Jump to
S1C2
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -342.178045 |
| Energy at 298.15K | |
| HF Energy | -341.854156 |
| Nuclear repulsion energy | 245.410976 |
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 B2PLYP/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 |
3091 |
3091 |
63.65 |
|
|
|
| 2 |
A1 |
1931 |
1931 |
592.43 |
|
|
|
| 3 |
A1 |
1583 |
1583 |
1.84 |
|
|
|
| 4 |
A1 |
1420 |
1420 |
0.94 |
|
|
|
| 5 |
A1 |
1205 |
1205 |
240.85 |
|
|
|
| 6 |
A1 |
960 |
960 |
11.25 |
|
|
|
| 7 |
A1 |
824 |
824 |
38.04 |
|
|
|
| 8 |
A1 |
724 |
724 |
0.58 |
|
|
|
| 9 |
A2 |
3119 |
3119 |
0.00 |
|
|
|
| 10 |
A2 |
1274 |
1274 |
0.00 |
|
|
|
| 11 |
A2 |
1189 |
1189 |
0.00 |
|
|
|
| 12 |
A2 |
184i |
184i |
0.00 |
|
|
|
| 13 |
B1 |
3142 |
3142 |
56.83 |
|
|
|
| 14 |
B1 |
1291 |
1291 |
1.51 |
|
|
|
| 15 |
B1 |
872 |
872 |
0.77 |
|
|
|
| 16 |
B1 |
759 |
759 |
22.70 |
|
|
|
| 17 |
B1 |
137 |
137 |
2.12 |
|
|
|
| 18 |
B2 |
3083 |
3083 |
31.35 |
|
|
|
| 19 |
B2 |
1570 |
1570 |
3.12 |
|
|
|
| 20 |
B2 |
1429 |
1429 |
12.06 |
|
|
|
| 21 |
B2 |
1195 |
1195 |
1.38 |
|
|
|
| 22 |
B2 |
1031 |
1031 |
327.03 |
|
|
|
| 23 |
B2 |
752 |
752 |
4.27 |
|
|
|
| 24 |
B2 |
509 |
509 |
0.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16452.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16452.3 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 B2PLYP/6-311G*
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 |
2.050 |
| O3 |
0.000 |
1.132 |
0.058 |
| O4 |
0.000 |
-1.132 |
0.058 |
| C5 |
0.000 |
0.775 |
-1.288 |
| C6 |
0.000 |
-0.775 |
-1.288 |
| H7 |
-0.887 |
1.189 |
-1.770 |
| H8 |
0.887 |
1.189 |
-1.770 |
| H9 |
0.887 |
-1.189 |
-1.770 |
| H10 |
-0.887 |
-1.189 |
-1.770 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1823 | 1.3924 | 1.3924 | 2.2910 | 2.2910 | 3.0260 | 3.0260 | 3.0260 | 3.0260 |
O2 | 1.1823 | | 2.2918 | 2.2918 | 3.4270 | 3.4270 | 4.0977 | 4.0977 | 4.0977 | 4.0977 | O3 | 1.3924 | 2.2918 | | 2.2649 | 1.3924 | 2.3344 | 2.0321 | 2.0321 | 3.0845 | 3.0845 | O4 | 1.3924 | 2.2918 | 2.2649 | | 2.3344 | 1.3924 | 3.0845 | 3.0845 | 2.0321 | 2.0321 | C5 | 2.2910 | 3.4270 | 1.3924 | 2.3344 | | 1.5500 | 1.0910 | 1.0910 | 2.2080 | 2.2080 | C6 | 2.2910 | 3.4270 | 2.3344 | 1.3924 | 1.5500 | | 2.2080 | 2.2080 | 1.0910 | 1.0910 | H7 | 3.0260 | 4.0977 | 2.0321 | 3.0845 | 1.0910 | 2.2080 | | 1.7744 | 2.9667 | 2.3775 | H8 | 3.0260 | 4.0977 | 2.0321 | 3.0845 | 1.0910 | 2.2080 | 1.7744 | | 2.3775 | 2.9667 | H9 | 3.0260 | 4.0977 | 3.0845 | 2.0321 | 2.2080 | 1.0910 | 2.9667 | 2.3775 | | 1.7744 | H10 | 3.0260 | 4.0977 | 3.0845 | 2.0321 | 2.2080 | 1.0910 | 2.3775 | 2.9667 | 1.7744 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.705 |
