Jump to
S1C2
Energy calculated at G2
| | hartrees |
| Energy at 0K | -341.916603 |
| Energy at 298.15K | -341.911393 |
| HF Energy | -340.533414 |
| Nuclear repulsion energy | 249.288848 |
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 HF/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 |
3258 |
3069 |
60.16 |
|
|
|
| 2 |
A1 |
2126 |
2003 |
822.50 |
|
|
|
| 3 |
A1 |
1708 |
1609 |
8.21 |
|
|
|
| 4 |
A1 |
1555 |
1465 |
7.03 |
|
|
|
| 5 |
A1 |
1371 |
1292 |
317.84 |
|
|
|
| 6 |
A1 |
1026 |
967 |
16.43 |
|
|
|
| 7 |
A1 |
929 |
875 |
32.95 |
|
|
|
| 8 |
A1 |
791 |
745 |
1.70 |
|
|
|
| 9 |
A2 |
3280 |
3090 |
0.00 |
|
|
|
| 10 |
A2 |
1381 |
1301 |
0.00 |
|
|
|
| 11 |
A2 |
1292 |
1217 |
0.00 |
|
|
|
| 12 |
A2 |
185i |
175i |
0.00 |
|
|
|
| 13 |
B1 |
3304 |
3113 |
71.60 |
|
|
|
| 14 |
B1 |
1394 |
1313 |
3.13 |
|
|
|
| 15 |
B1 |
932 |
878 |
5.60 |
|
|
|
| 16 |
B1 |
865 |
815 |
49.00 |
|
|
|
| 17 |
B1 |
132 |
124 |
1.82 |
|
|
|
| 18 |
B2 |
3246 |
3058 |
37.24 |
|
|
|
| 19 |
B2 |
1694 |
1597 |
2.51 |
|
|
|
| 20 |
B2 |
1569 |
1479 |
32.65 |
|
|
|
| 21 |
B2 |
1343 |
1266 |
8.67 |
|
|
|
| 22 |
B2 |
1190 |
1122 |
363.75 |
|
|
|
| 23 |
B2 |
828 |
780 |
0.00 |
|
|
|
| 24 |
B2 |
557 |
525 |
0.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17792.2 cm
-1
Scaled (by 0.9422) Zero Point Vibrational Energy (zpe) 16763.8 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 MP2=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 |
2.063 |
| O3 |
0.000 |
1.135 |
0.056 |
| O4 |
0.000 |
-1.135 |
0.056 |
| C5 |
0.000 |
0.773 |
-1.292 |
| C6 |
0.000 |
-0.773 |
-1.292 |
| H7 |
-0.889 |
1.188 |
-1.775 |
| H8 |
0.889 |
1.188 |
-1.775 |
| H9 |
0.889 |
-1.188 |
-1.775 |
| H10 |
-0.889 |
-1.188 |
-1.775 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1945 | 1.3958 | 1.3958 | 2.2945 | 2.2945 | 3.0308 | 3.0308 | 3.0308 | 3.0308 |
O2 | 1.1945 | | 2.3055 | 2.3055 | 3.4427 | 3.4427 | 4.1142 | 4.1142 | 4.1142 | 4.1142 | O3 | 1.3958 | 2.3055 | | 2.2704 | 1.3958 | 2.3364 | 2.0357 | 2.0357 | 3.0883 | 3.0883 | O4 | 1.3958 | 2.3055 | 2.2704 | | 2.3364 | 1.3958 | 3.0883 | 3.0883 | 2.0357 | 2.0357 | C5 | 2.2945 | 3.4427 | 1.3958 | 2.3364 | | 1.5463 | 1.0930 | 1.0930 | 2.2064 | 2.2064 | C6 | 2.2945 | 3.4427 | 2.3364 | 1.3958 | 1.5463 | | 2.2064 | 2.2064 | 1.0930 | 1.0930 | H7 | 3.0308 | 4.1142 | 2.0357 | 3.0883 | 1.0930 | 2.2064 | | 1.7775 | 2.9670 | 2.3756 | H8 | 3.0308 | 4.1142 | 2.0357 | 3.0883 | 1.0930 | 2.2064 | 1.7775 | | 2.3756 | 2.9670 | H9 | 3.0308 | 4.1142 | 3.0883 | 2.0357 | 2.2064 | 1.0930 | 2.9670 | 2.3756 | | 1.7775 | H10 | 3.0308 | 4.1142 | 3.0883 | 2.0357 | 2.2064 | 1.0930 | 2.3756 | 2.9670 | 1.7775 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
112.101 |
|
C1 |
O4 |
C6 |
112.101 |
| O2 |
C1 |
O3 |
125.352 |
|
O2 |
C1 |
O4 |
125.352 |
| O3 |
C1 |
O4 |
109.296 |
|
O3 |
C5 |
C6 |
103.251 |
| O3 |
C5 |
H7 |
109.812 |
|
O3 |
C5 |
H8 |
109.812 |
| O4 |
C6 |
C5 |
103.251 |
|
O4 |
C6 |
H9 |
109.812 |
| O4 |
C6 |
H10 |
109.812 |
|
C5 |
C6 |
H9 |
112.578 |
| C5 |
C6 |
H10 |
112.578 |
|
C6 |
C5 |
H7 |
112.578 |
| C6 |
C5 |
H8 |
112.578 |
|
H7 |
C5 |
H8 |
108.688 |
| H9 |
C6 |
H10 |
108.688 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at G2
