Jump to
S1C2
Energy calculated at MP2/LANL2DZ
| | hartrees |
| Energy at 0K | -341.017398 |
| Energy at 298.15K | |
| HF Energy | -340.393801 |
| Nuclear repulsion energy | 235.970898 |
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/LANL2DZ
| 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 |
3098 |
2984 |
62.33 |
|
|
|
| 2 |
A1 |
1745 |
1681 |
509.03 |
|
|
|
| 3 |
A1 |
1569 |
1511 |
0.40 |
|
|
|
| 4 |
A1 |
1389 |
1338 |
0.39 |
|
|
|
| 5 |
A1 |
1065 |
1025 |
196.69 |
|
|
|
| 6 |
A1 |
928 |
893 |
27.42 |
|
|
|
| 7 |
A1 |
704 |
678 |
52.90 |
|
|
|
| 8 |
A1 |
668 |
643 |
1.55 |
|
|
|
| 9 |
A2 |
3159 |
3042 |
0.00 |
|
|
|
| 10 |
A2 |
1244 |
1198 |
0.00 |
|
|
|
| 11 |
A2 |
1152 |
1109 |
0.00 |
|
|
|
| 12 |
A2 |
158i |
153i |
0.00 |
|
|
|
| 13 |
B1 |
3181 |
3063 |
44.40 |
|
|
|
| 14 |
B1 |
1232 |
1187 |
1.26 |
|
|
|
| 15 |
B1 |
873 |
841 |
0.19 |
|
|
|
| 16 |
B1 |
663 |
639 |
30.71 |
|
|
|
| 17 |
B1 |
138 |
133 |
7.75 |
|
|
|
| 18 |
B2 |
3089 |
2975 |
25.93 |
|
|
|
| 19 |
B2 |
1558 |
1500 |
3.10 |
|
|
|
| 20 |
B2 |
1389 |
1338 |
0.77 |
|
|
|
| 21 |
B2 |
1072 |
1033 |
8.43 |
|
|
|
| 22 |
B2 |
856 |
824 |
318.69 |
|
|
|
| 23 |
B2 |
694 |
668 |
20.46 |
|
|
|
| 24 |
B2 |
448 |
432 |
2.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15876.7 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 15290.9 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/LANL2DZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.919 |
| O2 |
0.000 |
0.000 |
2.145 |
| O3 |
0.000 |
1.178 |
0.055 |
| O4 |
0.000 |
-1.178 |
0.055 |
| C5 |
0.000 |
0.792 |
-1.355 |
| C6 |
0.000 |
-0.792 |
-1.355 |
| H7 |
-0.903 |
1.209 |
-1.822 |
| H8 |
0.903 |
1.209 |
-1.822 |
| H9 |
0.903 |
-1.209 |
-1.822 |
| H10 |
-0.903 |
-1.209 |
-1.822 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.2251 | 1.4613 | 1.4613 | 2.4081 | 2.4081 | 3.1295 | 3.1295 | 3.1295 | 3.1295 |
O2 | 1.2251 | | 2.3991 | 2.3991 | 3.5878 | 3.5878 | 4.2441 | 4.2441 | 4.2441 | 4.2441 | O3 | 1.4613 | 2.3991 | | 2.3558 | 1.4613 | 2.4219 | 2.0831 | 2.0831 | 3.1676 | 3.1676 | O4 | 1.4613 | 2.3991 | 2.3558 | | 2.4219 | 1.4613 | 3.1676 | 3.1676 | 2.0831 | 2.0831 | C5 | 2.4081 | 3.5878 | 1.4613 | 2.4219 | | 1.5835 | 1.0992 | 1.0992 | 2.2440 | 2.2440 | C6 | 2.4081 | 3.5878 | 2.4219 | 1.4613 | 1.5835 | | 2.2440 | 2.2440 | 1.0992 | 1.0992 | H7 | 3.1295 | 4.2441 | 2.0831 | 3.1676 | 1.0992 | 2.2440 | | 1.8064 | 3.0176 | 2.4172 | H8 | 3.1295 | 4.2441 | 2.0831 | 3.1676 | 1.0992 | 2.2440 | 1.8064 | | 2.4172 | 3.0176 | H9 | 3.1295 | 4.2441 | 3.1676 | 2.0831 | 2.2440 | 1.0992 | 3.0176 | 2.4172 | | 1.8064 | H10 | 3.1295 | 4.2441 | 3.1676 | 2.0831 | 2.2440 | 1.0992 | 2.4172 | 3.0176 | 1.8064 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.965 |
|
C1 |
O4 |
C6 |
110.965 |
| O2 |
C1 |
O3 |
126.287 |
|
O2 |
C1 |
O4 |
126.287 |
| O3 |
C1 |
O4 |
107.425 |
|
O3 |
C5 |
C6 |
105.323 |
| O3 |
C5 |
H7 |
108.058 |
|
O3 |
C5 |
H8 |
108.058 |
| O4 |
C6 |
C5 |
105.323 |
|
O4 |
C6 |
H9 |
108.058 |
| O4 |
C6 |
H10 |
108.058 |
|
C5 |
C6 |
H9 |
112.289 |
| C5 |
C6 |
H10 |
112.289 |
|
C6 |
C5 |
H7 |
112.289 |
| C6 |
C5 |
H8 |
112.289 |
|
H7 |
C5 |
H8 |
110.518 |
| H9 |
C6 |
H10 |
110.518 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2/LANL2DZ
