Jump to
S2C1
Energy calculated at MP3=FULL/6-31+G**
| | hartrees |
| Energy at 0K | -192.627444 |
| Energy at 298.15K | -192.633374 |
| HF Energy | -191.976386 |
| Nuclear repulsion energy | 119.519844 |
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 MP3=FULL/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 |
3261 |
3038 |
6.64 |
|
|
|
| 2 |
A1 |
3134 |
2920 |
8.09 |
|
|
|
| 3 |
A1 |
1871 |
1743 |
163.38 |
|
|
|
| 4 |
A1 |
1530 |
1426 |
24.49 |
|
|
|
| 5 |
A1 |
1448 |
1349 |
12.59 |
|
|
|
| 6 |
A1 |
1122 |
1045 |
0.04 |
|
|
|
| 7 |
A1 |
824 |
767 |
0.58 |
|
|
|
| 8 |
A1 |
387 |
360 |
1.18 |
|
|
|
| 9 |
A2 |
3205 |
2986 |
0.00 |
|
|
|
| 10 |
A2 |
1520 |
1416 |
0.00 |
|
|
|
| 11 |
A2 |
920 |
857 |
0.00 |
|
|
|
| 12 |
A2 |
23 |
22 |
0.00 |
|
|
|
| 13 |
B1 |
3211 |
2991 |
20.45 |
|
|
|
| 14 |
B1 |
1539 |
1434 |
21.99 |
|
|
|
| 15 |
B1 |
1156 |
1077 |
0.60 |
|
|
|
| 16 |
B1 |
497 |
463 |
1.16 |
|
|
|
| 17 |
B1 |
132 |
123 |
0.12 |
|
|
|
| 18 |
B2 |
3260 |
3037 |
9.84 |
|
|
|
| 19 |
B2 |
3129 |
2915 |
2.54 |
|
|
|
| 20 |
B2 |
1522 |
1417 |
0.70 |
|
|
|
| 21 |
B2 |
1455 |
1356 |
57.67 |
|
|
|
| 22 |
B2 |
1291 |
1203 |
57.42 |
|
|
|
| 23 |
B2 |
935 |
871 |
3.41 |
|
|
|
| 24 |
B2 |
548 |
511 |
17.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18959.6 cm
-1
Scaled (by 0.9316) Zero Point Vibrational Energy (zpe) 17662.8 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 MP3=FULL/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.186 |
| O2 |
0.000 |
0.000 |
1.399 |
| C3 |
0.000 |
1.286 |
-0.615 |
| C4 |
0.000 |
-1.286 |
-0.615 |
| H5 |
0.000 |
2.137 |
0.059 |
| H6 |
0.000 |
-2.137 |
0.059 |
| H7 |
0.877 |
1.326 |
-1.260 |
| H8 |
-0.877 |
1.326 |
-1.260 |
| H9 |
-0.877 |
-1.326 |
-1.260 |
| H10 |
0.877 |
-1.326 |
-1.260 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.2132 | 1.5152 | 1.5152 | 2.1405 | 2.1405 | 2.1485 | 2.1485 | 2.1485 | 2.1485 |
O2 | 1.2132 | | 2.3897 | 2.3897 | 2.5222 | 2.5222 | 3.0977 | 3.0977 | 3.0977 | 3.0977 | C3 | 1.5152 | 2.3897 | | 2.5727 | 1.0849 | 3.4888 | 1.0895 | 1.0895 | 2.8298 | 2.8298 | C4 | 1.5152 | 2.3897 | 2.5727 | | 3.4888 | 1.0849 | 2.8298 | 2.8298 | 1.0895 | 1.0895 | H5 | 2.1405 | 2.5222 | 1.0849 | 3.4888 | | 4.2734 | 1.7794 | 1.7794 | 3.8073 | 3.8073 | H6 | 2.1405 | 2.5222 | 3.4888 | 1.0849 | 4.2734 | | 3.8073 | 3.8073 | 1.7794 | 1.7794 | H7 | 2.1485 | 3.0977 | 1.0895 | 2.8298 | 1.7794 | 3.8073 | | 1.7548 | 3.1792 | 2.6511 | H8 | 2.1485 | 3.0977 | 1.0895 | 2.8298 | 1.7794 | 3.8073 | 1.7548 | | 2.6511 | 3.1792 | H9 | 2.1485 | 3.0977 | 2.8298 | 1.0895 | 3.8073 | 1.7794 | 3.1792 | 2.6511 | | 1.7548 | H10 | 2.1485 | 3.0977 | 2.8298 | 1.0895 | 3.8073 | 1.7794 | 2.6511 | 3.1792 | 1.7548 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
109.705 |
|
C1 |
C3 |
H7 |
110.075 |
| C1 |
C3 |
H8 |
110.075 |
|
C1 |
C4 |
H6 |
109.705 |
| C1 |
C4 |
H9 |
110.075 |
|
C1 |
C4 |
H10 |
110.075 |
| O2 |
C1 |
C3 |
121.901 |
|
O2 |
C1 |
C4 |
121.901 |
| C3 |
C1 |
C4 |
116.198 |
|
H5 |
C3 |
H7 |
109.837 |
| H5 |
C3 |
H8 |
109.837 |
|
H6 |
C4 |
H9 |
109.837 |
| H6 |
C4 |
H10 |
109.837 |
|
H7 |
C3 |
H8 |
107.278 |
| H9 |
C4 |
H10 |
107.278 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP3=FULL/6-31+G**
| | hartrees |
| Energy at 0K | -192.503007 |
| Energy at 298.15K | -192.509058 |
| HF Energy | -191.893136 |
| Nuclear repulsion energy | 117.539140 |
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 MP3=FULL/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' |
3236 |
3015 |
15.47 |
|
|
|
| 2 |
A' |
3192 |
2974 |
25.17 |
|
|
|
| 3 |
A' |
3094 |
2882 |
39.33 |
|
|
|
| 4 |
A' |
1553 |
1447 |
7.00 |
|
|
|
| 5 |
A' |
1537 |
1432 |
9.50 |
|
|
|
| 6 |
A' |
1462 |
1362 |
0.57 |
|
|
|
| 7 |
A' |
1335 |
1243 |
26.01 |
|
|
|
| 8 |
A' |
1153 |
1074 |
0.26 |
|
|
|
| 9 |
A' |
1006 |
937 |
4.90 |
|
|
|
| 10 |
A' |
830 |
773 |
5.95 |
|
|
|
| 11 |
A' |
403 |
375 |
0.60 |
|
|
|
| 12 |
A' |
332 |
310 |
0.72 |
|
|
|
| 13 |
A' |
205 |
191 |
0.28 |
|
|
|
| 14 |
A" |
3235 |
3014 |
8.66 |
|
|
|
| 15 |
A" |
3193 |
2974 |
4.39 |
|
|
|
| 16 |
A" |
3092 |
2880 |
24.94 |
|
|
|
| 17 |
A" |
1533 |
1428 |
0.17 |
|
|
|
| 18 |
A" |
1523 |
1419 |
5.07 |
|
|
|
| 19 |
A" |
1445 |
1347 |
1.66 |
|
|
|
| 20 |
A" |
1237 |
1153 |
3.74 |
|
|
|
| 21 |
A" |
1001 |
933 |
2.98 |
|
|
|
| 22 |
A" |
989 |
922 |
0.07 |
|
|
|
| 23 |
A" |
380 |
354 |
6.43 |
|
|
|
| 24 |
A" |
190 |
177 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18578.4 cm
-1
Scaled (by 0.9316) Zero Point Vibrational Energy (zpe) 17307.7 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 MP3=FULL/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.185 |
0.266 |
0.000 |
| O2 |
-0.552 |
1.269 |
0.000 |
| C3 |
0.185 |
-0.585 |
1.298 |
| C4 |
0.185 |
-0.585 |
-1.298 |
| H5 |
-0.829 |
-0.674 |
1.688 |
| H6 |
-0.829 |
-0.674 |
-1.688 |
| H7 |
0.578 |
-1.574 |
1.126 |
| H8 |
0.800 |
-0.111 |
2.061 |
| H9 |
0.578 |
-1.574 |
-1.126 |
| H10 |
0.800 |
-0.111 |
-2.061 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.2446 | 1.5522 | 1.5522 | 2.1820 | 2.1820 | 2.1927 | 2.1833 | 2.1927 | 2.1833 |
O2 | 1.2446 | | 2.3802 | 2.3802 | 2.5887 | 2.5887 | 3.2600 | 2.8246 | 3.2600 | 2.8246 | C3 | 1.5522 | 2.3802 | | 2.5965 | 1.0899 | 3.1552 | 1.0782 | 1.0881 | 2.6477 | 3.4475 | C4 | 1.5522 | 2.3802 | 2.5965 | | 3.1552 | 1.0899 | 2.6477 | 3.4475 | 1.0782 | 1.0881 | H5 | 2.1820 | 2.5887 | 1.0899 | 3.1552 | | 3.3766 | 1.7625 | 1.7630 | 3.2728 | 4.1261 | H6 | 2.1820 | 2.5887 | 3.1552 | 1.0899 | 3.3766 | | 3.2728 | 4.1261 | 1.7625 | 1.7630 | H7 | 2.1927 | 3.2600 | 1.0782 | 2.6477 | 1.7625 | 3.2728 | | 1.7499 | 2.2523 | 3.5135 | H8 | 2.1833 | 2.8246 | 1.0881 | 3.4475 | 1.7630 | 4.1261 | 1.7499 | | 3.5135 | 4.1214 | H9 | 2.1927 | 3.2600 | 2.6477 | 1.0782 | 3.2728 | 1.7625 | 2.2523 | 3.5135 | | 1.7499 | H10 | 2.1833 | 2.8246 | 3.4475 | 1.0881 | 4.1261 | 1.7630 | 3.5135 | 4.1214 | 1.7499 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability