Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -342.291636 |
| Energy at 298.15K | |
| HF Energy | -342.291636 |
| Nuclear repulsion energy | 246.408802 |
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 B1B95/6-31+G**
| 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 |
3094 |
2960 |
58.81 |
|
|
|
| 2 |
A1 |
1960 |
1875 |
685.39 |
|
|
|
| 3 |
A1 |
1558 |
1490 |
1.93 |
|
|
|
| 4 |
A1 |
1406 |
1345 |
0.42 |
|
|
|
| 5 |
A1 |
1244 |
1190 |
257.91 |
|
|
|
| 6 |
A1 |
963 |
921 |
8.28 |
|
|
|
| 7 |
A1 |
854 |
817 |
36.86 |
|
|
|
| 8 |
A1 |
725 |
694 |
0.86 |
|
|
|
| 9 |
A2 |
3126 |
2990 |
0.00 |
|
|
|
| 10 |
A2 |
1258 |
1203 |
0.00 |
|
|
|
| 11 |
A2 |
1172 |
1121 |
0.00 |
|
|
|
| 12 |
A2 |
185i |
177i |
0.00 |
|
|
|
| 13 |
B1 |
3147 |
3010 |
36.88 |
|
|
|
| 14 |
B1 |
1275 |
1220 |
2.18 |
|
|
|
| 15 |
B1 |
865 |
828 |
0.49 |
|
|
|
| 16 |
B1 |
763 |
730 |
25.01 |
|
|
|
| 17 |
B1 |
137 |
131 |
2.10 |
|
|
|
| 18 |
B2 |
3087 |
2953 |
22.89 |
|
|
|
| 19 |
B2 |
1544 |
1477 |
5.74 |
|
|
|
| 20 |
B2 |
1417 |
1355 |
18.39 |
|
|
|
| 21 |
B2 |
1227 |
1174 |
7.80 |
|
|
|
| 22 |
B2 |
1068 |
1022 |
332.67 |
|
|
|
| 23 |
B2 |
754 |
721 |
1.12 |
|
|
|
| 24 |
B2 |
504 |
482 |
0.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16480.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 15764.8 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 B1B95/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.862 |
| O2 |
0.000 |
0.000 |
2.047 |
| O3 |
0.000 |
1.124 |
0.056 |
| O4 |
0.000 |
-1.124 |
0.056 |
| C5 |
0.000 |
0.772 |
-1.282 |
| C6 |
0.000 |
-0.772 |
-1.282 |
| H7 |
-0.887 |
1.186 |
-1.765 |
| H8 |
0.887 |
1.186 |
-1.765 |
| H9 |
0.887 |
-1.186 |
-1.765 |
| H10 |
-0.887 |
-1.186 |
-1.765 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1847 | 1.3833 | 1.3833 | 2.2789 | 2.2789 | 3.0164 | 3.0164 | 3.0164 | 3.0164 |
O2 | 1.1847 | | 2.2864 | 2.2864 | 3.4172 | 3.4172 | 4.0900 | 4.0900 | 4.0900 | 4.0900 | O3 | 1.3833 | 2.2864 | | 2.2480 | 1.3833 | 2.3204 | 2.0268 | 2.0268 | 3.0725 | 3.0725 | O4 | 1.3833 | 2.2864 | 2.2480 | | 2.3204 | 1.3833 | 3.0725 | 3.0725 | 2.0268 | 2.0268 | C5 | 2.2789 | 3.4172 | 1.3833 | 2.3204 | | 1.5440 | 1.0918 | 1.0918 | 2.2034 | 2.2034 | C6 | 2.2789 | 3.4172 | 2.3204 | 1.3833 | 1.5440 | | 2.2034 | 2.2034 | 1.0918 | 1.0918 | H7 | 3.0164 | 4.0900 | 2.0268 | 3.0725 | 1.0918 | 2.2034 | | 1.7740 | 2.9621 | 2.3722 | H8 | 3.0164 | 4.0900 | 2.0268 | 3.0725 | 1.0918 | 2.2034 | 1.7740 | | 2.3722 | 2.9621 | H9 | 3.0164 | 4.0900 | 3.0725 | 2.0268 | 2.2034 | 1.0918 | 2.9621 | 2.3722 | | 1.7740 | H10 | 3.0164 | 4.0900 | 3.0725 | 2.0268 | 2.2034 | 1.0918 | 2.3722 | 2.9621 | 1.7740 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.915 |
|
C1 |
O4 |
C6 |
110.915 |
| O2 |
C1 |
O3 |
125.655 |
|
O2 |
C1 |
O4 |
125.655 |
| O3 |
C1 |
O4 |
108.689 |
|
O3 |
C5 |
C6 |
104.740 |
| O3 |
C5 |
H7 |
109.382 |
|
O3 |
C5 |
H8 |
109.382 |
| O4 |
C6 |
C5 |
104.740 |
|
O4 |
C6 |
H9 |
109.382 |
| O4 |
C6 |
H10 |
109.382 |
|
C5 |
C6 |
H9 |
112.286 |
| C5 |
C6 |
H10 |
112.286 |
|
C6 |
C5 |
H7 |
112.286 |
| C6 |
C5 |
H8 |
112.286 |
|
H7 |
C5 |
H8 |
108.662 |
| H9 |
C6 |
H10 |
108.662 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.702 |
|
|
|
| 2 |
O |
-0.462 |
|
|
|
| 3 |
O |
-0.357 |
|
|
|
| 4 |
O |
-0.357 |
|
|
|
| 5 |
C |
-0.095 |
|
|
|
| 6 |
C |
-0.095 |
|
|
|
| 7 |
H |
0.166 |
|
|
|
| 8 |
H |
0.166 |
|
|
|
| 9 |
H |
0.166 |
|
|
|
| 10 |
H |
0.166 |
|
|
|
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 |
-5.149 |
5.149 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.225 |
0.000 |
0.000 |
| y |
0.000 |
-36.586 |
0.000 |
| z |
0.000 |
0.000 |
-36.203 |
|
| Traceless |
| | x | y | z |
| x |
4.169 |
0.000 |
0.000 |
| y |
0.000 |
-2.372 |
0.000 |
| z |
0.000 |
0.000 |
-1.797 |
|
| Polar |
| 3z2-r2 | -3.594 |
| x2-y2 | 4.361 |
| 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 |
4.725 |
0.000 |
0.000 |
| y |
0.000 |
5.812 |
0.000 |
| z |
0.000 |
0.000 |
7.973 |
<r2> (average value of r
2) Å
2
| <r2> |
128.221 |
| (<r2>)1/2 |
11.323 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -342.292558 |
| Energy at 298.15K | -342.298960 |
| HF Energy | -342.292558 |
| Nuclear repulsion energy | 247.036923 |
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 B1B95/6-31+G**
| 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 |
3155 |
3018 |
17.51 |
|
|
|
| 2 |
A |
3070 |
2937 |
30.81 |
|
|
|
| 3 |
A |
1965 |
1879 |
664.68 |
|
|
|
| 4 |
A |
1543 |
1476 |
2.25 |
|
|
|
| 5 |
A |
1412 |
1350 |
6.16 |
|
|
|
| 6 |
A |
1265 |
1210 |
35.63 |
|
|
|
| 7 |
A |
1236 |
1182 |
181.96 |
|
|
|
| 8 |
A |
1159 |
1108 |
29.40 |
|
|
|
| 9 |
A |
968 |
926 |
2.97 |
|
|
|
| 10 |
A |
849 |
812 |
40.55 |
|
|
|
| 11 |
A |
722 |
691 |
1.13 |
|
|
|
| 12 |
A |
144 |
138 |
0.62 |
|
|
|
| 13 |
B |
3164 |
3027 |
20.53 |
|
|
|
| 14 |
B |
3075 |
2942 |
44.34 |
|
|
|
| 15 |
B |
1534 |
1468 |
7.28 |
|
|
|
| 16 |
B |
1408 |
1347 |
15.74 |
|
|
|
| 17 |
B |
1279 |
1223 |
6.15 |
|
|
|
| 18 |
B |
1199 |
1147 |
5.81 |
|
|
|
| 19 |
B |
1060 |
1014 |
306.94 |
|
|
|
| 20 |
B |
909 |
869 |
7.84 |
|
|
|
| 21 |
B |
774 |
741 |
25.39 |
|
|
|
| 22 |
B |
684 |
655 |
0.94 |
|
|
|
| 23 |
B |
506 |
484 |
0.10 |
|
|
|
| 24 |
B |
147 |
141 |
1.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16613.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 15892.1 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 B1B95/6-31+G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.857 |
| O2 |
0.000 |
0.000 |
2.041 |
| O3 |
0.000 |
1.124 |
0.045 |
| O4 |
0.000 |
-1.124 |
0.045 |
| C5 |
0.203 |
0.736 |
-1.271 |
| C6 |
-0.203 |
-0.736 |
-1.271 |
| H7 |
-0.410 |
1.350 |
-1.930 |
| H8 |
1.257 |
0.870 |
-1.535 |
| H9 |
0.410 |
-1.350 |
-1.930 |
| H10 |
-1.257 |
-0.870 |
-1.535 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1843 | 1.3869 | 1.3869 | 2.2610 | 2.2610 | 3.1235 | 2.8389 | 3.1235 | 2.8389 |
O2 | 1.1843 | | 2.2912 | 2.2912 | 3.3992 | 3.3992 | 4.2140 | 3.8894 | 4.2140 | 3.8894 | O3 | 1.3869 | 2.2912 | | 2.2487 | 1.3869 | 2.2881 | 2.0291 | 2.0352 | 3.1923 | 2.8381 | O4 | 1.3869 | 2.2912 | 2.2487 | | 2.2881 | 1.3869 | 3.1923 | 2.8381 | 2.0291 | 2.0352 | C5 | 2.2610 | 3.3992 | 1.3869 | 2.2881 | | 1.5279 | 1.0895 | 1.0948 | 2.1980 | 2.1872 | C6 | 2.2610 | 3.3992 | 2.2881 | 1.3869 | 1.5279 | | 2.1980 | 2.1872 | 1.0895 | 1.0948 | H7 | 3.1235 | 4.2140 | 2.0291 | 3.1923 | 1.0895 | 2.1980 | | 1.7796 | 2.8226 | 2.4091 | H8 | 2.8389 | 3.8894 | 2.0352 | 2.8381 | 1.0948 | 2.1872 | 1.7796 | | 2.4091 | 3.0581 | H9 | 3.1235 | 4.2140 | 3.1923 | 2.0291 | 2.1980 | 1.0895 | 2.8226 | 2.4091 | | 1.7796 | H10 | 2.8389 | 3.8894 | 2.8381 | 2.0352 | 2.1872 | 1.0948 | 2.4091 | 3.0581 | 1.7796 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.193 |
|
C1 |
O4 |
C6 |
109.193 |
| O2 |
C1 |
O3 |
125.838 |
|
O2 |
C1 |
O4 |
125.838 |
| O3 |
C1 |
O4 |
108.324 |
|
O3 |
C5 |
C6 |
103.332 |
| O3 |
C5 |
H7 |
109.463 |
|
O3 |
C5 |
H8 |
109.622 |
| O4 |
C6 |
C5 |
103.332 |
|
O4 |
C6 |
H9 |
109.463 |
| O4 |
C6 |
H10 |
109.622 |
|
C5 |
C6 |
H9 |
113.165 |
| C5 |
C6 |
H10 |
111.959 |
|
C6 |
C5 |
H7 |
113.165 |
| C6 |
C5 |
H8 |
111.959 |
|
H7 |
C5 |
H8 |
109.125 |
| H9 |
C6 |
H10 |
109.125 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.714 |
|
|
|
| 2 |
O |
-0.472 |
|
|
|
| 3 |
O |
-0.355 |
|
|
|
| 4 |
O |
-0.355 |
|
|
|
| 5 |
C |
-0.103 |
|
|
|
| 6 |
C |
-0.103 |
|
|
|
| 7 |
H |
0.170 |
|
|
|
| 8 |
H |
0.168 |
|
|
|
| 9 |
H |
0.170 |
|
|
|
| 10 |
H |
0.168 |
|
|
|
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 |
-5.087 |
5.087 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.315 |
0.315 |
0.000 |
| y |
0.315 |
-36.614 |
0.000 |
| z |
0.000 |
0.000 |
-35.961 |
|
| Traceless |
| | x | y | z |
| x |
3.973 |
0.315 |
0.000 |
| y |
0.315 |
-2.477 |
0.000 |
| z |
0.000 |
0.000 |
-1.496 |
|
| Polar |
| 3z2-r2 | -2.992 |
| x2-y2 | 4.300 |
| xy | 0.315 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.860 |
0.151 |
0.000 |
| y |
0.151 |
5.781 |
0.000 |
| z |
0.000 |
0.000 |
7.951 |
<r2> (average value of r
2) Å
2
| <r2> |
127.043 |
| (<r2>)1/2 |
11.271 |