| | hartrees |
| Energy at 0K | -341.018011 |
| Energy at 298.15K | -341.024055 |
| HF Energy | -340.393611 |
| Nuclear repulsion energy | 236.365029 |
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/LANL2DZ
| 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 |
3170 |
3053 |
7.58 |
|
|
|
| 2 |
A |
3089 |
2975 |
45.49 |
|
|
|
| 3 |
A |
1745 |
1681 |
493.24 |
|
|
|
| 4 |
A |
1558 |
1500 |
0.51 |
|
|
|
| 5 |
A |
1394 |
1342 |
0.85 |
|
|
|
| 6 |
A |
1238 |
1192 |
14.27 |
|
|
|
| 7 |
A |
1157 |
1115 |
0.38 |
|
|
|
| 8 |
A |
1056 |
1017 |
179.86 |
|
|
|
| 9 |
A |
932 |
897 |
23.46 |
|
|
|
| 10 |
A |
699 |
674 |
56.24 |
|
|
|
| 11 |
A |
664 |
639 |
0.47 |
|
|
|
| 12 |
A |
114 |
110 |
1.00 |
|
|
|
| 13 |
B |
3186 |
3069 |
34.58 |
|
|
|
| 14 |
B |
3085 |
2971 |
39.00 |
|
|
|
| 15 |
B |
1551 |
1493 |
4.48 |
|
|
|
| 16 |
B |
1387 |
1336 |
0.65 |
|
|
|
| 17 |
B |
1227 |
1182 |
1.99 |
|
|
|
| 18 |
B |
1063 |
1024 |
8.96 |
|
|
|
| 19 |
B |
905 |
871 |
60.70 |
|
|
|
| 20 |
B |
831 |
800 |
252.28 |
|
|
|
| 21 |
B |
673 |
648 |
30.15 |
|
|
|
| 22 |
B |
655 |
631 |
12.99 |
|
|
|
| 23 |
B |
449 |
432 |
2.51 |
|
|
|
| 24 |
B |
148 |
143 |
7.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15986.6 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 15396.7 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 MP2/LANL2DZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.915 |
| O2 |
0.000 |
0.000 |
2.140 |
| O3 |
0.000 |
1.179 |
0.045 |
| O4 |
0.000 |
-1.179 |
0.045 |
| C5 |
0.195 |
0.761 |
-1.346 |
| C6 |
-0.195 |
-0.761 |
-1.346 |
| H7 |
-0.465 |
1.372 |
-1.975 |
| H8 |
1.251 |
0.919 |
-1.616 |
| H9 |
0.465 |
-1.372 |
-1.975 |
| H10 |
-1.251 |
-0.919 |
-1.616 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.2251 | 1.4652 | 1.4652 | 2.3933 | 2.3933 | 3.2331 | 2.9694 | 3.2331 | 2.9694 |
O2 | 1.2251 | | 2.4040 | 2.4040 | 3.5733 | 3.5733 | 4.3631 | 4.0645 | 4.3631 | 4.0645 | O3 | 1.4652 | 2.4040 | | 2.3578 | 1.4652 | 2.3949 | 2.0822 | 2.0956 | 3.2870 | 2.9541 | O4 | 1.4652 | 2.4040 | 2.3578 | | 2.3949 | 1.4652 | 3.2870 | 2.9541 | 2.0822 | 2.0956 | C5 | 2.3933 | 3.5733 | 1.4652 | 2.3949 | | 1.5712 | 1.0978 | 1.1012 | 2.2402 | 2.2330 | C6 | 2.3933 | 3.5733 | 2.3949 | 1.4652 | 1.5712 | | 2.2402 | 2.2330 | 1.0978 | 1.1012 | H7 | 3.2331 | 4.3631 | 2.0822 | 3.2870 | 1.0978 | 2.2402 | | 1.8101 | 2.8968 | 2.4486 | H8 | 2.9694 | 4.0645 | 2.0956 | 2.9541 | 1.1012 | 2.2330 | 1.8101 | | 2.4486 | 3.1042 | H9 | 3.2331 | 4.3631 | 3.2870 | 2.0822 | 2.2402 | 1.0978 | 2.8968 | 2.4486 | | 1.8101 | H10 | 2.9694 | 4.0645 | 2.9541 | 2.0956 | 2.2330 | 1.1012 | 2.4486 | 3.1042 | 1.8101 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.520 |
|
C1 |
O4 |
C6 |
109.520 |
| O2 |
C1 |
O3 |
126.427 |
|
O2 |
C1 |
O4 |
126.427 |
| O3 |
C1 |
O4 |
107.146 |
|
O3 |
C5 |
C6 |
104.078 |
| O3 |
C5 |
H7 |
107.810 |
|
O3 |
C5 |
H8 |
108.658 |
| O4 |
C6 |
C5 |
104.078 |
|
O4 |
C6 |
H9 |
107.810 |
| O4 |
C6 |
H10 |
108.658 |
|
C5 |
C6 |
H9 |
112.941 |
| C5 |
C6 |
H10 |
112.159 |
|
C6 |
C5 |
H7 |
112.941 |
| C6 |
C5 |
H8 |
112.159 |
|
H7 |
C5 |
H8 |
110.805 |
| H9 |
C6 |
H10 |
110.805 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability