Jump to
S1C2
Energy calculated at MP2=FULL/6-311G**
| | hartrees |
| Energy at 0K | -341.722730 |
| Energy at 298.15K | |
| HF Energy | -340.611678 |
| Nuclear repulsion energy | 245.693900 |
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 MP2=FULL/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 |
3116 |
2956 |
56.09 |
|
|
|
| 2 |
A1 |
1943 |
1843 |
561.29 |
|
|
|
| 3 |
A1 |
1574 |
1493 |
2.38 |
|
|
|
| 4 |
A1 |
1420 |
1347 |
0.88 |
|
|
|
| 5 |
A1 |
1231 |
1168 |
239.18 |
|
|
|
| 6 |
A1 |
980 |
930 |
14.02 |
|
|
|
| 7 |
A1 |
838 |
795 |
43.47 |
|
|
|
| 8 |
A1 |
725 |
688 |
0.13 |
|
|
|
| 9 |
A2 |
3156 |
2993 |
0.00 |
|
|
|
| 10 |
A2 |
1269 |
1204 |
0.00 |
|
|
|
| 11 |
A2 |
1184 |
1123 |
0.00 |
|
|
|
| 12 |
A2 |
207i |
196i |
0.00 |
|
|
|
| 13 |
B1 |
3178 |
3014 |
42.63 |
|
|
|
| 14 |
B1 |
1294 |
1227 |
1.98 |
|
|
|
| 15 |
B1 |
870 |
825 |
1.02 |
|
|
|
| 16 |
B1 |
762 |
723 |
21.06 |
|
|
|
| 17 |
B1 |
131 |
124 |
2.24 |
|
|
|
| 18 |
B2 |
3109 |
2949 |
24.82 |
|
|
|
| 19 |
B2 |
1561 |
1481 |
4.06 |
|
|
|
| 20 |
B2 |
1429 |
1356 |
15.55 |
|
|
|
| 21 |
B2 |
1223 |
1160 |
5.88 |
|
|
|
| 22 |
B2 |
1049 |
995 |
323.37 |
|
|
|
| 23 |
B2 |
755 |
716 |
2.31 |
|
|
|
| 24 |
B2 |
515 |
489 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16551.1 cm
-1
Scaled (by 0.9486) Zero Point Vibrational Energy (zpe) 15700.4 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 MP2=FULL/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 |
2.048 |
| O3 |
0.000 |
1.132 |
0.058 |
| O4 |
0.000 |
-1.132 |
0.058 |
| C5 |
0.000 |
0.773 |
-1.285 |
| C6 |
0.000 |
-0.773 |
-1.285 |
| H7 |
-0.890 |
1.181 |
-1.769 |
| H8 |
0.890 |
1.181 |
-1.769 |
| H9 |
0.890 |
-1.181 |
-1.769 |
| H10 |
-0.890 |
-1.181 |
-1.769 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1843 | 1.3898 | 1.3898 | 2.2838 | 2.2838 | 3.0200 | 3.0200 | 3.0200 | 3.0200 |
O2 | 1.1843 | | 2.2899 | 2.2899 | 3.4218 | 3.4218 | 4.0939 | 4.0939 | 4.0939 | 4.0939 | O3 | 1.3898 | 2.2899 | | 2.2644 | 1.3898 | 2.3312 | 2.0329 | 2.0329 | 3.0790 | 3.0790 | O4 | 1.3898 | 2.2899 | 2.2644 | | 2.3312 | 1.3898 | 3.0790 | 3.0790 | 2.0329 | 2.0329 | C5 | 2.2838 | 3.4218 | 1.3898 | 2.3312 | | 1.5470 | 1.0920 | 1.0920 | 2.2013 | 2.2013 | C6 | 2.2838 | 3.4218 | 2.3312 | 1.3898 | 1.5470 | | 2.2013 | 2.2013 | 1.0920 | 1.0920 | H7 | 3.0200 | 4.0939 | 2.0329 | 3.0790 | 1.0920 | 2.2013 | | 1.7797 | 2.9571 | 2.3616 | H8 | 3.0200 | 4.0939 | 2.0329 | 3.0790 | 1.0920 | 2.2013 | 1.7797 | | 2.3616 | 2.9571 | H9 | 3.0200 | 4.0939 | 3.0790 | 2.0329 | 2.2013 | 1.0920 | 2.9571 | 2.3616 | | 1.7797 | H10 | 3.0200 | 4.0939 | 3.0790 | 2.0329 | 2.2013 | 1.0920 | 2.3616 | 2.9571 | 1.7797 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.495 |
|
C1 |
O4 |
C6 |
110.495 |
| O2 |
C1 |
O3 |
125.451 |
|
O2 |
C1 |
O4 |
125.451 |
| O3 |
C1 |
O4 |
109.099 |
|
O3 |
C5 |
C6 |
104.956 |
| O3 |
C5 |
H7 |
109.410 |
|
O3 |
C5 |
H8 |
109.410 |
| O4 |
C6 |
C5 |
104.956 |
|
O4 |
C6 |
H9 |
109.410 |
| O4 |
C6 |
H10 |
109.410 |
|
C5 |
C6 |
H9 |
111.900 |
| C5 |
C6 |
H10 |
111.900 |
|
C6 |
C5 |
H7 |
111.900 |
| C6 |
C5 |
H8 |
111.900 |
|
H7 |
C5 |
H8 |
109.158 |
| H9 |
C6 |
H10 |
109.158 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2=FULL/6-311G**
| | hartrees |
| Energy at 0K | -341.724655 |
| Energy at 298.15K | -341.731165 |
| HF Energy | -340.611706 |
| Nuclear repulsion energy | 246.586776 |
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 MP2=FULL/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 |
3183 |
3019 |
14.86 |
|
|
|
| 2 |
A |
3094 |
2935 |
28.98 |
|
|
|
| 3 |
A |
1945 |
1845 |
537.96 |
|
|
|
| 4 |
A |
1559 |
1478 |
3.26 |
|
|
|
| 5 |
A |
1433 |
1359 |
8.93 |
|
|
|
| 6 |
A |
1281 |
1215 |
16.05 |
|
|
|
| 7 |
A |
1228 |
1165 |
155.10 |
|
|
|
| 8 |
A |
1168 |
1108 |
53.59 |
|
|
|
| 9 |
A |
981 |
931 |
4.74 |
|
|
|
| 10 |
A |
833 |
790 |
48.29 |
|
|
|
| 11 |
A |
722 |
685 |
0.35 |
|
|
|
| 12 |
A |
197 |
187 |
0.87 |
|
|
|
| 13 |
B |
3193 |
3029 |
24.46 |
|
|
|
| 14 |
B |
3098 |
2939 |
46.89 |
|
|
|
| 15 |
B |
1552 |
1472 |
5.87 |
|
|
|
| 16 |
B |
1420 |
1347 |
12.11 |
|
|
|
| 17 |
B |
1299 |
1232 |
7.22 |
|
|
|
| 18 |
B |
1191 |
1130 |
5.66 |
|
|
|
| 19 |
B |
1044 |
990 |
280.45 |
|
|
|
| 20 |
B |
924 |
876 |
20.04 |
|
|
|
| 21 |
B |
778 |
738 |
22.81 |
|
|
|
| 22 |
B |
673 |
639 |
1.60 |
|
|
|
| 23 |
B |
515 |
489 |
0.12 |
|
|
|
| 24 |
B |
150 |
142 |
1.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16729.4 cm
-1
Scaled (by 0.9486) Zero Point Vibrational Energy (zpe) 15869.5 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 MP2=FULL/6-311G**
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 |
2.040 |
| O3 |
0.000 |
1.132 |
0.042 |
| O4 |
0.000 |
-1.132 |
0.042 |
| C5 |
0.238 |
0.725 |
-1.270 |
| C6 |
-0.238 |
-0.725 |
-1.270 |
| H7 |
-0.320 |
1.363 |
-1.955 |
| H8 |
1.309 |
0.791 |
-1.491 |
| H9 |
0.320 |
-1.363 |
-1.955 |
| H10 |
-1.309 |
-0.791 |
-1.491 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1842 | 1.3942 | 1.3942 | 2.2591 | 2.2591 | 3.1404 | 2.8013 | 3.1404 | 2.8013 |
O2 | 1.1842 | | 2.2966 | 2.2966 | 3.3973 | 3.3973 | 4.2334 | 3.8481 | 4.2334 | 3.8481 | O3 | 1.3942 | 2.2966 | | 2.2636 | 1.3942 | 2.2862 | 2.0355 | 2.0442 | 3.2115 | 2.7857 | O4 | 1.3942 | 2.2966 | 2.2636 | | 2.2862 | 1.3942 | 3.2115 | 2.7857 | 2.0355 | 2.0442 | C5 | 2.2591 | 3.3973 | 1.3942 | 2.2862 | | 1.5265 | 1.0897 | 1.0952 | 2.1990 | 2.1775 | C6 | 2.2591 | 3.3973 | 2.2862 | 1.3942 | 1.5265 | | 2.1990 | 2.1775 | 1.0897 | 1.0952 | H7 | 3.1404 | 4.2334 | 2.0355 | 3.2115 | 1.0897 | 2.1990 | | 1.7878 | 2.8001 | 2.4153 | H8 | 2.8013 | 3.8481 | 2.0442 | 2.7857 | 1.0952 | 2.1775 | 1.7878 | | 2.4153 | 3.0590 | H9 | 3.1404 | 4.2334 | 3.2115 | 2.0355 | 2.1990 | 1.0897 | 2.8001 | 2.4153 | | 1.7878 | H10 | 2.8013 | 3.8481 | 2.7857 | 2.0442 | 2.1775 | 1.0952 | 2.4153 | 3.0590 | 1.7878 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.224 |
|
C1 |
O4 |
C6 |
108.224 |
| O2 |
C1 |
O3 |
125.728 |
|
O2 |
C1 |
O4 |
125.728 |
| O3 |
C1 |
O4 |
108.543 |
|
O3 |
C5 |
C6 |
102.932 |
| O3 |
C5 |
H7 |
109.454 |
|
O3 |
C5 |
H8 |
109.821 |
| O4 |
C6 |
C5 |
102.932 |
|
O4 |
C6 |
H9 |
109.454 |
| O4 |
C6 |
H10 |
109.821 |
|
C5 |
C6 |
H9 |
113.340 |
| C5 |
C6 |
H10 |
111.249 |
|
C6 |
C5 |
H7 |
113.340 |
| C6 |
C5 |
H8 |
111.249 |
|
H7 |
C5 |
H8 |
109.817 |
| H9 |
C6 |
H10 |
109.817 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability