Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -342.360767 |
| Energy at 298.15K | |
| HF Energy | -342.360767 |
| Nuclear repulsion energy | 247.123838 |
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 B1B95/6-311G*
| 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 |
3087 |
2959 |
64.37 |
|
|
|
| 2 |
A1 |
1976 |
1895 |
649.74 |
|
|
|
| 3 |
A1 |
1569 |
1504 |
1.70 |
|
|
|
| 4 |
A1 |
1414 |
1355 |
0.93 |
|
|
|
| 5 |
A1 |
1240 |
1189 |
252.38 |
|
|
|
| 6 |
A1 |
966 |
926 |
8.83 |
|
|
|
| 7 |
A1 |
855 |
819 |
34.45 |
|
|
|
| 8 |
A1 |
730 |
700 |
1.02 |
|
|
|
| 9 |
A2 |
3112 |
2984 |
0.00 |
|
|
|
| 10 |
A2 |
1271 |
1218 |
0.00 |
|
|
|
| 11 |
A2 |
1180 |
1131 |
0.00 |
|
|
|
| 12 |
A2 |
182i |
174i |
0.00 |
|
|
|
| 13 |
B1 |
3136 |
3006 |
57.24 |
|
|
|
| 14 |
B1 |
1290 |
1237 |
1.52 |
|
|
|
| 15 |
B1 |
868 |
832 |
0.77 |
|
|
|
| 16 |
B1 |
774 |
742 |
24.17 |
|
|
|
| 17 |
B1 |
137 |
132 |
1.85 |
|
|
|
| 18 |
B2 |
3079 |
2952 |
32.22 |
|
|
|
| 19 |
B2 |
1556 |
1491 |
4.99 |
|
|
|
| 20 |
B2 |
1424 |
1365 |
17.84 |
|
|
|
| 21 |
B2 |
1224 |
1173 |
2.42 |
|
|
|
| 22 |
B2 |
1061 |
1017 |
333.68 |
|
|
|
| 23 |
B2 |
758 |
726 |
1.94 |
|
|
|
| 24 |
B2 |
515 |
493 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16519.5 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 15835.6 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 B1B95/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.861 |
| O2 |
0.000 |
0.000 |
2.037 |
| O3 |
0.000 |
1.122 |
0.057 |
| O4 |
0.000 |
-1.122 |
0.057 |
| C5 |
0.000 |
0.771 |
-1.278 |
| C6 |
0.000 |
-0.771 |
-1.278 |
| H7 |
-0.885 |
1.185 |
-1.761 |
| H8 |
0.885 |
1.185 |
-1.761 |
| H9 |
0.885 |
-1.185 |
-1.761 |
| H10 |
-0.885 |
-1.185 |
-1.761 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1760 | 1.3804 | 1.3804 | 2.2731 | 2.2731 | 3.0104 | 3.0104 | 3.0104 | 3.0104 |
O2 | 1.1760 | | 2.2757 | 2.2757 | 3.4029 | 3.4029 | 4.0760 | 4.0760 | 4.0760 | 4.0760 | O3 | 1.3804 | 2.2757 | | 2.2446 | 1.3804 | 2.3161 | 2.0234 | 2.0234 | 3.0680 | 3.0680 | O4 | 1.3804 | 2.2757 | 2.2446 | | 2.3161 | 1.3804 | 3.0680 | 3.0680 | 2.0234 | 2.0234 | C5 | 2.2731 | 3.4029 | 1.3804 | 2.3161 | | 1.5410 | 1.0904 | 1.0904 | 2.2001 | 2.2001 | C6 | 2.2731 | 3.4029 | 2.3161 | 1.3804 | 1.5410 | | 2.2001 | 2.2001 | 1.0904 | 1.0904 | H7 | 3.0104 | 4.0760 | 2.0234 | 3.0680 | 1.0904 | 2.2001 | | 1.7703 | 2.9577 | 2.3694 | H8 | 3.0104 | 4.0760 | 2.0234 | 3.0680 | 1.0904 | 2.2001 | 1.7703 | | 2.3694 | 2.9577 | H9 | 3.0104 | 4.0760 | 3.0680 | 2.0234 | 2.2001 | 1.0904 | 2.9577 | 2.3694 | | 1.7703 | H10 | 3.0104 | 4.0760 | 3.0680 | 2.0234 | 2.2001 | 1.0904 | 2.3694 | 2.9577 | 1.7703 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.844 |
|
C1 |
O4 |
C6 |
110.844 |
| O2 |
C1 |
O3 |
125.608 |
|
O2 |
C1 |
O4 |
125.608 |
| O3 |
C1 |
O4 |
108.785 |
|
O3 |
C5 |
C6 |
104.764 |
| O3 |
C5 |
H7 |
109.397 |
|
O3 |
C5 |
H8 |
109.397 |
| O4 |
C6 |
C5 |
104.764 |
|
O4 |
C6 |
H9 |
109.397 |
| O4 |
C6 |
H10 |
109.397 |
|
C5 |
C6 |
H9 |
112.323 |
| C5 |
C6 |
H10 |
112.323 |
|
C6 |
C5 |
H7 |
112.323 |
| C6 |
C5 |
H8 |
112.323 |
|
H7 |
C5 |
H8 |
108.542 |
| H9 |
C6 |
H10 |
108.542 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.512 |
|
|
|
| 2 |
O |
-0.310 |
|
|
|
| 3 |
O |
-0.291 |
|
|
|
| 4 |
O |
-0.291 |
|
|
|
| 5 |
C |
-0.274 |
|
|
|
| 6 |
C |
-0.274 |
|
|
|
| 7 |
H |
0.232 |
|
|
|
| 8 |
H |
0.232 |
|
|
|
| 9 |
H |
0.232 |
|
|
|
| 10 |
H |
0.232 |
|
|
|
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 |
-4.854 |
4.854 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.809 |
0.000 |
0.000 |
| y |
0.000 |
-36.215 |
0.000 |
| z |
0.000 |
0.000 |
-35.488 |
|
| Traceless |
| | x | y | z |
| x |
4.043 |
0.000 |
0.000 |
| y |
0.000 |
-2.566 |
0.000 |
| z |
0.000 |
0.000 |
-1.477 |
|
| Polar |
| 3z2-r2 | -2.954 |
| x2-y2 | 4.406 |
| 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 |
4.236 |
0.000 |
0.000 |
| y |
0.000 |
5.147 |
0.000 |
| z |
0.000 |
0.000 |
7.268 |
<r2> (average value of r
2) Å
2
| <r2> |
127.264 |
| (<r2>)1/2 |
11.281 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -342.361689 |
| Energy at 298.15K | -342.368112 |
| HF Energy | -342.361689 |
| Nuclear repulsion energy | 247.764939 |
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 B1B95/6-311G*
| 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 |
3145 |
3014 |
23.06 |
|
|
|
| 2 |
A |
3060 |
2934 |
31.16 |
|
|
|
| 3 |
A |
1980 |
1898 |
630.93 |
|
|
|
| 4 |
A |
1554 |
1489 |
2.12 |
|
|
|
| 5 |
A |
1420 |
1361 |
7.53 |
|
|
|
| 6 |
A |
1276 |
1224 |
21.85 |
|
|
|
| 7 |
A |
1235 |
1184 |
182.85 |
|
|
|
| 8 |
A |
1165 |
1117 |
35.32 |
|
|
|
| 9 |
A |
970 |
930 |
3.29 |
|
|
|
| 10 |
A |
850 |
815 |
38.16 |
|
|
|
| 11 |
A |
727 |
697 |
1.30 |
|
|
|
| 12 |
A |
146 |
140 |
0.60 |
|
|
|
| 13 |
B |
3154 |
3024 |
33.57 |
|
|
|
| 14 |
B |
3066 |
2939 |
59.98 |
|
|
|
| 15 |
B |
1545 |
1481 |
6.85 |
|
|
|
| 16 |
B |
1416 |
1358 |
15.53 |
|
|
|
| 17 |
B |
1293 |
1240 |
5.66 |
|
|
|
| 18 |
B |
1198 |
1148 |
3.88 |
|
|
|
| 19 |
B |
1055 |
1011 |
302.55 |
|
|
|
| 20 |
B |
911 |
873 |
11.68 |
|
|
|
| 21 |
B |
784 |
751 |
25.56 |
|
|
|
| 22 |
B |
685 |
657 |
1.04 |
|
|
|
| 23 |
B |
516 |
495 |
0.09 |
|
|
|
| 24 |
B |
147 |
141 |
1.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16649.2 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 15959.9 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 B1B95/6-311G*
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 |
2.031 |
| O3 |
0.000 |
1.123 |
0.046 |
| O4 |
0.000 |
-1.123 |
0.046 |
| C5 |
0.204 |
0.734 |
-1.267 |
| C6 |
-0.204 |
-0.734 |
-1.267 |
| H7 |
-0.404 |
1.350 |
-1.926 |
| H8 |
1.258 |
0.864 |
-1.529 |
| H9 |
0.404 |
-1.350 |
-1.926 |
| H10 |
-1.258 |
-0.864 |
-1.529 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1757 | 1.3840 | 1.3840 | 2.2551 | 2.2551 | 3.1182 | 2.8307 | 3.1182 | 2.8307 |
O2 | 1.1757 | | 2.2807 | 2.2807 | 3.3850 | 3.3850 | 4.2007 | 3.8731 | 4.2007 | 3.8731 | O3 | 1.3840 | 2.2807 | | 2.2450 | 1.3840 | 2.2833 | 2.0256 | 2.0320 | 3.1885 | 2.8297 | O4 | 1.3840 | 2.2807 | 2.2450 | | 2.2833 | 1.3840 | 3.1885 | 2.8297 | 2.0256 | 2.0320 | C5 | 2.2551 | 3.3850 | 1.3840 | 2.2833 | | 1.5247 | 1.0879 | 1.0935 | 2.1957 | 2.1821 | C6 | 2.2551 | 3.3850 | 2.2833 | 1.3840 | 1.5247 | | 2.1957 | 2.1821 | 1.0879 | 1.0935 | H7 | 3.1182 | 4.2007 | 2.0256 | 3.1885 | 1.0879 | 2.1957 | | 1.7765 | 2.8190 | 2.4064 | H8 | 2.8307 | 3.8731 | 2.0320 | 2.8297 | 1.0935 | 2.1821 | 1.7765 | | 2.4064 | 3.0522 | H9 | 3.1182 | 4.2007 | 3.1885 | 2.0256 | 2.1957 | 1.0879 | 2.8190 | 2.4064 | | 1.7765 | H10 | 2.8307 | 3.8731 | 2.8297 | 2.0320 | 2.1821 | 1.0935 | 2.4064 | 3.0522 | 1.7765 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.114 |
|
C1 |
O4 |
C6 |
109.114 |
| O2 |
C1 |
O3 |
125.802 |
|
O2 |
C1 |
O4 |
125.802 |
| O3 |
C1 |
O4 |
108.396 |
|
O3 |
C5 |
C6 |
103.329 |
| O3 |
C5 |
H7 |
109.477 |
|
O3 |
C5 |
H8 |
109.646 |
| O4 |
C6 |
C5 |
103.329 |
|
O4 |
C6 |
H9 |
109.477 |
| O4 |
C6 |
H10 |
109.646 |
|
C5 |
C6 |
H9 |
113.312 |
| C5 |
C6 |
H10 |
111.851 |
|
C6 |
C5 |
H7 |
113.312 |
| C6 |
C5 |
H8 |
111.851 |
|
H7 |
C5 |
H8 |
109.058 |
| H9 |
C6 |
H10 |
109.058 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.514 |
|
|
|
| 2 |
O |
-0.306 |
|
|
|
| 3 |
O |
-0.292 |
|
|
|
| 4 |
O |
-0.292 |
|
|
|
| 5 |
C |
-0.277 |
|
|
|
| 6 |
C |
-0.277 |
|
|
|
| 7 |
H |
0.234 |
|
|
|
| 8 |
H |
0.230 |
|
|
|
| 9 |
H |
0.234 |
|
|
|
| 10 |
H |
0.230 |
|
|
|
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 |
-4.791 |
4.791 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.910 |
0.193 |
0.000 |
| y |
0.193 |
-36.213 |
0.000 |
| z |
0.000 |
0.000 |
-35.273 |
|
| Traceless |
| | x | y | z |
| x |
3.833 |
0.193 |
0.000 |
| y |
0.193 |
-2.621 |
0.000 |
| z |
0.000 |
0.000 |
-1.211 |
|
| Polar |
| 3z2-r2 | -2.423 |
| x2-y2 | 4.303 |
| xy | 0.193 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.347 |
0.160 |
0.000 |
| y |
0.160 |
5.095 |
0.000 |
| z |
0.000 |
0.000 |
7.228 |
<r2> (average value of r
2) Å
2
| <r2> |
126.075 |
| (<r2>)1/2 |
11.228 |