Jump to
S1C2
S2C1
S2C2
Energy calculated at M06-2X/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -193.132196 |
| Energy at 298.15K | -193.138135 |
| HF Energy | -193.132196 |
| Nuclear repulsion energy | 119.884947 |
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 M06-2X/6-311+G(3df,2p)
| 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 |
3175 |
3175 |
3.05 |
59.58 |
0.57 |
0.73 |
| 2 |
A |
3119 |
3119 |
0.00 |
8.91 |
0.75 |
0.86 |
| 3 |
A |
3062 |
3062 |
3.78 |
279.34 |
0.00 |
0.01 |
| 4 |
A |
1859 |
1859 |
208.65 |
12.59 |
0.60 |
0.75 |
| 5 |
A |
1476 |
1476 |
29.25 |
11.04 |
0.63 |
0.77 |
| 6 |
A |
1470 |
1470 |
0.00 |
8.01 |
0.75 |
0.86 |
| 7 |
A |
1390 |
1390 |
16.56 |
0.97 |
0.75 |
0.86 |
| 8 |
A |
1086 |
1086 |
0.02 |
1.94 |
0.22 |
0.36 |
| 9 |
A |
886 |
886 |
0.00 |
0.19 |
0.75 |
0.86 |
| 10 |
A |
804 |
804 |
1.28 |
16.05 |
0.11 |
0.19 |
| 11 |
A |
383 |
383 |
1.80 |
0.57 |
0.67 |
0.80 |
| 12 |
A |
39 |
39 |
0.00 |
0.16 |
0.75 |
0.86 |
| 13 |
B |
3174 |
3174 |
7.72 |
45.33 |
0.75 |
0.86 |
| 14 |
B |
3126 |
3126 |
9.72 |
81.81 |
0.75 |
0.86 |
| 15 |
B |
3056 |
3056 |
0.25 |
0.82 |
0.75 |
0.86 |
| 16 |
B |
1494 |
1494 |
20.52 |
0.00 |
0.75 |
0.86 |
| 17 |
B |
1465 |
1465 |
0.26 |
0.77 |
0.75 |
0.86 |
| 18 |
B |
1398 |
1398 |
70.92 |
0.01 |
0.75 |
0.86 |
| 19 |
B |
1248 |
1248 |
62.16 |
3.59 |
0.75 |
0.86 |
| 20 |
B |
1125 |
1125 |
3.23 |
0.09 |
0.75 |
0.86 |
| 21 |
B |
895 |
895 |
4.70 |
1.50 |
0.75 |
0.86 |
| 22 |
B |
541 |
541 |
16.09 |
1.43 |
0.75 |
0.86 |
| 23 |
B |
493 |
493 |
0.57 |
0.35 |
0.75 |
0.86 |
| 24 |
B |
146 |
146 |
0.13 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 18453.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 18453.6 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 M06-2X/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.187 |
| O2 |
0.000 |
0.000 |
1.390 |
| C3 |
0.000 |
1.284 |
-0.610 |
| C4 |
0.000 |
-1.284 |
-0.610 |
| H5 |
0.001 |
2.138 |
0.060 |
| H6 |
-0.001 |
-2.138 |
0.060 |
| H7 |
0.877 |
1.317 |
-1.259 |
| H8 |
-0.878 |
1.318 |
-1.257 |
| H9 |
-0.877 |
-1.317 |
-1.259 |
| H10 |
0.878 |
-1.318 |
-1.257 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.2027 | 1.5112 | 1.5112 | 2.1417 | 2.1417 | 2.1439 | 2.1437 | 2.1439 | 2.1437 |
O2 | 1.2027 | | 2.3766 | 2.3766 | 2.5178 | 2.5178 | 3.0857 | 3.0848 | 3.0857 | 3.0848 | C3 | 1.5112 | 2.3766 | | 2.5672 | 1.0859 | 3.4865 | 1.0913 | 1.0913 | 2.8205 | 2.8214 | C4 | 1.5112 | 2.3766 | 2.5672 | | 3.4865 | 1.0859 | 2.8205 | 2.8214 | 1.0913 | 1.0913 | H5 | 2.1417 | 2.5178 | 1.0859 | 3.4865 | | 4.2758 | 1.7832 | 1.7832 | 3.8014 | 3.8014 | H6 | 2.1417 | 2.5178 | 3.4865 | 1.0859 | 4.2758 | | 3.8014 | 3.8014 | 1.7832 | 1.7832 | H7 | 2.1439 | 3.0857 | 1.0913 | 2.8205 | 1.7832 | 3.8014 | | 1.7550 | 3.1650 | 2.6359 | H8 | 2.1437 | 3.0848 | 1.0913 | 2.8214 | 1.7832 | 3.8014 | 1.7550 | | 2.6359 | 3.1684 | H9 | 2.1439 | 3.0857 | 2.8205 | 1.0913 | 3.8014 | 1.7832 | 3.1650 | 2.6359 | | 1.7550 | H10 | 2.1437 | 3.0848 | 2.8214 | 1.0913 | 3.8014 | 1.7832 | 2.6359 | 3.1684 | 1.7550 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
110.028 |
|
C1 |
C3 |
H7 |
109.883 |
| C1 |
C3 |
H8 |
109.873 |
|
C1 |
C4 |
H6 |
110.028 |
| C1 |
C4 |
H9 |
109.883 |
|
C1 |
C4 |
H10 |
109.873 |
| O2 |
C1 |
C3 |
121.853 |
|
O2 |
C1 |
C4 |
121.853 |
| C3 |
C1 |
C4 |
116.295 |
|
H5 |
C3 |
H7 |
109.982 |
| H5 |
C3 |
H8 |
109.974 |
|
H6 |
C4 |
H9 |
109.982 |
| H6 |
C4 |
H10 |
109.974 |
|
H7 |
C3 |
H8 |
107.053 |
| H9 |
C4 |
H10 |
107.053 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.643 |
|
|
|
| 2 |
O |
-0.742 |
|
|
|
| 3 |
C |
-0.586 |
|
|
|
| 4 |
C |
-0.586 |
|
|
|
| 5 |
H |
0.199 |
|
|
|
| 6 |
H |
0.199 |
|
|
|
| 7 |
H |
0.218 |
|
|
|
| 8 |
H |
0.218 |
|
|
|
| 9 |
H |
0.218 |
|
|
|
| 10 |
H |
0.218 |
|
|
|
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 |
-3.066 |
3.066 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.366 |
-0.001 |
0.000 |
| y |
-0.001 |
-23.616 |
0.000 |
| z |
0.000 |
0.000 |
-29.121 |
|
| Traceless |
| | x | y | z |
| x |
2.002 |
-0.001 |
0.000 |
| y |
-0.001 |
3.128 |
0.000 |
| z |
0.000 |
0.000 |
-5.130 |
|
| Polar |
| 3z2-r2 | -10.260 |
| x2-y2 | -0.750 |
| xy | -0.001 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.861 |
-0.000 |
0.000 |
| y |
-0.000 |
6.535 |
0.000 |
| z |
0.000 |
0.000 |
6.660 |
<r2> (average value of r
2) Å
2
| <r2> |
81.466 |
| (<r2>)1/2 |
9.026 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at M06-2X/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -193.132196 |
| Energy at 298.15K | |
| HF Energy | -193.132196 |
| Nuclear repulsion energy | 119.884740 |
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 M06-2X/6-311+G(3df,2p)
| 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 |
3175 |
3175 |
3.05 |
59.60 |
0.57 |
0.73 |
| 2 |
A |
3119 |
3119 |
0.00 |
8.91 |
0.75 |
0.86 |
| 3 |
A |
3062 |
3062 |
3.78 |
279.33 |
0.00 |
0.01 |
| 4 |
A |
1859 |
1859 |
208.68 |
12.59 |
0.60 |
0.75 |
| 5 |
A |
1476 |
1476 |
29.24 |
11.04 |
0.63 |
0.77 |
| 6 |
A |
1470 |
1470 |
0.00 |
8.01 |
0.75 |
0.86 |
| 7 |
A |
1390 |
1390 |
16.57 |
0.98 |
0.75 |
0.86 |
| 8 |
A |
1086 |
1086 |
0.02 |
1.94 |
0.22 |
0.36 |
| 9 |
A |
886 |
886 |
0.00 |
0.19 |
0.75 |
0.86 |
| 10 |
A |
804 |
804 |
1.28 |
16.05 |
0.11 |
0.19 |
| 11 |
A |
383 |
383 |
1.80 |
0.57 |
0.67 |
0.80 |
| 12 |
A |
39 |
39 |
0.00 |
0.16 |
0.75 |
0.86 |
| 13 |
B |
3174 |
3174 |
7.73 |
45.32 |
0.75 |
0.86 |
| 14 |
B |
3126 |
3126 |
9.71 |
81.80 |
0.75 |
0.86 |
| 15 |
B |
3056 |
3056 |
0.25 |
0.81 |
0.75 |
0.86 |
| 16 |
B |
1494 |
1494 |
20.52 |
0.00 |
0.75 |
0.86 |
| 17 |
B |
1465 |
1465 |
0.26 |
0.77 |
0.75 |
0.86 |
| 18 |
B |
1398 |
1398 |
70.90 |
0.01 |
0.75 |
0.86 |
| 19 |
B |
1248 |
1248 |
62.17 |
3.59 |
0.75 |
0.86 |
| 20 |
B |
1125 |
1125 |
3.23 |
0.09 |
0.75 |
0.86 |
| 21 |
B |
895 |
895 |
4.70 |
1.50 |
0.75 |
0.86 |
| 22 |
B |
541 |
541 |
16.09 |
1.44 |
0.75 |
0.86 |
| 23 |
B |
493 |
493 |
0.57 |
0.35 |
0.75 |
0.86 |
| 24 |
B |
146 |
146 |
0.13 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 18453.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 18453.6 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 M06-2X/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.187 |
| O2 |
0.000 |
0.000 |
1.390 |
| C3 |
0.000 |
1.284 |
-0.611 |
| C4 |
0.000 |
-1.284 |
-0.611 |
| H5 |
0.000 |
2.138 |
0.060 |
| H6 |
-0.000 |
-2.138 |
0.060 |
| H7 |
0.878 |
1.318 |
-1.258 |
| H8 |
-0.878 |
1.318 |
-1.258 |
| H9 |
-0.878 |
-1.318 |
-1.258 |
| H10 |
0.878 |
-1.318 |
-1.258 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.2027 | 1.5112 | 1.5112 | 2.1417 | 2.1417 | 2.1438 | 2.1438 | 2.1438 | 2.1438 |
O2 | 1.2027 | | 2.3767 | 2.3767 | 2.5179 | 2.5179 | 3.0853 | 3.0852 | 3.0853 | 3.0852 | C3 | 1.5112 | 2.3767 | | 2.5671 | 1.0859 | 3.4865 | 1.0913 | 1.0913 | 2.8208 | 2.8208 | C4 | 1.5112 | 2.3767 | 2.5671 | | 3.4865 | 1.0859 | 2.8208 | 2.8208 | 1.0913 | 1.0913 | H5 | 2.1417 | 2.5179 | 1.0859 | 3.4865 | | 4.2759 | 1.7832 | 1.7832 | 3.8013 | 3.8013 | H6 | 2.1417 | 2.5179 | 3.4865 | 1.0859 | 4.2759 | | 3.8013 | 3.8013 | 1.7832 | 1.7832 | H7 | 2.1438 | 3.0853 | 1.0913 | 2.8208 | 1.7832 | 3.8013 | | 1.7551 | 3.1665 | 2.6357 | H8 | 2.1438 | 3.0852 | 1.0913 | 2.8208 | 1.7832 | 3.8013 | 1.7551 | | 2.6357 | 3.1666 | H9 | 2.1438 | 3.0853 | 2.8208 | 1.0913 | 3.8013 | 1.7832 | 3.1665 | 2.6357 | | 1.7551 | H10 | 2.1438 | 3.0852 | 2.8208 | 1.0913 | 3.8013 | 1.7832 | 2.6357 | 3.1666 | 1.7551 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
