Jump to
S1C2
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -342.351862 |
| Energy at 298.15K | |
| HF Energy | -342.351862 |
| Nuclear repulsion energy | 246.159352 |
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 B3PW91/6-311G*
| 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 |
3065 |
2951 |
64.78 |
|
|
|
| 2 |
A1 |
1956 |
1883 |
631.47 |
|
|
|
| 3 |
A1 |
1562 |
1504 |
1.34 |
|
|
|
| 4 |
A1 |
1407 |
1354 |
0.72 |
|
|
|
| 5 |
A1 |
1216 |
1171 |
241.98 |
|
|
|
| 6 |
A1 |
958 |
922 |
9.30 |
|
|
|
| 7 |
A1 |
841 |
810 |
34.30 |
|
|
|
| 8 |
A1 |
728 |
700 |
0.96 |
|
|
|
| 9 |
A2 |
3090 |
2975 |
0.00 |
|
|
|
| 10 |
A2 |
1264 |
1216 |
0.00 |
|
|
|
| 11 |
A2 |
1175 |
1132 |
0.00 |
|
|
|
| 12 |
A2 |
172i |
166i |
0.00 |
|
|
|
| 13 |
B1 |
3114 |
2997 |
57.44 |
|
|
|
| 14 |
B1 |
1282 |
1235 |
1.36 |
|
|
|
| 15 |
B1 |
865 |
833 |
0.55 |
|
|
|
| 16 |
B1 |
766 |
737 |
23.09 |
|
|
|
| 17 |
B1 |
142 |
137 |
1.85 |
|
|
|
| 18 |
B2 |
3058 |
2944 |
32.79 |
|
|
|
| 19 |
B2 |
1549 |
1491 |
4.66 |
|
|
|
| 20 |
B2 |
1416 |
1364 |
14.70 |
|
|
|
| 21 |
B2 |
1204 |
1159 |
1.38 |
|
|
|
| 22 |
B2 |
1042 |
1003 |
331.19 |
|
|
|
| 23 |
B2 |
755 |
727 |
3.45 |
|
|
|
| 24 |
B2 |
513 |
493 |
0.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16397.4 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 15785.7 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 B3PW91/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.864 |
| O2 |
0.000 |
0.000 |
2.044 |
| O3 |
0.000 |
1.128 |
0.058 |
| O4 |
0.000 |
-1.128 |
0.058 |
| C5 |
0.000 |
0.773 |
-1.283 |
| C6 |
0.000 |
-0.773 |
-1.283 |
| H7 |
-0.888 |
1.190 |
-1.767 |
| H8 |
0.888 |
1.190 |
-1.767 |
| H9 |
0.888 |
-1.190 |
-1.767 |
| H10 |
-0.888 |
-1.190 |
-1.767 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1794 | 1.3865 | 1.3865 | 2.2823 | 2.2823 | 3.0212 | 3.0212 | 3.0212 | 3.0212 |
O2 | 1.1794 | | 2.2839 | 2.2839 | 3.4154 | 3.4154 | 4.0897 | 4.0897 | 4.0897 | 4.0897 | O3 | 1.3865 | 2.2839 | | 2.2553 | 1.3865 | 2.3262 | 2.0301 | 2.0301 | 3.0801 | 3.0801 | O4 | 1.3865 | 2.2839 | 2.2553 | | 2.3262 | 1.3865 | 3.0801 | 3.0801 | 2.0301 | 2.0301 | C5 | 2.2823 | 3.4154 | 1.3865 | 2.3262 | | 1.5469 | 1.0934 | 1.0934 | 2.2082 | 2.2082 | C6 | 2.2823 | 3.4154 | 2.3262 | 1.3865 | 1.5469 | | 2.2082 | 2.2082 | 1.0934 | 1.0934 | H7 | 3.0212 | 4.0897 | 2.0301 | 3.0801 | 1.0934 | 2.2082 | | 1.7753 | 2.9685 | 2.3792 | H8 | 3.0212 | 4.0897 | 2.0301 | 3.0801 | 1.0934 | 2.2082 | 1.7753 | | 2.3792 | 2.9685 | H9 | 3.0212 | 4.0897 | 3.0801 | 2.0301 | 2.2082 | 1.0934 | 2.9685 | 2.3792 | | 1.7753 | H10 | 3.0212 | 4.0897 | 3.0801 | 2.0301 | 2.2082 | 1.0934 | 2.3792 | 2.9685 | 1.7753 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.781 |
|
C1 |
O4 |
C6 |
110.781 |
| O2 |
C1 |
O3 |
125.581 |
|
O2 |
C1 |
O4 |
125.581 |
| O3 |
C1 |
O4 |
108.838 |
|
O3 |
C5 |
C6 |
104.800 |
| O3 |
C5 |
H7 |
109.325 |
|
O3 |
C5 |
H8 |
109.325 |
| O4 |
C6 |
C5 |
104.800 |
|
O4 |
C6 |
H9 |
109.325 |
| O4 |
C6 |
H10 |
109.325 |
|
C5 |
C6 |
H9 |
112.370 |
| C5 |
C6 |
H10 |
112.370 |
|
C6 |
C5 |
H7 |
112.370 |
| C6 |
C5 |
H8 |
112.370 |
|
H7 |
C5 |
H8 |
108.547 |
| H9 |
C6 |
H10 |
108.547 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.517 |
|
|
|
| 2 |
O |
-0.313 |
|
|
|
| 3 |
O |
-0.295 |
|
|
|
| 4 |
O |
-0.295 |
|
|
|
| 5 |
C |
-0.271 |
|
|
|
| 6 |
C |
-0.271 |
|
|
|
| 7 |
H |
0.232 |
|
|
|
| 8 |
H |
0.232 |
|
|
|
| 9 |
H |
0.232 |
|
|
|
| 10 |
H |
0.232 |
|
|
|
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 |
-4.874 |
4.874 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.850 |
0.000 |
0.000 |
| y |
0.000 |
-36.268 |
0.000 |
| z |
0.000 |
0.000 |
-35.537 |
|
| Traceless |
| | x | y | z |
| x |
4.053 |
0.000 |
0.000 |
| y |
0.000 |
-2.574 |
0.000 |
| z |
0.000 |
0.000 |
-1.479 |
|
| Polar |
| 3z2-r2 | -2.957 |
| x2-y2 | 4.418 |
| 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 |
4.253 |
0.000 |
0.000 |
| y |
0.000 |
5.206 |
0.000 |
| z |
0.000 |
0.000 |
7.354 |
<r2> (average value of r
2) Å
2
| <r2> |
128.108 |
| (<r2>)1/2 |
11.318 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -342.352527 |
| Energy at 298.15K | -342.358906 |
| HF Energy | -342.352527 |
| Nuclear repulsion energy | 246.694051 |
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 B3PW91/6-311G*
| 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 |
3119 |
3002 |
22.72 |
|
|
|
| 2 |
A |
3041 |
2927 |
33.43 |
|
|
|
| 3 |
A |
1958 |
1885 |
615.71 |
|
|
|
| 4 |
A |
1549 |
1491 |
1.66 |
|
|
|
| 5 |
A |
1411 |
1359 |
5.44 |
|
|
|
| 6 |
A |
1268 |
1221 |
17.74 |
|
|
|
| 7 |
A |
1216 |
1170 |
165.21 |
|
|
|
| 8 |
A |
1160 |
1116 |
50.89 |
|
|
|
| 9 |
A |
960 |
924 |
3.93 |
|
|
|
| 10 |
A |
837 |
806 |
37.77 |
|
|
|
| 11 |
A |
726 |
699 |
1.18 |
|
|
|
| 12 |
A |
129 |
124 |
0.54 |
|
|
|
| 13 |
B |
3129 |
3013 |
35.78 |
|
|
|
| 14 |
B |
3046 |
2932 |
58.57 |
|
|
|
| 15 |
B |
1540 |
1483 |
6.22 |
|
|
|
| 16 |
B |
1410 |
1357 |
12.99 |
|
|
|
| 17 |
B |
1284 |
1236 |
4.48 |
|
|
|
| 18 |
B |
1182 |
1138 |
3.41 |
|
|
|
| 19 |
B |
1038 |
999 |
300.17 |
|
|
|
| 20 |
B |
901 |
867 |
14.94 |
|
|
|
| 21 |
B |
774 |
746 |
24.21 |
|
|
|
| 22 |
B |
693 |
667 |
1.49 |
|
|
|
| 23 |
B |
512 |
493 |
0.19 |
|
|
|
| 24 |
B |
150 |
144 |
1.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16516.1 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 15900.0 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 B3PW91/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.860 |
| O2 |
0.000 |
0.000 |
2.039 |
| O3 |
0.000 |
1.128 |
0.048 |
| O4 |
0.000 |
-1.128 |
0.048 |
| C5 |
0.189 |
0.743 |
-1.274 |
| C6 |
-0.189 |
-0.743 |
-1.274 |
| H7 |
-0.446 |
1.348 |
-1.922 |
| H8 |
1.237 |
0.899 |
-1.555 |
| H9 |
0.446 |
-1.348 |
-1.922 |
| H10 |
-1.237 |
-0.899 |
-1.555 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1792 | 1.3896 | 1.3896 | 2.2673 | 2.2673 | 3.1235 | 2.8586 | 3.1235 | 2.8586 |
O2 | 1.1792 | | 2.2883 | 2.2883 | 3.4004 | 3.4004 | 4.2080 | 3.9062 | 4.2080 | 3.9062 | O3 | 1.3896 | 2.2883 | | 2.2553 | 1.3896 | 2.2982 | 2.0319 | 2.0379 | 3.1953 | 2.8650 | O4 | 1.3896 | 2.2883 | 2.2553 | | 2.2982 | 1.3896 | 3.1953 | 2.8650 | 2.0319 | 2.0379 | C5 | 2.2673 | 3.4004 | 1.3896 | 2.2982 | | 1.5331 | 1.0910 | 1.0963 | 2.2042 | 2.1928 | C6 | 2.2673 | 3.4004 | 2.2982 | 1.3896 | 1.5331 | | 2.2042 | 2.1928 | 1.0910 | 1.0963 | H7 | 3.1235 | 4.2080 | 2.0319 | 3.1953 | 1.0910 | 2.2042 | | 1.7805 | 2.8402 | 2.4102 | H8 | 2.8586 | 3.9062 | 2.0379 | 2.8650 | 1.0963 | 2.1928 | 1.7805 | | 2.4102 | 3.0584 | H9 | 3.1235 | 4.2080 | 3.1953 | 2.0319 | 2.2042 | 1.0910 | 2.8402 | 2.4102 | | 1.7805 | H10 | 2.8586 | 3.9062 | 2.8650 | 2.0379 | 2.1928 | 1.0963 | 2.4102 | 3.0584 | 1.7805 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.335 |
|
C1 |
O4 |
C6 |
109.335 |
| O2 |
C1 |
O3 |
125.755 |
|
O2 |
C1 |
O4 |
125.755 |
| O3 |
C1 |
O4 |
108.489 |
|
O3 |
C5 |
C6 |
103.581 |
| O3 |
C5 |
H7 |
109.407 |
|
O3 |
C5 |
H8 |
109.564 |
| O4 |
C6 |
C5 |
103.581 |
|
O4 |
C6 |
H9 |
109.407 |
| O4 |
C6 |
H10 |
109.564 |
|
C5 |
C6 |
H9 |
113.203 |
| C5 |
C6 |
H10 |
111.948 |
|
C6 |
C5 |
H7 |
113.203 |
| C6 |
C5 |
H8 |
111.948 |
|
H7 |
C5 |
H8 |
108.978 |
| H9 |
C6 |
H10 |
108.978 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.518 |
|
|
|
| 2 |
O |
-0.310 |
|
|
|
| 3 |
O |
-0.295 |
|
|
|
| 4 |
O |
-0.295 |
|
|
|
| 5 |
C |
-0.273 |
|
|
|
| 6 |
C |
-0.273 |
|
|
|
| 7 |
H |
0.235 |
|
|
|
| 8 |
H |
0.229 |
|
|
|
| 9 |
H |
0.235 |
|
|
|
| 10 |
H |
0.229 |
|
|
|
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 |
-4.819 |
4.819 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.938 |
0.169 |
0.000 |
| y |
0.169 |
-36.270 |
0.000 |
| z |
0.000 |
0.000 |
-35.357 |
|
| Traceless |
| | x | y | z |
| x |
3.876 |
0.169 |
0.000 |
| y |
0.169 |
-2.623 |
0.000 |
| z |
0.000 |
0.000 |
-1.253 |
|
| Polar |
| 3z2-r2 | -2.505 |
| x2-y2 | 4.332 |
| xy | 0.169 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.350 |
0.154 |
0.000 |
| y |
0.154 |
5.159 |
0.000 |
| z |
0.000 |
0.000 |
7.319 |
<r2> (average value of r
2) Å
2
| <r2> |
127.103 |
| (<r2>)1/2 |
11.274 |