Jump to
S1C2
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -342.190721 |
| Energy at 298.15K | |
| HF Energy | -341.859573 |
| Nuclear repulsion energy | 245.377583 |
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 |
3082 |
3082 |
59.08 |
|
|
|
| 2 |
A1 |
1931 |
1931 |
591.93 |
|
|
|
| 3 |
A1 |
1567 |
1567 |
1.99 |
|
|
|
| 4 |
A1 |
1408 |
1408 |
0.65 |
|
|
|
| 5 |
A1 |
1204 |
1204 |
237.40 |
|
|
|
| 6 |
A1 |
956 |
956 |
11.54 |
|
|
|
| 7 |
A1 |
824 |
824 |
38.52 |
|
|
|
| 8 |
A1 |
723 |
723 |
0.56 |
|
|
|
| 9 |
A2 |
3110 |
3110 |
0.00 |
|
|
|
| 10 |
A2 |
1262 |
1262 |
0.00 |
|
|
|
| 11 |
A2 |
1179 |
1179 |
0.00 |
|
|
|
| 12 |
A2 |
186i |
186i |
0.00 |
|
|
|
| 13 |
B1 |
3133 |
3133 |
50.04 |
|
|
|
| 14 |
B1 |
1281 |
1281 |
1.75 |
|
|
|
| 15 |
B1 |
865 |
865 |
0.77 |
|
|
|
| 16 |
B1 |
759 |
759 |
22.74 |
|
|
|
| 17 |
B1 |
137 |
137 |
2.03 |
|
|
|
| 18 |
B2 |
3074 |
3074 |
28.36 |
|
|
|
| 19 |
B2 |
1554 |
1554 |
3.55 |
|
|
|
| 20 |
B2 |
1420 |
1420 |
13.53 |
|
|
|
| 21 |
B2 |
1194 |
1194 |
1.30 |
|
|
|
| 22 |
B2 |
1029 |
1029 |
321.47 |
|
|
|
| 23 |
B2 |
751 |
751 |
4.23 |
|
|
|
| 24 |
B2 |
509 |
509 |
0.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16381.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16381.8 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 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 |
1.133 |
0.058 |
| O4 |
0.000 |
-1.133 |
0.058 |
| C5 |
0.000 |
0.775 |
-1.288 |
| C6 |
0.000 |
-0.775 |
-1.288 |
| H7 |
-0.888 |
1.186 |
-1.771 |
| H8 |
0.888 |
1.186 |
-1.771 |
| H9 |
0.888 |
-1.186 |
-1.771 |
| H10 |
-0.888 |
-1.186 |
-1.771 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1822 | 1.3926 | 1.3926 | 2.2914 | 2.2914 | 3.0268 | 3.0268 | 3.0268 | 3.0268 |
O2 | 1.1822 | | 2.2919 | 2.2919 | 3.4273 | 3.4273 | 4.0988 | 4.0988 | 4.0988 | 4.0988 | O3 | 1.3926 | 2.2919 | | 2.2653 | 1.3927 | 2.3350 | 2.0341 | 2.0341 | 3.0837 | 3.0837 | O4 | 1.3926 | 2.2919 | 2.2653 | | 2.3350 | 1.3927 | 3.0837 | 3.0837 | 2.0341 | 2.0341 | C5 | 2.2914 | 3.4273 | 1.3927 | 2.3350 | | 1.5506 | 1.0911 | 1.0911 | 2.2062 | 2.2062 | C6 | 2.2914 | 3.4273 | 2.3350 | 1.3927 | 1.5506 | | 2.2062 | 2.2062 | 1.0911 | 1.0911 | H7 | 3.0268 | 4.0988 | 2.0341 | 3.0837 | 1.0911 | 2.2062 | | 1.7762 | 2.9627 | 2.3712 | H8 | 3.0268 | 4.0988 | 2.0341 | 3.0837 | 1.0911 | 2.2062 | 1.7762 | | 2.3712 | 2.9627 | H9 | 3.0268 | 4.0988 | 3.0837 | 2.0341 | 2.2062 | 1.0911 | 2.9627 | 2.3712 | | 1.7762 | H10 | 3.0268 | 4.0988 | 3.0837 | 2.0341 | 2.2062 | 1.0911 | 2.3712 | 2.9627 | 1.7762 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.711 |
|
C1 |
O4 |
C6 |
110.711 |
| O2 |
C1 |
O3 |
125.579 |
|
O2 |
C1 |
O4 |
125.579 |
| O3 |
C1 |
O4 |
108.842 |
|
O3 |
C5 |
C6 |
104.869 |
| O3 |
C5 |
H7 |
109.363 |
|
O3 |
C5 |
H8 |
109.363 |
| O4 |
C6 |
C5 |
104.869 |
|
O4 |
C6 |
H9 |
109.363 |
| O4 |
C6 |
H10 |
109.363 |
|
C5 |
C6 |
H9 |
112.088 |
| C5 |
C6 |
H10 |
112.088 |
|
C6 |
C5 |
H7 |
112.088 |
| C6 |
C5 |
H8 |
112.088 |
|
H7 |
C5 |
H8 |
108.961 |
| H9 |
C6 |
H10 |
108.961 |
|
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 |
0.483 |
|
|
|
| 2 |
O |
-0.295 |
|
|
|
| 3 |
O |
-0.310 |
|
|
|
| 4 |
O |
-0.310 |
|
|
|
| 5 |
C |
-0.035 |
|
|
|
| 6 |
C |
-0.035 |
|
|
|
| 7 |
H |
0.126 |
|
|
|
| 8 |
H |
0.126 |
|
|
|
| 9 |
H |
0.126 |
|
|
|
| 10 |
H |
0.126 |
|
|
|
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 |
-4.802 |
4.802 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.183 |
0.000 |
0.000 |
| y |
0.000 |
-36.687 |
0.000 |
| z |
0.000 |
0.000 |
-35.734 |
|
| Traceless |
| | x | y | z |
| x |
4.028 |
0.000 |
0.000 |
| y |
0.000 |
-2.729 |
0.000 |
| z |
0.000 |
0.000 |
-1.299 |
|
| Polar |
| 3z2-r2 | -2.598 |
| x2-y2 | 4.505 |
| 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 |
4.268 |
0.000 |
0.000 |
| y |
0.000 |
5.241 |
0.000 |
| z |
0.000 |
0.000 |
7.444 |
<r2> (average value of r
2) Å
2
| <r2> |
128.965 |
| (<r2>)1/2 |
11.356 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -342.191782 |
| Energy at 298.15K | -342.198203 |
| HF Energy | -341.860075 |
| Nuclear repulsion energy | 246.042386 |
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 |
3138 |
3138 |
18.94 |
|
|
|
| 2 |
A |
3057 |
3057 |
30.22 |
|
|
|
| 3 |
A |
1933 |
1933 |
574.24 |
|
|
|
| 4 |
A |
1553 |
1553 |
2.45 |
|
|
|
| 5 |
A |
1416 |
1416 |
6.05 |
|
|
|
| 6 |
A |
1268 |
1268 |
15.89 |
|
|
|
| 7 |
A |
1208 |
1208 |
129.43 |
|
|
|
| 8 |
A |
1159 |
1159 |
82.25 |
|
|
|
| 9 |
A |
959 |
959 |
4.79 |
|
|
|
| 10 |
A |
819 |
819 |
42.39 |
|
|
|
| 11 |
A |
721 |
721 |
0.82 |
|
|
|
| 12 |
A |
157 |
157 |
0.65 |
|
|
|
| 13 |
B |
3148 |
3148 |
29.73 |
|
|
|
| 14 |
B |
3063 |
3063 |
52.73 |
|
|
|
| 15 |
B |
1546 |
1546 |
5.08 |
|
|
|
| 16 |
B |
1413 |
1413 |
11.43 |
|
|
|
| 17 |
B |
1283 |
1283 |
5.79 |
|
|
|
| 18 |
B |
1171 |
1171 |
3.65 |
|
|
|
| 19 |
B |
1027 |
1027 |
279.27 |
|
|
|
| 20 |
B |
905 |
905 |
23.99 |
|
|
|
| 21 |
B |
770 |
770 |
23.86 |
|
|
|
| 22 |
B |
684 |
684 |
1.90 |
|
|
|
| 23 |
B |
509 |
509 |
0.23 |
|
|
|
| 24 |
B |
149 |
149 |
1.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16527.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 16527.3 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 C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.863 |
| O2 |
0.000 |
0.000 |
2.045 |
| O3 |
0.000 |
1.132 |
0.046 |
| O4 |
0.000 |
-1.132 |
0.046 |
| C5 |
0.209 |
0.738 |
-1.277 |
| C6 |
-0.209 |
-0.738 |
-1.277 |
| H7 |
-0.397 |
1.355 |
-1.939 |
| H8 |
1.266 |
0.858 |
-1.534 |
| H9 |
0.397 |
-1.355 |
-1.939 |
| H10 |
-1.266 |
-0.858 |
-1.534 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1821 | 1.3962 | 1.3962 | 2.2728 | 2.2728 | 3.1369 | 2.8427 | 3.1369 | 2.8427 |
O2 | 1.1821 | | 2.2972 | 2.2972 | 3.4089 | 3.4089 | 4.2261 | 3.8916 | 4.2261 | 3.8916 | O3 | 1.3962 | 2.2972 | | 2.2649 | 1.3962 | 2.3005 | 2.0362 | 2.0431 | 3.2066 | 2.8388 | O4 | 1.3962 | 2.2972 | 2.2649 | | 2.3005 | 1.3962 | 3.2066 | 2.8388 | 2.0362 | 2.0431 | C5 | 2.2728 | 3.4089 | 1.3962 | 2.3005 | | 1.5341 | 1.0889 | 1.0942 | 2.2028 | 2.1881 | C6 | 2.2728 | 3.4089 | 2.3005 | 1.3962 | 1.5341 | | 2.2028 | 2.1881 | 1.0889 | 1.0942 | H7 | 3.1369 | 4.2261 | 2.0362 | 3.2066 | 1.0889 | 2.2028 | | 1.7822 | 2.8231 | 2.4109 | H8 | 2.8427 | 3.8916 | 2.0431 | 2.8388 | 1.0942 | 2.1881 | 1.7822 | | 2.4109 | 3.0581 | H9 | 3.1369 | 4.2261 | 3.2066 | 2.0362 | 2.2028 | 1.0889 | 2.8231 | 2.4109 | | 1.7822 | H10 | 2.8427 | 3.8916 | 2.8388 | 2.0431 | 2.1881 | 1.0942 | 2.4109 | 3.0581 | 1.7822 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.966 |
|
C1 |
O4 |
C6 |
108.966 |
| O2 |
C1 |
O3 |
125.795 |
|
O2 |
C1 |
O4 |
125.795 |
| O3 |
C1 |
O4 |
108.410 |
|
O3 |
C5 |
C6 |
103.356 |
| O3 |
C5 |
H7 |
109.424 |
|
O3 |
C5 |
H8 |
109.657 |
| O4 |
C6 |
C5 |
103.356 |
|
O4 |
C6 |
H9 |
109.424 |
| O4 |
C6 |
H10 |
109.657 |
|
C5 |
C6 |
H9 |
113.145 |
| C5 |
C6 |
H10 |
111.622 |
|
C6 |
C5 |
H7 |
113.145 |
| C6 |
C5 |
H8 |
111.622 |
|
H7 |
C5 |
H8 |
109.447 |
| H9 |
C6 |
H10 |
109.447 |
|
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 |
0.485 |
|
|
|
| 2 |
O |
-0.291 |
|
|
|
| 3 |
O |
-0.311 |
|
|
|
| 4 |
O |
-0.311 |
|
|
|
| 5 |
C |
-0.036 |
|
|
|
| 6 |
C |
-0.036 |
|
|
|
| 7 |
H |
0.127 |
|
|
|
| 8 |
H |
0.123 |
|
|
|
| 9 |
H |
0.127 |
|
|
|
| 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 |
-4.735 |
4.735 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.288 |
0.208 |
0.000 |
| y |
0.208 |
-36.682 |
0.000 |
| z |
0.000 |
0.000 |
-35.524 |
|
| Traceless |
| | x | y | z |
| x |
3.815 |
0.208 |
0.000 |
| y |
0.208 |
-2.776 |
0.000 |
| z |
0.000 |
0.000 |
-1.038 |
|
| Polar |
| 3z2-r2 | -2.077 |
| x2-y2 | 4.394 |
| xy | 0.208 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.380 |
0.158 |
0.000 |
| y |
0.158 |
5.191 |
0.000 |
| z |
0.000 |
0.000 |
7.406 |
<r2> (average value of r
2) Å
2
| <r2> |
127.727 |
| (<r2>)1/2 |
11.302 |