| | hartrees |
| Energy at 0K | -341.916387 |
| Energy at 298.15K | -341.923416 |
| HF Energy | -340.533777 |
| Nuclear repulsion energy | 249.685371 |
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 HF/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 |
3300 |
3110 |
22.24 |
|
|
|
| 2 |
A |
3239 |
3052 |
31.91 |
|
|
|
| 3 |
A |
2129 |
2006 |
808.62 |
|
|
|
| 4 |
A |
1700 |
1602 |
8.37 |
|
|
|
| 5 |
A |
1559 |
1469 |
13.52 |
|
|
|
| 6 |
A |
1384 |
1304 |
36.60 |
|
|
|
| 7 |
A |
1365 |
1286 |
244.58 |
|
|
|
| 8 |
A |
1283 |
1209 |
26.01 |
|
|
|
| 9 |
A |
1025 |
966 |
8.98 |
|
|
|
| 10 |
A |
928 |
874 |
36.98 |
|
|
|
| 11 |
A |
789 |
743 |
1.88 |
|
|
|
| 12 |
A |
74 |
70 |
0.48 |
|
|
|
| 13 |
B |
3313 |
3122 |
52.85 |
|
|
|
| 14 |
B |
3238 |
3051 |
57.08 |
|
|
|
| 15 |
B |
1689 |
1591 |
3.14 |
|
|
|
| 16 |
B |
1563 |
1473 |
30.98 |
|
|
|
| 17 |
B |
1397 |
1316 |
7.10 |
|
|
|
| 18 |
B |
1325 |
1249 |
8.86 |
|
|
|
| 19 |
B |
1187 |
1118 |
350.53 |
|
|
|
| 20 |
B |
976 |
919 |
5.16 |
|
|
|
| 21 |
B |
872 |
821 |
51.21 |
|
|
|
| 22 |
B |
768 |
724 |
1.28 |
|
|
|
| 23 |
B |
558 |
526 |
0.43 |
|
|
|
| 24 |
B |
140 |
132 |
1.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17899.4 cm
-1
Scaled (by 0.9422) Zero Point Vibrational Energy (zpe) 16864.8 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 MP2=FULL/6-31G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.861 |
| O2 |
0.000 |
0.000 |
2.055 |
| O3 |
0.000 |
1.135 |
0.041 |
| O4 |
0.000 |
-1.135 |
0.041 |
| C5 |
0.231 |
0.728 |
-1.278 |
| C6 |
-0.231 |
-0.728 |
-1.278 |
| H7 |
-0.340 |
1.366 |
-1.954 |
| H8 |
1.299 |
0.814 |
-1.510 |
| H9 |
0.340 |
-1.366 |
-1.954 |
| H10 |
-1.299 |
-0.814 |
-1.510 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1943 | 1.4002 | 1.4002 | 2.2716 | 2.2716 | 3.1473 | 2.8235 | 3.1473 | 2.8235 |
O2 | 1.1943 | | 2.3120 | 2.3120 | 3.4200 | 3.4200 | 4.2492 | 3.8811 | 4.2492 | 3.8811 | O3 | 1.4002 | 2.3120 | | 2.2703 | 1.4002 | 2.2946 | 2.0370 | 2.0485 | 3.2175 | 2.8097 | O4 | 1.4002 | 2.3120 | 2.2703 | | 2.2946 | 1.4002 | 3.2175 | 2.8097 | 2.0370 | 2.0485 | C5 | 2.2716 | 3.4200 | 1.4002 | 2.2946 | | 1.5271 | 1.0909 | 1.0958 | 2.2028 | 2.1845 | C6 | 2.2716 | 3.4200 | 2.2946 | 1.4002 | 1.5271 | | 2.2028 | 2.1845 | 1.0909 | 1.0958 | H7 | 3.1473 | 4.2492 | 2.0370 | 3.2175 | 1.0909 | 2.2028 | | 1.7851 | 2.8156 | 2.4229 | H8 | 2.8235 | 3.8811 | 2.0485 | 2.8097 | 1.0958 | 2.1845 | 1.7851 | | 2.4229 | 3.0658 | H9 | 3.1473 | 4.2492 | 3.2175 | 2.0370 | 2.2028 | 1.0909 | 2.8156 | 2.4229 | | 1.7851 | H10 | 2.8235 | 3.8811 | 2.8097 | 2.0485 | 2.1845 | 1.0958 | 2.4229 | 3.0658 | 1.7851 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.552 |
|
C1 |
O4 |
C6 |
109.552 |
| O2 |
C1 |
O3 |
125.315 |
|
O2 |
C1 |
O4 |
125.315 |
| O3 |
C1 |
O4 |
109.369 |
|
O3 |
C5 |
C6 |
101.634 |
| O3 |
C5 |
H7 |
109.558 |
|
O3 |
C5 |
H8 |
109.339 |
| O4 |
C6 |
C5 |
101.634 |
|
O4 |
C6 |
H9 |
109.558 |
| O4 |
C6 |
H10 |
109.339 |
|
C5 |
C6 |
H9 |
114.069 |
| C5 |
C6 |
H10 |
112.164 |
|
C6 |
C5 |
H7 |
114.069 |
| C6 |
C5 |
H8 |
112.164 |
|
H7 |
C5 |
H8 |
109.727 |
| H9 |
C6 |
H10 |
109.727 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability