.0156 | 3.0156 | 3.0156 | 3.0156 |
O2 | 1.1837 | | 2.2836 | 2.2836 | 3.4130 | 3.4130 | 4.0883 | 4.0883 | 4.0883 | 4.0883 | O3 | 1.3818 | 2.2836 | | 2.2470 | 1.3818 | 2.3193 | 2.0276 | 2.0276 | 3.0729 | 3.0729 | O4 | 1.3818 | 2.2836 | 2.2470 | | 2.3193 | 1.3818 | 3.0729 | 3.0729 | 2.0276 | 2.0276 | C5 | 2.2758 | 3.4130 | 1.3818 | 2.3193 | | 1.5443 | 1.0925 | 1.0925 | 2.2041 | 2.2041 | C6 | 2.2758 | 3.4130 | 2.3193 | 1.3818 | 1.5443 | | 2.2041 | 2.2041 | 1.0925 | 1.0925 | H7 | 3.0156 | 4.0883 | 2.0276 | 3.0729 | 1.0925 | 2.2041 | | 1.7729 | 2.9620 | 2.3728 | H8 | 3.0156 | 4.0883 | 2.0276 | 3.0729 | 1.0925 | 2.2041 | 1.7729 | | 2.3728 | 2.9620 | H9 | 3.0156 | 4.0883 | 3.0729 | 2.0276 | 2.2041 | 1.0925 | 2.9620 | 2.3728 | | 1.7729 | H10 | 3.0156 | 4.0883 | 3.0729 | 2.0276 | 2.2041 | 1.0925 | 2.3728 | 2.9620 | 1.7729 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.875 |
|
C1 |
O4 |
C6 |
110.875 |
| O2 |
C1 |
O3 |
125.604 |
|
O2 |
C1 |
O4 |
125.604 |
| O3 |
C1 |
O4 |
108.792 |
|
O3 |
C5 |
C6 |
104.729 |
| O3 |
C5 |
H7 |
109.504 |
|
O3 |
C5 |
H8 |
109.504 |
| O4 |
C6 |
C5 |
104.729 |
|
O4 |
C6 |
H9 |
109.504 |
| O4 |
C6 |
H10 |
109.504 |
|
C5 |
C6 |
H9 |
112.281 |
| C5 |
C6 |
H10 |
112.281 |
|
C6 |
C5 |
H7 |
112.281 |
| C6 |
C5 |
H8 |
112.281 |
|
H7 |
C5 |
H8 |
108.460 |
| H9 |
C6 |
H10 |
108.460 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.814 |
|
|
|
| 2 |
O |
-0.439 |
|
|
|
| 3 |
O |
-0.463 |
|
|
|
| 4 |
O |
-0.463 |
|
|
|
| 5 |
C |
-0.097 |
|
|
|
| 6 |
C |
-0.097 |
|
|
|
| 7 |
H |
0.186 |
|
|
|
| 8 |
H |
0.186 |
|
|
|
| 9 |
H |
0.186 |
|
|
|
| 10 |
H |
0.186 |
|
|
|
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 |
-31.712 |
0.000 |
0.000 |
| y |
0.000 |
-35.741 |
0.000 |
| z |
0.000 |
0.000 |
-35.175 |
|
| Traceless |
| | x | y | z |
| x |
3.747 |
0.000 |
0.000 |
| y |
0.000 |
-2.298 |
0.000 |
| z |
0.000 |
0.000 |
-1.449 |
|
| Polar |
| 3z2-r2 | -2.898 |
| x2-y2 | 4.029 |
| 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 |
4.130 |
0.000 |
0.000 |
| y |
0.000 |
4.966 |
0.000 |
| z |
0.000 |
0.000 |
7.134 |
<r2> (average value of r
2) Å
2
| <r2> |
127.565 |
| (<r2>)1/2 |
11.294 |
Jump to
S1C1
Energy calculated at B1B95/6-31G**
| | hartrees |
| Energy at 0K | -342.276494 |
| Energy at 298.15K | -342.282901 |
| HF Energy | -342.276494 |
| Nuclear repulsion energy | 247.189317 |
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 B1B95/6-31G**
| 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 |
3159 |
3016 |
17.25 |
|
|
|
| 2 |
A |
3077 |
2938 |
27.61 |
|
|
|
| 3 |
A |
1992 |
1902 |
585.82 |
|
|
|
| 4 |
A |
1565 |
1494 |
4.05 |
|
|
|
| 5 |
A |
1424 |
1360 |
8.83 |
|
|
|
| 6 |
A |
1275 |
1218 |
30.51 |
|
|
|
| 7 |
A |
1244 |
1187 |
170.86 |
|
|
|
| 8 |
A |
1169 |
1116 |
29.66 |
|
|
|
| 9 |
A |
973 |
929 |
3.05 |
|
|
|
| 10 |
A |
856 |
818 |
34.42 |
|
|
|
| 11 |
A |
726 |
693 |
1.11 |
|
|
|
| 12 |
A |
136 |
130 |
0.56 |
|
|
|
| 13 |
B |
3168 |
3025 |
28.63 |
|
|
|
| 14 |
B |
3082 |
2943 |
49.70 |
|
|
|
| 15 |
B |
1556 |
1486 |
4.19 |
|
|
|
| 16 |
B |
1424 |
1360 |
18.52 |
|
|
|
| 17 |
B |
1289 |
1231 |
4.07 |
|
|
|
| 18 |
B |
1206 |
1152 |
6.57 |
|
|
|
| 19 |
B |
1075 |
1026 |
296.13 |
|
|
|
| 20 |
B |
915 |
874 |
4.99 |
|
|
|
| 21 |
B |
773 |
739 |
25.39 |
|
|
|
| 22 |
B |
688 |
657 |
0.71 |
|
|
|
| 23 |
B |
510 |
487 |
0.02 |
|
|
|
| 24 |
B |
150 |
143 |
1.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16717.1 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 15961.5 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 B1B95/6-31G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.856 |
| O2 |
0.000 |
0.000 |
2.039 |
| O3 |
0.000 |
1.124 |
0.046 |
| O4 |
0.000 |
-1.124 |
0.046 |
| C5 |
0.200 |
0.738 |
-1.270 |
| C6 |
-0.200 |
-0.738 |
-1.270 |
| H7 |
-0.418 |
1.350 |
-1.927 |
| H8 |
1.252 |
0.876 |
-1.540 |
| H9 |
0.418 |
-1.350 |
-1.927 |
| H10 |
-1.252 |
-0.876 |
-1.540 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1833 | 1.3854 | 1.3854 | 2.2586 | 2.2586 | 3.1210 | 2.8418 | 3.1210 | 2.8418 |
O2 | 1.1833 | | 2.2883 | 2.2883 | 3.3958 | 3.3958 | 4.2103 | 3.8918 | 4.2103 | 3.8918 | O3 | 1.3854 | 2.2883 | | 2.2478 | 1.3854 | 2.2882 | 2.0292 | 2.0360 | 3.1914 | 2.8429 | O4 | 1.3854 | 2.2883 | 2.2478 | | 2.2882 | 1.3854 | 3.1914 | 2.8429 | 2.0292 | 2.0360 | C5 | 2.2586 | 3.3958 | 1.3854 | 2.2882 | | 1.5287 | 1.0901 | 1.0953 | 2.1993 | 2.1877 | C6 | 2.2586 | 3.3958 | 2.2882 | 1.3854 | 1.5287 | | 2.1993 | 2.1877 | 1.0901 | 1.0953 | H7 | 3.1210 | 4.2103 | 2.0292 | 3.1914 | 1.0901 | 2.1993 | | 1.7787 | 2.8255 | 2.4080 | H8 | 2.8418 | 3.8918 | 2.0360 | 2.8429 | 1.0953 | 2.1877 | 1.7787 | | 2.4080 | 3.0564 | H9 | 3.1210 | 4.2103 | 3.1914 | 2.0292 | 2.1993 | 1.0901 | 2.8255 | 2.4080 | | 1.7787 | H10 | 2.8418 | 3.8918 | 2.8429 | 2.0360 | 2.1877 | 1.0953 | 2.4080 | 3.0564 | 1.7787 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.206 |
|
C1 |
O4 |
C6 |
109.206 |
| O2 |
C1 |
O3 |
125.780 |
|
O2 |
C1 |
O4 |
125.780 |
| O3 |
C1 |
O4 |
108.440 |
|
O3 |
C5 |
C6 |
103.370 |
| O3 |
C5 |
H7 |
109.537 |
|
O3 |
C5 |
H8 |
109.767 |
| O4 |
C6 |
C5 |
103.370 |
|
O4 |
C6 |
H9 |
109.537 |
| O4 |
C6 |
H10 |
109.767 |
|
C5 |
C6 |
H9 |
113.167 |
| C5 |
C6 |
H10 |
111.900 |
|
C6 |
C5 |
H7 |
113.167 |
| C6 |
C5 |
H8 |
111.900 |
|
H7 |
C5 |
H8 |
108.951 |
| H9 |
C6 |
H10 |
108.951 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.819 |
|
|
|
| 2 |
O |
-0.440 |
|
|
|
| 3 |
O |
-0.463 |
|
|
|
| 4 |
O |
-0.463 |
|
|
|
| 5 |
C |
-0.100 |
|
|
|
| 6 |
C |
-0.100 |
|
|
|
| 7 |
H |
0.190 |
|
|
|
| 8 |
H |
0.183 |
|
|
|
| 9 |
H |
0.190 |
|
|
|
| 10 |
H |
0.183 |
|
|
|
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 |
-4.770 |
4.770 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.769 |
0.226 |
0.000 |
| y |
0.226 |
-35.761 |
0.000 |
| z |
0.000 |
0.000 |
-34.986 |
|
| Traceless |
| | x | y | z |
| x |
3.605 |
0.226 |
0.000 |
| y |
0.226 |
-2.383 |
0.000 |
| z |
0.000 |
0.000 |
-1.221 |
|
| Polar |
| 3z2-r2 | -2.443 |
| x2-y2 | 3.992 |
| xy | 0.226 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.211 |
0.135 |
0.000 |
| y |
0.135 |
4.911 |
0.000 |
| z |
0.000 |
0.000 |
7.103 |
<r2> (average value of r
2) Å
2
| <r2> |
126.431 |
| (<r2>)1/2 |
11.244 |