Jump to
S1C2
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -338.619700 |
| Energy at 298.15K | |
| HF Energy | -338.619700 |
| Nuclear repulsion energy | 244.162514 |
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/3-21G*
| 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 |
3273 |
2954 |
31.56 |
|
|
|
| 2 |
A1 |
2085 |
1882 |
664.57 |
|
|
|
| 3 |
A1 |
1708 |
1541 |
3.62 |
|
|
|
| 4 |
A1 |
1499 |
1353 |
0.13 |
|
|
|
| 5 |
A1 |
1268 |
1145 |
268.36 |
|
|
|
| 6 |
A1 |
946 |
854 |
9.82 |
|
|
|
| 7 |
A1 |
854 |
771 |
31.41 |
|
|
|
| 8 |
A1 |
764 |
690 |
2.17 |
|
|
|
| 9 |
A2 |
3302 |
2981 |
0.00 |
|
|
|
| 10 |
A2 |
1381 |
1246 |
0.00 |
|
|
|
| 11 |
A2 |
1248 |
1127 |
0.00 |
|
|
|
| 12 |
A2 |
176i |
158i |
0.00 |
|
|
|
| 13 |
B1 |
3326 |
3002 |
40.71 |
|
|
|
| 14 |
B1 |
1368 |
1234 |
1.48 |
|
|
|
| 15 |
B1 |
929 |
838 |
3.75 |
|
|
|
| 16 |
B1 |
818 |
739 |
64.90 |
|
|
|
| 17 |
B1 |
111 |
100 |
5.21 |
|
|
|
| 18 |
B2 |
3262 |
2944 |
27.42 |
|
|
|
| 19 |
B2 |
1693 |
1528 |
1.52 |
|
|
|
| 20 |
B2 |
1539 |
1389 |
1.94 |
|
|
|
| 21 |
B2 |
1262 |
1139 |
3.88 |
|
|
|
| 22 |
B2 |
1062 |
959 |
349.81 |
|
|
|
| 23 |
B2 |
804 |
725 |
0.01 |
|
|
|
| 24 |
B2 |
532 |
480 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17428.2 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 15730.7 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 HF/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.890 |
| O2 |
0.000 |
0.000 |
2.066 |
| O3 |
0.000 |
1.130 |
0.056 |
| O4 |
0.000 |
-1.130 |
0.056 |
| C5 |
0.000 |
0.785 |
-1.305 |
| C6 |
0.000 |
-0.785 |
-1.305 |
| H7 |
-0.882 |
1.185 |
-1.778 |
| H8 |
0.882 |
1.185 |
-1.778 |
| H9 |
0.882 |
-1.185 |
-1.778 |
| H10 |
-0.882 |
-1.185 |
-1.778 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1758 | 1.4041 | 1.4041 | 2.3307 | 2.3307 | 3.0492 | 3.0492 | 3.0492 | 3.0492 |
O2 | 1.1758 | | 2.3053 | 2.3053 | 3.4606 | 3.4606 | 4.1175 | 4.1175 | 4.1175 | 4.1175 | O3 | 1.4041 | 2.3053 | | 2.2596 | 1.4041 | 2.3489 | 2.0357 | 2.0357 | 3.0819 | 3.0819 | O4 | 1.4041 | 2.3053 | 2.2596 | | 2.3489 | 1.4041 | 3.0819 | 3.0819 | 2.0357 | 2.0357 | C5 | 2.3307 | 3.4606 | 1.4041 | 2.3489 | | 1.5691 | 1.0775 | 1.0775 | 2.2089 | 2.2089 | C6 | 2.3307 | 3.4606 | 2.3489 | 1.4041 | 1.5691 | | 2.2089 | 2.2089 | 1.0775 | 1.0775 | H7 | 3.0492 | 4.1175 | 2.0357 | 3.0819 | 1.0775 | 2.2089 | | 1.7631 | 2.9535 | 2.3695 | H8 | 3.0492 | 4.1175 | 2.0357 | 3.0819 | 1.0775 | 2.2089 | 1.7631 | | 2.3695 | 2.9535 | H9 | 3.0492 | 4.1175 | 3.0819 | 2.0357 | 2.2089 | 1.0775 | 2.9535 | 2.3695 | | 1.7631 | H10 | 3.0492 | 4.1175 | 3.0819 | 2.0357 | 2.2089 | 1.0775 | 2.3695 | 2.9535 | 1.7631 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
112.188 |
|
C1 |
O4 |
C6 |
112.188 |
| O2 |
C1 |
O3 |
126.423 |
|
O2 |
C1 |
O4 |
126.423 |
| O3 |
C1 |
O4 |
107.155 |
|
O3 |
C5 |
C6 |
104.234 |
| O3 |
C5 |
H7 |
109.526 |
|
O3 |
C5 |
H8 |
109.526 |
| O4 |
C6 |
C5 |
104.234 |
|
O4 |
C6 |
H9 |
109.526 |
| O4 |
C6 |
H10 |
109.526 |
|
C5 |
C6 |
H9 |
111.802 |
| C5 |
C6 |
H10 |
111.802 |
|
C6 |
C5 |
H7 |
111.802 |
| C6 |
C5 |
H8 |
111.802 |
|
H7 |
C5 |
H8 |
109.792 |
| H9 |
C6 |
H10 |
109.792 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.174 |
|
|
|
| 2 |
O |
-0.574 |
|
|
|
| 3 |
O |
-0.675 |
|
|
|
| 4 |
O |
-0.675 |
|
|
|
| 5 |
C |
-0.116 |
|
|
|
| 6 |
C |
-0.116 |
|
|
|
| 7 |
H |
0.245 |
|
|
|
| 8 |
H |
0.245 |
|
|
|
| 9 |
H |
0.245 |
|
|
|
| 10 |
H |
0.245 |
|
|
|
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 |
-5.594 |
5.594 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.071 |
0.000 |
0.000 |
| y |
0.000 |
-38.345 |
0.000 |
| z |
0.000 |
0.000 |
-35.729 |
|
| Traceless |
| | x | y | z |
| x |
4.966 |
0.000 |
0.000 |
| y |
0.000 |
-4.444 |
0.000 |
| z |
0.000 |
0.000 |
-0.521 |
|
| Polar |
| 3z2-r2 | -1.042 |
| x2-y2 | 6.273 |
| 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 |
3.404 |
0.000 |
0.000 |
| y |
0.000 |
4.129 |
0.000 |
| z |
0.000 |
0.000 |
6.274 |
<r2> (average value of r
2) Å
2
| <r2> |
130.642 |
| (<r2>)1/2 |
11.430 |
Jump to
S1C1
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -338.620098 |
| Energy at 298.15K | -338.626422 |
| HF Energy | -338.620098 |
| Nuclear repulsion energy | 244.576549 |
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/3-21G*
| 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 |
3321 |
2998 |
8.61 |
|
|
|
| 2 |
A |
3258 |
2940 |
18.39 |
|
|
|
| 3 |
A |
2089 |
1886 |
647.56 |
|
|
|
| 4 |
A |
1700 |
1534 |
3.83 |
|
|
|
| 5 |
A |
1508 |
1362 |
3.76 |
|
|
|
| 6 |
A |
1376 |
1242 |
17.39 |
|
|
|
| 7 |
A |
1274 |
1150 |
121.04 |
|
|
|
| 8 |
A |
1237 |
1116 |
120.07 |
|
|
|
| 9 |
A |
953 |
860 |
4.97 |
|
|
|
| 10 |
A |
852 |
769 |
33.33 |
|
|
|
| 11 |
A |
762 |
688 |
2.55 |
|
|
|
| 12 |
A |
51 |
46 |
0.57 |
|
|
|
| 13 |
B |
3335 |
3010 |
29.37 |
|
|
|
| 14 |
B |
3257 |
2940 |
38.89 |
|
|
|
| 15 |
B |
1689 |
1525 |
2.13 |
|
|
|
| 16 |
B |
1538 |
1388 |
1.64 |
|
|
|
| 17 |
B |
1370 |
1236 |
3.24 |
|
|
|
| 18 |
B |
1246 |
1125 |
5.62 |
|
|
|
| 19 |
B |
1065 |
961 |
324.04 |
|
|
|
| 20 |
B |
969 |
874 |
17.65 |
|
|
|
| 21 |
B |
824 |
744 |
66.42 |
|
|
|
| 22 |
B |
745 |
672 |
1.41 |
|
|
|
| 23 |
B |
532 |
480 |
0.00 |
|
|
|
| 24 |
B |
123 |
111 |
5.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17535.4 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 15827.4 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 HF/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.886 |
| O2 |
0.000 |
0.000 |
2.062 |
| O3 |
0.000 |
1.130 |
0.048 |
| O4 |
0.000 |
-1.130 |
0.048 |
| C5 |
0.176 |
0.759 |
-1.297 |
| C6 |
-0.176 |
-0.759 |
-1.297 |
| H7 |
-0.485 |
1.337 |
-1.918 |
| H8 |
1.201 |
0.924 |
-1.591 |
| H9 |
0.485 |
-1.337 |
-1.918 |
| H10 |
-1.201 |
-0.924 |
-1.591 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1756 | 1.4070 | 1.4070 | 2.3183 | 2.3183 | 3.1450 | 2.9038 | 3.1450 | 2.9038 |
O2 | 1.1756 | | 2.3091 | 2.3091 | 3.4483 | 3.4483 | 4.2270 | 3.9545 | 4.2270 | 3.9545 | O3 | 1.4070 | 2.3091 | | 2.2602 | 1.4070 | 2.3256 | 2.0362 | 2.0424 | 3.1925 | 2.8895 | O4 | 1.4070 | 2.3091 | 2.2602 | | 2.3256 | 1.4070 | 3.1925 | 2.8895 | 2.0362 | 2.0424 | C5 | 2.3183 | 3.4483 | 1.4070 | 2.3256 | | 1.5573 | 1.0758 | 1.0795 | 2.2078 | 2.1941 | C6 | 2.3183 | 3.4483 | 2.3256 | 1.4070 | 1.5573 | | 2.2078 | 2.1941 | 1.0758 | 1.0795 | H7 | 3.1450 | 4.2270 | 2.0362 | 3.1925 | 1.0758 | 2.2078 | | 1.7668 | 2.8451 | 2.3950 | H8 | 2.9038 | 3.9545 | 2.0424 | 2.8895 | 1.0795 | 2.1941 | 1.7668 | | 2.3950 | 3.0314 | H9 | 3.1450 | 4.2270 | 3.1925 | 2.0362 | 2.2078 | 1.0758 | 2.8451 | 2.3950 | | 1.7668 | H10 | 2.9038 | 3.9545 | 2.8895 | 2.0424 | 2.1941 | 1.0795 | 2.3950 | 3.0314 | 1.7668 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.950 |
|
C1 |
O4 |
C6 |
110.950 |
| O2 |
C1 |
O3 |
126.560 |
|
O2 |
C1 |
O4 |
126.560 |
| O3 |
C1 |
O4 |
106.879 |
|
O3 |
C5 |
C6 |
103.243 |
| O3 |
C5 |
H7 |
109.476 |
|
O3 |
C5 |
H8 |
109.752 |
| O4 |
C6 |
C5 |
103.243 |
|
O4 |
C6 |
H9 |
109.476 |
| O4 |
C6 |
H10 |
109.752 |
|
C5 |
C6 |
H9 |
112.681 |
| C5 |
C6 |
H10 |
111.342 |
|
C6 |
C5 |
H7 |
112.681 |
| C6 |
C5 |
H8 |
111.342 |
|
H7 |
C5 |
H8 |
110.119 |
| H9 |
C6 |
H10 |
110.119 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.171 |
|
|
|
| 2 |
O |
-0.573 |
|
|
|
| 3 |
O |
-0.672 |
|
|
|
| 4 |
O |
-0.672 |
|
|
|
| 5 |
C |
-0.117 |
|
|
|
| 6 |
C |
-0.117 |
|
|
|
| 7 |
H |
0.249 |
|
|
|
| 8 |
H |
0.242 |
|
|
|
| 9 |
H |
0.249 |
|
|
|
| 10 |
H |
0.242 |
|
|
|
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 |
-5.543 |
5.543 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.097 |
0.282 |
0.000 |
| y |
0.282 |
-38.380 |
0.000 |
| z |
0.000 |
0.000 |
-35.593 |
|
| Traceless |
| | x | y | z |
| x |
4.890 |
0.282 |
0.000 |
| y |
0.282 |
-4.535 |
0.000 |
| z |
0.000 |
0.000 |
-0.355 |
|
| Polar |
| 3z2-r2 | -0.709 |
| x2-y2 | 6.283 |
| xy | 0.282 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.455 |
0.094 |
0.000 |
| y |
0.094 |
4.082 |
0.000 |
| z |
0.000 |
0.000 |
6.269 |
<r2> (average value of r
2) Å
2
| <r2> |
129.815 |
| (<r2>)1/2 |
11.394 |