|
C1 |
O4 |
C6 |
110.705 |
| O2 |
C1 |
O3 |
125.581 |
|
O2 |
C1 |
O4 |
125.581 |
| O3 |
C1 |
O4 |
108.839 |
|
O3 |
C5 |
C6 |
104.876 |
| O3 |
C5 |
H7 |
109.224 |
|
O3 |
C5 |
H8 |
109.224 |
| O4 |
C6 |
C5 |
104.876 |
|
O4 |
C6 |
H9 |
109.224 |
| O4 |
C6 |
H10 |
109.224 |
|
C5 |
C6 |
H9 |
112.286 |
| C5 |
C6 |
H10 |
112.286 |
|
C6 |
C5 |
H7 |
112.286 |
| C6 |
C5 |
H8 |
112.286 |
|
H7 |
C5 |
H8 |
108.825 |
| H9 |
C6 |
H10 |
108.825 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.498 |
|
|
|
| 2 |
O |
-0.297 |
|
|
|
| 3 |
O |
-0.299 |
|
|
|
| 4 |
O |
-0.299 |
|
|
|
| 5 |
C |
-0.253 |
|
|
|
| 6 |
C |
-0.253 |
|
|
|
| 7 |
H |
0.226 |
|
|
|
| 8 |
H |
0.226 |
|
|
|
| 9 |
H |
0.226 |
|
|
|
| 10 |
H |
0.226 |
|
|
|
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 |
-4.855 |
4.855 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.175 |
0.000 |
0.000 |
| y |
0.000 |
-36.737 |
0.000 |
| z |
0.000 |
0.000 |
-35.697 |
|
| Traceless |
| | x | y | z |
| x |
4.043 |
0.000 |
0.000 |
| y |
0.000 |
-2.802 |
0.000 |
| z |
0.000 |
0.000 |
-1.241 |
|
| Polar |
| 3z2-r2 | -2.483 |
| x2-y2 | 4.563 |
| 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 |
4.237 |
0.000 |
0.000 |
| y |
0.000 |
5.193 |
0.000 |
| z |
0.000 |
0.000 |
7.390 |
<r2> (average value of r
2) Å
2
| <r2> |
128.940 |
| (<r2>)1/2 |
11.355 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -342.179052 |
| Energy at 298.15K | -342.185459 |
| HF Energy | -341.854617 |
| Nuclear repulsion energy | 246.061181 |
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 B2PLYP/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 |
3146 |
3146 |
21.00 |
|
|
|
| 2 |
A |
3067 |
3067 |
32.64 |
|
|
|
| 3 |
A |
1933 |
1933 |
574.66 |
|
|
|
| 4 |
A |
1568 |
1568 |
2.17 |
|
|
|
| 5 |
A |
1425 |
1425 |
6.62 |
|
|
|
| 6 |
A |
1278 |
1278 |
15.79 |
|
|
|
| 7 |
A |
1211 |
1211 |
113.38 |
|
|
|
| 8 |
A |
1165 |
1165 |
101.73 |
|
|
|
| 9 |
A |
963 |
963 |
4.83 |
|
|
|
| 10 |
A |
820 |
820 |
41.82 |
|
|
|
| 11 |
A |
721 |
721 |
0.83 |
|
|
|
| 12 |
A |
154 |
154 |
0.70 |
|
|
|
| 13 |
B |
3157 |
3157 |
34.84 |
|
|
|
| 14 |
B |
3071 |
3071 |
57.16 |
|
|
|
| 15 |
B |
1560 |
1560 |
4.68 |
|
|
|
| 16 |
B |
1421 |
1421 |
10.28 |
|
|
|
| 17 |
B |
1292 |
1292 |
4.93 |
|
|
|
| 18 |
B |
1173 |
1173 |
3.97 |
|
|
|
| 19 |
B |
1029 |
1029 |
282.94 |
|
|
|
| 20 |
B |
907 |
907 |
25.80 |
|
|
|
| 21 |
B |
770 |
770 |
23.94 |
|
|
|
| 22 |
B |
685 |
685 |
1.91 |
|
|
|
| 23 |
B |
509 |
509 |
0.24 |
|
|
|
| 24 |
B |
149 |
149 |
1.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16587.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16587.2 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 B2PLYP/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.862 |
| O2 |
0.000 |
0.000 |
2.045 |
| O3 |
0.000 |
1.132 |
0.046 |
| O4 |
0.000 |
-1.132 |
0.046 |
| C5 |
0.207 |
0.738 |
-1.277 |
| C6 |
-0.207 |
-0.738 |
-1.277 |
| H7 |
-0.400 |
1.357 |
-1.935 |
| H8 |
1.263 |
0.863 |
-1.535 |
| H9 |
0.400 |
-1.357 |
-1.935 |
| H10 |
-1.263 |
-0.863 |
-1.535 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1821 | 1.3959 | 1.3959 | 2.2728 | 2.2728 | 3.1351 | 2.8442 | 3.1351 | 2.8442 |
O2 | 1.1821 | | 2.2971 | 2.2971 | 3.4090 | 3.4090 | 4.2239 | 3.8930 | 4.2239 | 3.8930 | O3 | 1.3959 | 2.2971 | | 2.2645 | 1.3959 | 2.3005 | 2.0338 | 2.0416 | 3.2066 | 2.8421 | O4 | 1.3959 | 2.2971 | 2.2645 | | 2.3005 | 1.3959 | 3.2066 | 2.8421 | 2.0338 | 2.0416 | C5 | 2.2728 | 3.4090 | 1.3959 | 2.3005 | | 1.5337 | 1.0888 | 1.0940 | 2.2046 | 2.1894 | C6 | 2.2728 | 3.4090 | 2.3005 | 1.3959 | 1.5337 | | 2.2046 | 2.1894 | 1.0888 | 1.0940 | H7 | 3.1351 | 4.2239 | 2.0338 | 3.2066 | 1.0888 | 2.2046 | | 1.7807 | 2.8294 | 2.4152 | H8 | 2.8442 | 3.8930 | 2.0416 | 2.8421 | 1.0940 | 2.1894 | 1.7807 | | 2.4152 | 3.0598 | H9 | 3.1351 | 4.2239 | 3.2066 | 2.0338 | 2.2046 | 1.0888 | 2.8294 | 2.4152 | | 1.7807 | H10 | 2.8442 | 3.8930 | 2.8421 | 2.0416 | 2.1894 | 1.0940 | 2.4152 | 3.0598 | 1.7807 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.990 |
|
C1 |
O4 |
C6 |
108.990 |
| O2 |
C1 |
O3 |
125.795 |
|
O2 |
C1 |
O4 |
125.795 |
| O3 |
C1 |
O4 |
108.410 |
|
O3 |
C5 |
C6 |
103.388 |
| O3 |
C5 |
H7 |
109.253 |
|
O3 |
C5 |
H8 |
109.563 |
| O4 |
C6 |
C5 |
103.388 |
|
O4 |
C6 |
H9 |
109.253 |
| O4 |
C6 |
H10 |
109.563 |
|
C5 |
C6 |
H9 |
113.334 |
| C5 |
C6 |
H10 |
111.771 |
|
C6 |
C5 |
H7 |
113.334 |
| C6 |
C5 |
H8 |
111.771 |
|
H7 |
C5 |
H8 |
109.334 |
| H9 |
C6 |
H10 |
109.334 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.500 |
|
|
|
| 2 |
O |
-0.293 |
|
|
|
| 3 |
O |
-0.301 |
|
|
|
| 4 |
O |
-0.301 |
|
|
|
| 5 |
C |
-0.254 |
|
|
|
| 6 |
C |
-0.254 |
|
|
|
| 7 |
H |
0.228 |
|
|
|
| 8 |
H |
0.222 |
|
|
|
| 9 |
H |
0.228 |
|
|
|
| 10 |
H |
0.222 |
|
|
|
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 |
-4.787 |
4.787 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.281 |
0.194 |
0.000 |
| y |
0.194 |
-36.737 |
0.000 |
| z |
0.000 |
0.000 |
-35.493 |
|
| Traceless |
| | x | y | z |
| x |
3.835 |
0.194 |
0.000 |
| y |
0.194 |
-2.851 |
0.000 |
| z |
0.000 |
0.000 |
-0.984 |
|
| Polar |
| 3z2-r2 | -1.968 |
| x2-y2 | 4.457 |
| xy | 0.194 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.346 |
0.156 |
0.000 |
| y |
0.156 |
5.142 |
0.000 |
| z |
0.000 |
0.000 |
7.351 |
<r2> (average value of r
2) Å
2
| <r2> |
127.726 |
| (<r2>)1/2 |
11.302 |