Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-31G*
| | hartrees |
| Energy at 0K | -342.077961 |
| Energy at 298.15K | |
| HF Energy | -341.769804 |
| Nuclear repulsion energy | 244.882549 |
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 B2PLYP=FULL/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 |
3107 |
2947 |
53.19 |
|
|
|
| 2 |
A1 |
1944 |
1843 |
548.70 |
|
|
|
| 3 |
A1 |
1597 |
1515 |
4.41 |
|
|
|
| 4 |
A1 |
1427 |
1353 |
2.02 |
|
|
|
| 5 |
A1 |
1215 |
1152 |
234.62 |
|
|
|
| 6 |
A1 |
966 |
916 |
10.70 |
|
|
|
| 7 |
A1 |
830 |
788 |
34.31 |
|
|
|
| 8 |
A1 |
724 |
687 |
0.50 |
|
|
|
| 9 |
A2 |
3137 |
2975 |
0.00 |
|
|
|
| 10 |
A2 |
1276 |
1210 |
0.00 |
|
|
|
| 11 |
A2 |
1195 |
1133 |
0.00 |
|
|
|
| 12 |
A2 |
180i |
171i |
0.00 |
|
|
|
| 13 |
B1 |
3159 |
2996 |
49.30 |
|
|
|
| 14 |
B1 |
1289 |
1223 |
1.02 |
|
|
|
| 15 |
B1 |
879 |
833 |
0.95 |
|
|
|
| 16 |
B1 |
748 |
710 |
23.53 |
|
|
|
| 17 |
B1 |
142 |
135 |
1.99 |
|
|
|
| 18 |
B2 |
3100 |
2940 |
27.37 |
|
|
|
| 19 |
B2 |
1584 |
1502 |
1.45 |
|
|
|
| 20 |
B2 |
1438 |
1364 |
15.41 |
|
|
|
| 21 |
B2 |
1204 |
1142 |
6.08 |
|
|
|
| 22 |
B2 |
1052 |
998 |
314.94 |
|
|
|
| 23 |
B2 |
754 |
715 |
1.70 |
|
|
|
| 24 |
B2 |
503 |
477 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16544.4 cm
-1
Scaled (by 0.9484) Zero Point Vibrational Energy (zpe) 15690.7 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 B2PLYP=FULL/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.868 |
| O2 |
0.000 |
0.000 |
2.059 |
| O3 |
0.000 |
1.134 |
0.057 |
| O4 |
0.000 |
-1.134 |
0.057 |
| C5 |
0.000 |
0.775 |
-1.291 |
| C6 |
0.000 |
-0.775 |
-1.291 |
| H7 |
-0.888 |
1.190 |
-1.775 |
| H8 |
0.888 |
1.190 |
-1.775 |
| H9 |
0.888 |
-1.190 |
-1.775 |
| H10 |
-0.888 |
-1.190 |
-1.775 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1906 | 1.3941 | 1.3941 | 2.2937 | 2.2937 | 3.0310 | 3.0310 | 3.0310 | 3.0310 |
O2 | 1.1906 | | 2.3007 | 2.3007 | 3.4378 | 3.4378 | 4.1106 | 4.1106 | 4.1106 | 4.1106 | O3 | 1.3941 | 2.3007 | | 2.2674 | 1.3941 | 2.3366 | 2.0359 | 2.0359 | 3.0887 | 3.0887 | O4 | 1.3941 | 2.3007 | 2.2674 | | 2.3366 | 1.3941 | 3.0887 | 3.0887 | 2.0359 | 2.0359 | C5 | 2.2937 | 3.4378 | 1.3941 | 2.3366 | | 1.5508 | 1.0927 | 1.0927 | 2.2100 | 2.2100 | C6 | 2.2937 | 3.4378 | 2.3366 | 1.3941 | 1.5508 | | 2.2100 | 2.2100 | 1.0927 | 1.0927 | H7 | 3.0310 | 4.1106 | 2.0359 | 3.0887 | 1.0927 | 2.2100 | | 1.7756 | 2.9689 | 2.3794 | H8 | 3.0310 | 4.1106 | 2.0359 | 3.0887 | 1.0927 | 2.2100 | 1.7756 | | 2.3794 | 2.9689 | H9 | 3.0310 | 4.1106 | 3.0887 | 2.0359 | 2.2100 | 1.0927 | 2.9689 | 2.3794 | | 1.7756 | H10 | 3.0310 | 4.1106 | 3.0887 | 2.0359 | 2.2100 | 1.0927 | 2.3794 | 2.9689 | 1.7756 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.699 |
|
C1 |
O4 |
C6 |
110.699 |
| O2 |
C1 |
O3 |
125.591 |
|
O2 |
C1 |
O4 |
125.591 |
| O3 |
C1 |
O4 |
108.818 |
|
O3 |
C5 |
C6 |
104.892 |
| O3 |
C5 |
H7 |
109.304 |
|
O3 |
C5 |
H8 |
109.304 |
| O4 |
C6 |
C5 |
104.892 |
|
O4 |
C6 |
H9 |
109.304 |
| O4 |
C6 |
H10 |
109.304 |
|
C5 |
C6 |
H9 |
112.282 |
| C5 |
C6 |
H10 |
112.282 |
|
C6 |
C5 |
H7 |
112.282 |
| C6 |
C5 |
H8 |
112.282 |
|
H7 |
C5 |
H8 |
108.671 |
| H9 |
C6 |
H10 |
108.671 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-31G*
| | hartrees |
| Energy at 0K | -342.078850 |
| Energy at 298.15K | -342.085230 |
| HF Energy | -341.770210 |
| Nuclear repulsion energy | 245.493642 |
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 B2PLYP=FULL/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 |
3163 |
3000 |
15.98 |
|
|
|
| 2 |
A |
3087 |
2927 |
28.75 |
|
|
|
| 3 |
A |
1945 |
1845 |
532.12 |
|
|
|
| 4 |
A |
1583 |
1502 |
4.54 |
|
|
|
| 5 |
A |
1432 |
1358 |
8.17 |
|
|
|
| 6 |
A |
1280 |
1214 |
16.20 |
|
|
|
| 7 |
A |
1219 |
1156 |
116.78 |
|
|
|
| 8 |
A |
1173 |
1112 |
91.30 |
|
|
|
| 9 |
A |
969 |
919 |
5.08 |
|
|
|
| 10 |
A |
826 |
783 |
38.01 |
|
|
|
| 11 |
A |
721 |
684 |
0.69 |
|
|
|
| 12 |
A |
144 |
136 |
0.65 |
|
|
|
| 13 |
B |
3173 |
3010 |
31.02 |
|
|
|
| 14 |
B |
3091 |
2931 |
47.63 |
|
|
|
| 15 |
B |
1575 |
1494 |
2.35 |
|
|
|
| 16 |
B |
1431 |
1357 |
13.38 |
|
|
|
| 17 |
B |
1290 |
1223 |
3.58 |
|
|
|
| 18 |
B |
1182 |
1121 |
5.69 |
|
|
|
| 19 |
B |
1047 |
993 |
286.50 |
|
|
|
| 20 |
B |
916 |
869 |
13.57 |
|
|
|
| 21 |
B |
760 |
721 |
24.57 |
|
|
|
| 22 |
B |
690 |
654 |
1.31 |
|
|
|
| 23 |
B |
503 |
477 |
0.08 |
|
|
|
| 24 |
B |
152 |
144 |
1.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16675.7 cm
-1
Scaled (by 0.9484) Zero Point Vibrational Energy (zpe) 15815.2 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 B2PLYP=FULL/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.863 |
| O2 |
0.000 |
0.000 |
2.053 |
| O3 |
0.000 |
1.134 |
0.045 |
| O4 |
0.000 |
-1.134 |
0.045 |
| C5 |
0.203 |
0.740 |
-1.280 |
| C6 |
-0.203 |
-0.740 |
-1.280 |
| H7 |
-0.413 |
1.355 |
-1.937 |
| H8 |
1.257 |
0.874 |
-1.546 |
| H9 |
0.413 |
-1.355 |
-1.937 |
| H10 |
-1.257 |
-0.874 |
-1.546 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1904 | 1.3976 | 1.3976 | 2.2761 | 2.2761 | 3.1378 | 2.8545 | 3.1378 | 2.8545 |
O2 | 1.1904 | | 2.3056 | 2.3056 | 3.4204 | 3.4204 | 4.2342 | 3.9117 | 4.2342 | 3.9117 | O3 | 1.3976 | 2.3056 | | 2.2675 | 1.3976 | 2.3044 | 2.0370 | 2.0453 | 3.2088 | 2.8539 | O4 | 1.3976 | 2.3056 | 2.2675 | | 2.3044 | 1.3976 | 3.2088 | 2.8539 | 2.0370 | 2.0453 | C5 | 2.2761 | 3.4204 | 1.3976 | 2.3044 | | 1.5354 | 1.0905 | 1.0954 | 2.2062 | 2.1930 | C6 | 2.2761 | 3.4204 | 2.3044 | 1.3976 | 1.5354 | | 2.2062 | 2.1930 | 1.0905 | 1.0954 | H7 | 3.1378 | 4.2342 | 2.0370 | 3.2088 | 1.0905 | 2.2062 | | 1.7814 | 2.8337 | 2.4156 | H8 | 2.8545 | 3.9117 | 2.0453 | 2.8539 | 1.0954 | 2.1930 | 1.7814 | | 2.4156 | 3.0622 | H9 | 3.1378 | 4.2342 | 3.2088 | 2.0370 | 2.2062 | 1.0905 | 2.8337 | 2.4156 | | 1.7814 | H10 | 2.8545 | 3.9117 | 2.8539 | 2.0453 | 2.1930 | 1.0954 | 2.4156 | 3.0622 | 1.7814 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.038 |
|
C1 |
O4 |
C6 |
109.038 |
| O2 |
C1 |
O3 |
125.784 |
|
O2 |
C1 |
O4 |
125.784 |
| O3 |
C1 |
O4 |
108.433 |
|
O3 |
C5 |
C6 |
103.471 |
| O3 |
C5 |
H7 |
109.290 |
|
O3 |
C5 |
H8 |
109.658 |
| O4 |
C6 |
C5 |
103.471 |
|
O4 |
C6 |
H9 |
109.290 |
| O4 |
C6 |
H10 |
109.658 |
|
C5 |
C6 |
H9 |
113.228 |
| C5 |
C6 |
H10 |
111.852 |
|
C6 |
C5 |
H7 |
113.228 |
| C6 |
C5 |
H8 |
111.852 |
|
H7 |
C5 |
H8 |
109.166 |
| H9 |
C6 |
H10 |
109.166 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability