Jump to
S1C2
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -342.302092 |
| Energy at 298.15K | |
| HF Energy | -342.302092 |
| Nuclear repulsion energy | 246.662514 |
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 B1B95/cc-pVDZ
| 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 |
3080 |
2960 |
56.53 |
|
|
|
| 2 |
A1 |
1980 |
1903 |
633.04 |
|
|
|
| 3 |
A1 |
1528 |
1469 |
2.42 |
|
|
|
| 4 |
A1 |
1392 |
1338 |
2.22 |
|
|
|
| 5 |
A1 |
1248 |
1199 |
241.10 |
|
|
|
| 6 |
A1 |
971 |
933 |
10.10 |
|
|
|
| 7 |
A1 |
861 |
828 |
32.32 |
|
|
|
| 8 |
A1 |
730 |
701 |
0.86 |
|
|
|
| 9 |
A2 |
3110 |
2989 |
0.00 |
|
|
|
| 10 |
A2 |
1245 |
1197 |
0.00 |
|
|
|
| 11 |
A2 |
1159 |
1114 |
0.00 |
|
|
|
| 12 |
A2 |
174i |
167i |
0.00 |
|
|
|
| 13 |
B1 |
3132 |
3010 |
44.95 |
|
|
|
| 14 |
B1 |
1263 |
1214 |
1.55 |
|
|
|
| 15 |
B1 |
855 |
822 |
0.45 |
|
|
|
| 16 |
B1 |
771 |
741 |
21.39 |
|
|
|
| 17 |
B1 |
141 |
135 |
1.46 |
|
|
|
| 18 |
B2 |
3071 |
2952 |
29.39 |
|
|
|
| 19 |
B2 |
1516 |
1457 |
7.11 |
|
|
|
| 20 |
B2 |
1405 |
1351 |
28.78 |
|
|
|
| 21 |
B2 |
1227 |
1180 |
5.79 |
|
|
|
| 22 |
B2 |
1080 |
1038 |
298.43 |
|
|
|
| 23 |
B2 |
761 |
732 |
0.96 |
|
|
|
| 24 |
B2 |
512 |
492 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16431.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15793.8 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 B1B95/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.860 |
| O2 |
0.000 |
0.000 |
2.041 |
| O3 |
0.000 |
1.125 |
0.058 |
| O4 |
0.000 |
-1.125 |
0.058 |
| C5 |
0.000 |
0.770 |
-1.278 |
| C6 |
0.000 |
-0.770 |
-1.278 |
| H7 |
-0.890 |
1.186 |
-1.769 |
| H8 |
0.890 |
1.186 |
-1.769 |
| H9 |
0.890 |
-1.186 |
-1.769 |
| H10 |
-0.890 |
-1.186 |
-1.769 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1818 | 1.3815 | 1.3815 | 2.2719 | 2.2719 | 3.0181 | 3.0181 | 3.0181 | 3.0181 |
O2 | 1.1818 | | 2.2805 | 2.2805 | 3.4073 | 3.4073 | 4.0889 | 4.0889 | 4.0889 | 4.0889 | O3 | 1.3815 | 2.2805 | | 2.2495 | 1.3815 | 2.3182 | 2.0330 | 2.0330 | 3.0769 | 3.0769 | O4 | 1.3815 | 2.2805 | 2.2495 | | 2.3182 | 1.3815 | 3.0769 | 3.0769 | 2.0330 | 2.0330 | C5 | 2.2719 | 3.4073 | 1.3815 | 2.3182 | | 1.5405 | 1.0983 | 1.0983 | 2.2045 | 2.2045 | C6 | 2.2719 | 3.4073 | 2.3182 | 1.3815 | 1.5405 | | 2.2045 | 2.2045 | 1.0983 | 1.0983 | H7 | 3.0181 | 4.0889 | 2.0330 | 3.0769 | 1.0983 | 2.2045 | | 1.7800 | 2.9652 | 2.3714 | H8 | 3.0181 | 4.0889 | 2.0330 | 3.0769 | 1.0983 | 2.2045 | 1.7800 | | 2.3714 | 2.9652 | H9 | 3.0181 | 4.0889 | 3.0769 | 2.0330 | 2.2045 | 1.0983 | 2.9652 | 2.3714 | | 1.7800 | H10 | 3.0181 | 4.0889 | 3.0769 | 2.0330 | 2.2045 | 1.0983 | 2.3714 | 2.9652 | 1.7800 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.626 |
|
C1 |
O4 |
C6 |
110.626 |
| O2 |
C1 |
O3 |
125.494 |
|
O2 |
C1 |
O4 |
125.494 |
| O3 |
C1 |
O4 |
109.012 |
|
O3 |
C5 |
C6 |
104.868 |
| O3 |
C5 |
H7 |
109.604 |
|
O3 |
C5 |
H8 |
109.604 |
| O4 |
C6 |
C5 |
104.868 |
|
O4 |
C6 |
H9 |
109.604 |
| O4 |
C6 |
H10 |
109.604 |
|
C5 |
C6 |
H9 |
112.225 |
| C5 |
C6 |
H10 |
112.225 |
|
C6 |
C5 |
H7 |
112.225 |
| C6 |
C5 |
H8 |
112.225 |
|
H7 |
C5 |
H8 |
108.256 |
| H9 |
C6 |
H10 |
108.256 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.352 |
|
|
|
| 2 |
O |
-0.211 |
|
|
|
| 3 |
O |
-0.266 |
|
|
|
| 4 |
O |
-0.266 |
|
|
|
| 5 |
C |
0.099 |
|
|
|
| 6 |
C |
0.099 |
|
|
|
| 7 |
H |
0.048 |
|
|
|
| 8 |
H |
0.048 |
|
|
|
| 9 |
H |
0.048 |
|
|
|
| 10 |
H |
0.048 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-4.626 |
4.626 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.722 |
0.000 |
0.000 |
| y |
0.000 |
-35.695 |
0.000 |
| z |
0.000 |
0.000 |
-35.265 |
|
| Traceless |
| | x | y | z |
| x |
3.758 |
0.000 |
0.000 |
| y |
0.000 |
-2.201 |
0.000 |
| z |
0.000 |
0.000 |
-1.556 |
|
| Polar |
| 3z2-r2 | -3.113 |
| x2-y2 | 3.973 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.186 |
0.000 |
0.000 |
| y |
0.000 |
5.087 |
0.000 |
| z |
0.000 |
0.000 |
7.198 |
<r2> (average value of r
2) Å
2
| <r2> |
127.466 |
| (<r2>)1/2 |
11.290 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -342.302812 |
| Energy at 298.15K | -342.309219 |
| HF Energy | -342.302812 |
| Nuclear repulsion energy | 247.221078 |
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 B1B95/cc-pVDZ
| 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 |
3143 |
3021 |
18.45 |
|
|
|
| 2 |
A |
3055 |
2937 |
29.45 |
|
|
|
| 3 |
A |
1983 |
1906 |
617.38 |
|
|
|
| 4 |
A |
1515 |
1456 |
2.95 |
|
|
|
| 5 |
A |
1400 |
1346 |
9.70 |
|
|
|
| 6 |
A |
1254 |
1205 |
45.08 |
|
|
|
| 7 |
A |
1239 |
1190 |
166.15 |
|
|
|
| 8 |
A |
1149 |
1104 |
18.53 |
|
|
|
| 9 |
A |
973 |
936 |
4.25 |
|
|
|
| 10 |
A |
856 |
823 |
35.73 |
|
|
|
| 11 |
A |
727 |
699 |
1.06 |
|
|
|
| 12 |
A |
132 |
127 |
0.38 |
|
|
|
| 13 |
B |
3152 |
3030 |
26.14 |
|
|
|
| 14 |
B |
3059 |
2941 |
52.59 |
|
|
|
| 15 |
B |
1507 |
1448 |
8.47 |
|
|
|
| 16 |
B |
1399 |
1344 |
25.45 |
|
|
|
| 17 |
B |
1269 |
1220 |
5.46 |
|
|
|
| 18 |
B |
1199 |
1152 |
4.80 |
|
|
|
| 19 |
B |
1072 |
1030 |
281.66 |
|
|
|
| 20 |
B |
903 |
868 |
3.85 |
|
|
|
| 21 |
B |
778 |
748 |
22.54 |
|
|
|
| 22 |
B |
690 |
664 |
0.54 |
|
|
|
| 23 |
B |
513 |
493 |
0.03 |
|
|
|
| 24 |
B |
149 |
143 |
1.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16557.1 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15914.7 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 B1B95/cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.855 |
| O2 |
0.000 |
0.000 |
2.036 |
| O3 |
0.000 |
1.125 |
0.047 |
| O4 |
0.000 |
-1.125 |
0.047 |
| C5 |
0.193 |
0.738 |
-1.268 |
| C6 |
-0.193 |
-0.738 |
-1.268 |
| H7 |
-0.437 |
1.346 |
-1.928 |
| H8 |
1.247 |
0.887 |
-1.551 |
| H9 |
0.437 |
-1.346 |
-1.928 |
| H10 |
-1.247 |
-0.887 |
-1.551 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1814 | 1.3847 | 1.3847 | 2.2559 | 2.2559 | 3.1215 | 2.8509 | 3.1215 | 2.8509 |
O2 | 1.1814 | | 2.2849 | 2.2849 | 3.3913 | 3.3913 | 4.2088 | 3.8995 | 4.2088 | 3.8995 | O3 | 1.3847 | 2.2849 | | 2.2501 | 1.3847 | 2.2892 | 2.0349 | 2.0407 | 3.1933 | 2.8562 | O4 | 1.3847 | 2.2849 | 2.2501 | | 2.2892 | 1.3847 | 3.1933 | 2.8562 | 2.0349 | 2.0407 | C5 | 2.2559 | 3.3913 | 1.3847 | 2.2892 | | 1.5264 | 1.0957 | 1.1013 | 2.1996 | 2.1900 | C6 | 2.2559 | 3.3913 | 2.2892 | 1.3847 | 1.5264 | | 2.1996 | 2.1900 | 1.0957 | 1.1013 | H7 | 3.1215 | 4.2088 | 2.0349 | 3.1933 | 1.0957 | 2.1996 | | 1.7855 | 2.8299 | 2.4053 | H8 | 2.8509 | 3.8995 | 2.0407 | 2.8562 | 1.1013 | 2.1900 | 1.7855 | | 2.4053 | 3.0610 | H9 | 3.1215 | 4.2088 | 3.1933 | 2.0349 | 2.1996 | 1.0957 | 2.8299 | 2.4053 | | 1.7855 | H10 | 2.8509 | 3.8995 | 2.8562 | 2.0407 | 2.1900 | 1.1013 | 2.4053 | 3.0610 | 1.7855 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.090 |
|
C1 |
O4 |
C6 |
109.090 |
| O2 |
C1 |
O3 |
125.663 |
|
O2 |
C1 |
O4 |
125.663 |
| O3 |
C1 |
O4 |
108.674 |
|
O3 |
C5 |
C6 |
103.588 |
| O3 |
C5 |
H7 |
109.695 |
|
O3 |
C5 |
H8 |
109.820 |
| O4 |
C6 |
C5 |
103.588 |
|
O4 |
C6 |
H9 |
109.695 |
| O4 |
C6 |
H10 |
109.820 |
|
C5 |
C6 |
H9 |
113.019 |
| C5 |
C6 |
H10 |
111.888 |
|
C6 |
C5 |
H7 |
113.019 |
| C6 |
C5 |
H8 |
111.888 |
|
H7 |
C5 |
H8 |
108.716 |
| H9 |
C6 |
H10 |
108.716 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.350 |
|
|
|
| 2 |
O |
-0.208 |
|
|
|
| 3 |
O |
-0.267 |
|
|
|
| 4 |
O |
-0.267 |
|
|
|
| 5 |
C |
0.101 |
|
|
|
| 6 |
C |
0.101 |
|
|
|
| 7 |
H |
0.049 |
|
|
|
| 8 |
H |
0.047 |
|
|
|
| 9 |
H |
0.049 |
|
|
|
| 10 |
H |
0.047 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-4.580 |
4.580 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.805 |
0.160 |
0.000 |
| y |
0.160 |
-35.693 |
0.000 |
| z |
0.000 |
0.000 |
-35.078 |
|
| Traceless |
| | x | y | z |
| x |
3.580 |
0.160 |
0.000 |
| y |
0.160 |
-2.252 |
0.000 |
| z |
0.000 |
0.000 |
-1.329 |
|
| Polar |
| 3z2-r2 | -2.657 |
| x2-y2 | 3.888 |
| xy | 0.160 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.282 |
0.161 |
0.000 |
| y |
0.161 |
5.030 |
0.000 |
| z |
0.000 |
0.000 |
7.165 |
<r2> (average value of r
2) Å
2
| <r2> |
126.412 |
| (<r2>)1/2 |
11.243 |