Jump to
S1C2
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -342.424087 |
| Energy at 298.15K | |
| HF Energy | -342.424087 |
| Nuclear repulsion energy | 245.502677 |
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 B3LYP/6-31G(2df,p)
| 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 |
3046 |
2939 |
59.11 |
|
|
|
| 2 |
A1 |
1951 |
1882 |
562.63 |
|
|
|
| 3 |
A1 |
1549 |
1495 |
3.29 |
|
|
|
| 4 |
A1 |
1395 |
1346 |
0.36 |
|
|
|
| 5 |
A1 |
1196 |
1155 |
226.51 |
|
|
|
| 6 |
A1 |
946 |
913 |
7.98 |
|
|
|
| 7 |
A1 |
836 |
807 |
31.00 |
|
|
|
| 8 |
A1 |
727 |
701 |
1.00 |
|
|
|
| 9 |
A2 |
3068 |
2961 |
0.00 |
|
|
|
| 10 |
A2 |
1251 |
1207 |
0.00 |
|
|
|
| 11 |
A2 |
1172 |
1131 |
0.00 |
|
|
|
| 12 |
A2 |
153i |
148i |
0.00 |
|
|
|
| 13 |
B1 |
3092 |
2983 |
47.75 |
|
|
|
| 14 |
B1 |
1266 |
1222 |
1.52 |
|
|
|
| 15 |
B1 |
858 |
828 |
0.82 |
|
|
|
| 16 |
B1 |
767 |
740 |
21.74 |
|
|
|
| 17 |
B1 |
146 |
141 |
1.21 |
|
|
|
| 18 |
B2 |
3039 |
2933 |
29.06 |
|
|
|
| 19 |
B2 |
1538 |
1484 |
2.65 |
|
|
|
| 20 |
B2 |
1414 |
1364 |
17.10 |
|
|
|
| 21 |
B2 |
1186 |
1145 |
2.20 |
|
|
|
| 22 |
B2 |
1039 |
1002 |
275.97 |
|
|
|
| 23 |
B2 |
753 |
727 |
2.27 |
|
|
|
| 24 |
B2 |
506 |
488 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16292.8 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 15722.5 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 B3LYP/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.867 |
| O2 |
0.000 |
0.000 |
2.049 |
| O3 |
0.000 |
1.131 |
0.059 |
| O4 |
0.000 |
-1.131 |
0.059 |
| C5 |
0.000 |
0.777 |
-1.286 |
| C6 |
0.000 |
-0.777 |
-1.286 |
| H7 |
-0.888 |
1.190 |
-1.775 |
| H8 |
0.888 |
1.190 |
-1.775 |
| H9 |
0.888 |
-1.190 |
-1.775 |
| H10 |
-0.888 |
-1.190 |
-1.775 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1818 | 1.3900 | 1.3900 | 2.2888 | 2.2888 | 3.0310 | 3.0310 | 3.0310 | 3.0310 |
O2 | 1.1818 | | 2.2890 | 2.2890 | 3.4240 | 3.4240 | 4.1023 | 4.1023 | 4.1023 | 4.1023 | O3 | 1.3900 | 2.2890 | | 2.2613 | 1.3900 | 2.3340 | 2.0383 | 2.0383 | 3.0885 | 3.0885 | O4 | 1.3900 | 2.2890 | 2.2613 | | 2.3340 | 1.3900 | 3.0885 | 3.0885 | 2.0383 | 2.0383 | C5 | 2.2888 | 3.4240 | 1.3900 | 2.3340 | | 1.5546 | 1.0949 | 1.0949 | 2.2136 | 2.2136 | C6 | 2.2888 | 3.4240 | 2.3340 | 1.3900 | 1.5546 | | 2.2136 | 2.2136 | 1.0949 | 1.0949 | H7 | 3.0310 | 4.1023 | 2.0383 | 3.0885 | 1.0949 | 2.2136 | | 1.7760 | 2.9704 | 2.3810 | H8 | 3.0310 | 4.1023 | 2.0383 | 3.0885 | 1.0949 | 2.2136 | 1.7760 | | 2.3810 | 2.9704 | H9 | 3.0310 | 4.1023 | 3.0885 | 2.0383 | 2.2136 | 1.0949 | 2.9704 | 2.3810 | | 1.7760 | H10 | 3.0310 | 4.1023 | 3.0885 | 2.0383 | 2.2136 | 1.0949 | 2.3810 | 2.9704 | 1.7760 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.840 |
|
C1 |
O4 |
C6 |
110.840 |
| O2 |
C1 |
O3 |
125.567 |
|
O2 |
C1 |
O4 |
125.567 |
| O3 |
C1 |
O4 |
108.865 |
|
O3 |
C5 |
C6 |
104.728 |
| O3 |
C5 |
H7 |
109.655 |
|
O3 |
C5 |
H8 |
109.655 |
| O4 |
C6 |
C5 |
104.728 |
|
O4 |
C6 |
H9 |
109.655 |
| O4 |
C6 |
H10 |
109.655 |
|
C5 |
C6 |
H9 |
112.173 |
| C5 |
C6 |
H10 |
112.173 |
|
C6 |
C5 |
H7 |
112.173 |
| C6 |
C5 |
H8 |
112.173 |
|
H7 |
C5 |
H8 |
108.394 |
| H9 |
C6 |
H10 |
108.394 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.523 |
|
|
|
| 2 |
O |
-0.348 |
|
|
|
| 3 |
O |
-0.235 |
|
|
|
| 4 |
O |
-0.235 |
|
|
|
| 5 |
C |
-0.107 |
|
|
|
| 6 |
C |
-0.107 |
|
|
|
| 7 |
H |
0.127 |
|
|
|
| 8 |
H |
0.127 |
|
|
|
| 9 |
H |
0.127 |
|
|
|
| 10 |
H |
0.127 |
|
|
|
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 |
-4.570 |
4.570 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.708 |
0.000 |
0.000 |
| y |
0.000 |
-35.512 |
0.000 |
| z |
0.000 |
0.000 |
-35.535 |
|
| Traceless |
| | x | y | z |
| x |
3.816 |
0.000 |
0.000 |
| y |
0.000 |
-1.890 |
0.000 |
| z |
0.000 |
0.000 |
-1.925 |
|
| Polar |
| 3z2-r2 | -3.851 |
| x2-y2 | 3.804 |
| 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 |
4.509 |
0.000 |
0.000 |
| y |
0.000 |
5.404 |
0.000 |
| z |
0.000 |
0.000 |
7.489 |
<r2> (average value of r
2) Å
2
| <r2> |
128.511 |
| (<r2>)1/2 |
11.336 |
Jump to
S1C1
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -342.424373 |
| Energy at 298.15K | -342.430661 |
| HF Energy | -342.424373 |
| Nuclear repulsion energy | 245.855322 |
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 B3LYP/6-31G(2df,p)
| 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 |
3092 |
2984 |
19.31 |
|
|
|
| 2 |
A |
3026 |
2920 |
33.97 |
|
|
|
| 3 |
A |
1953 |
1885 |
553.19 |
|
|
|
| 4 |
A |
1540 |
1486 |
3.62 |
|
|
|
| 5 |
A |
1398 |
1349 |
2.64 |
|
|
|
| 6 |
A |
1254 |
1210 |
15.84 |
|
|
|
| 7 |
A |
1199 |
1157 |
141.61 |
|
|
|
| 8 |
A |
1157 |
1116 |
64.11 |
|
|
|
| 9 |
A |
947 |
914 |
4.42 |
|
|
|
| 10 |
A |
834 |
804 |
33.53 |
|
|
|
| 11 |
A |
725 |
700 |
1.17 |
|
|
|
| 12 |
A |
82 |
79 |
0.23 |
|
|
|
| 13 |
B |
3104 |
2996 |
32.72 |
|
|
|
| 14 |
B |
3030 |
2924 |
46.08 |
|
|
|
| 15 |
B |
1532 |
1479 |
3.30 |
|
|
|
| 16 |
B |
1409 |
1360 |
15.32 |
|
|
|
| 17 |
B |
1268 |
1223 |
3.27 |
|
|
|
| 18 |
B |
1171 |
1130 |
2.81 |
|
|
|
| 19 |
B |
1035 |
998 |
261.91 |
|
|
|
| 20 |
B |
887 |
855 |
7.14 |
|
|
|
| 21 |
B |
771 |
744 |
22.10 |
|
|
|
| 22 |
B |
706 |
681 |
1.20 |
|
|
|
| 23 |
B |
506 |
488 |
0.03 |
|
|
|
| 24 |
B |
151 |
146 |
1.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16387.2 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 15813.7 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 B3LYP/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.864 |
| O2 |
0.000 |
0.000 |
2.046 |
| O3 |
0.000 |
1.131 |
0.052 |
| O4 |
0.000 |
-1.131 |
0.052 |
| C5 |
0.158 |
0.756 |
-1.280 |
| C6 |
-0.158 |
-0.756 |
-1.280 |
| H7 |
-0.528 |
1.331 |
-1.907 |
| H8 |
1.186 |
0.960 |
-1.604 |
| H9 |
0.528 |
-1.331 |
-1.907 |
| H10 |
-1.186 |
-0.960 |
-1.604 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1815 | 1.3922 | 1.3922 | 2.2787 | 2.2787 | 3.1192 | 2.9019 | 3.1192 | 2.9019 |
O2 | 1.1815 | | 2.2921 | 2.2921 | 3.4139 | 3.4139 | 4.2040 | 3.9561 | 4.2040 | 3.9561 | O3 | 1.3922 | 2.2921 | | 2.2615 | 1.3922 | 2.3149 | 2.0388 | 2.0441 | 3.1899 | 2.9190 | O4 | 1.3922 | 2.2921 | 2.2615 | | 2.3149 | 1.3922 | 3.1899 | 2.9190 | 2.0388 | 2.0441 | C5 | 2.2787 | 3.4139 | 1.3922 | 2.3149 | | 1.5450 | 1.0928 | 1.0972 | 2.2106 | 2.2035 | C6 | 2.2787 | 3.4139 | 2.3149 | 1.3922 | 1.5450 | | 2.2106 | 2.2035 | 1.0928 | 1.0972 | H7 | 3.1192 | 4.2040 | 2.0388 | 3.1899 | 1.0928 | 2.2106 | | 1.7796 | 2.8636 | 2.4023 | H8 | 2.9019 | 3.9561 | 2.0441 | 2.9190 | 1.0972 | 2.2035 | 1.7796 | | 2.4023 | 3.0512 | H9 | 3.1192 | 4.2040 | 3.1899 | 2.0388 | 2.2106 | 1.0928 | 2.8636 | 2.4023 | | 1.7796 | H10 | 2.9019 | 3.9561 | 2.9190 | 2.0441 | 2.2035 | 1.0972 | 2.4023 | 3.0512 | 1.7796 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
109.848 |
|
C1 |
O4 |
C6 |
109.848 |
| O2 |
C1 |
O3 |
125.689 |
|
O2 |
C1 |
O4 |
125.689 |
| O3 |
C1 |
O4 |
108.623 |
|
O3 |
C5 |
C6 |
103.901 |
| O3 |
C5 |
H7 |
109.674 |
|
O3 |
C5 |
H8 |
109.825 |
| O4 |
C6 |
C5 |
103.901 |
|
O4 |
C6 |
H9 |
109.674 |
| O4 |
C6 |
H10 |
109.825 |
|
C5 |
C6 |
H9 |
112.742 |
| C5 |
C6 |
H10 |
111.897 |
|
C6 |
C5 |
H7 |
112.742 |
| C6 |
C5 |
H8 |
111.897 |
|
H7 |
C5 |
H8 |
108.702 |
| H9 |
C6 |
H10 |
108.702 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.521 |
|
|
|
| 2 |
O |
-0.348 |
|
|
|
| 3 |
O |
-0.235 |
|
|
|
| 4 |
O |
-0.235 |
|
|
|
| 5 |
C |
-0.104 |
|
|
|
| 6 |
C |
-0.104 |
|
|
|
| 7 |
H |
0.131 |
|
|
|
| 8 |
H |
0.123 |
|
|
|
| 9 |
H |
0.131 |
|
|
|
| 10 |
H |
0.123 |
|
|
|
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 |
-4.542 |
4.542 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.762 |
0.140 |
0.000 |
| y |
0.140 |
-35.520 |
0.000 |
| z |
0.000 |
0.000 |
-35.410 |
|
| Traceless |
| | x | y | z |
| x |
3.703 |
0.140 |
0.000 |
| y |
0.140 |
-1.934 |
0.000 |
| z |
0.000 |
0.000 |
-1.769 |
|
| Polar |
| 3z2-r2 | -3.538 |
| x2-y2 | 3.758 |
| xy | 0.140 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.562 |
0.128 |
0.000 |
| y |
0.128 |
5.364 |
0.000 |
| z |
0.000 |
0.000 |
7.471 |
<r2> (average value of r
2) Å
2
| <r2> |
127.827 |
| (<r2>)1/2 |
11.306 |