110.031 |
|
C1 |
C3 |
H7 |
109.875 |
| C1 |
C3 |
H8 |
109.874 |
|
C1 |
C4 |
H6 |
110.031 |
| C1 |
C4 |
H9 |
109.875 |
|
C1 |
C4 |
H10 |
109.874 |
| O2 |
C1 |
C3 |
121.856 |
|
O2 |
C1 |
C4 |
121.856 |
| C3 |
C1 |
C4 |
116.288 |
|
H5 |
C3 |
H7 |
109.979 |
| H5 |
C3 |
H8 |
109.978 |
|
H6 |
C4 |
H9 |
109.979 |
| H6 |
C4 |
H10 |
109.978 |
|
H7 |
C3 |
H8 |
107.057 |
| H9 |
C4 |
H10 |
107.057 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.643 |
|
|
|
| 2 |
O |
-0.742 |
|
|
|
| 3 |
C |
-0.586 |
|
|
|
| 4 |
C |
-0.586 |
|
|
|
| 5 |
H |
0.199 |
|
|
|
| 6 |
H |
0.199 |
|
|
|
| 7 |
H |
0.218 |
|
|
|
| 8 |
H |
0.218 |
|
|
|
| 9 |
H |
0.218 |
|
|
|
| 10 |
H |
0.218 |
|
|
|
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 |
-3.066 |
3.066 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.366 |
0.000 |
0.000 |
| y |
0.000 |
-23.616 |
0.000 |
| z |
0.000 |
0.000 |
-29.122 |
|
| Traceless |
| | x | y | z |
| x |
2.003 |
0.000 |
0.000 |
| y |
0.000 |
3.128 |
0.000 |
| z |
0.000 |
0.000 |
-5.131 |
|
| Polar |
| 3z2-r2 | -10.261 |
| x2-y2 | -0.750 |
| 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 |
4.861 |
0.000 |
0.000 |
| y |
0.000 |
6.535 |
0.000 |
| z |
0.000 |
0.000 |
6.660 |
<r2> (average value of r
2) Å
2
| <r2> |
81.466 |
| (<r2>)1/2 |
9.026 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at M06-2X/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -193.003802 |
| Energy at 298.15K | |
| HF Energy | -193.003802 |
| Nuclear repulsion energy | 118.083974 |
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 M06-2X/6-311+G(3df,2p)
| 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' |
3152 |
3152 |
5.44 |
74.74 |
0.75 |
0.86 |
| 2 |
A' |
3109 |
3109 |
13.08 |
113.44 |
0.28 |
0.43 |
| 3 |
A' |
3009 |
3009 |
38.93 |
307.92 |
0.04 |
0.08 |
| 4 |
A' |
1503 |
1503 |
9.93 |
3.02 |
0.73 |
0.85 |
| 5 |
A' |
1478 |
1478 |
9.33 |
7.60 |
0.74 |
0.85 |
| 6 |
A' |
1403 |
1403 |
2.78 |
2.19 |
0.72 |
0.84 |
| 7 |
A' |
1279 |
1279 |
6.56 |
13.92 |
0.01 |
0.01 |
| 8 |
A' |
1100 |
1100 |
0.07 |
2.40 |
0.74 |
0.85 |
| 9 |
A' |
980 |
980 |
0.54 |
4.83 |
0.05 |
0.10 |
| 10 |
A' |
802 |
802 |
8.24 |
13.88 |
0.12 |
0.21 |
| 11 |
A' |
382 |
382 |
1.19 |
1.33 |
0.74 |
0.85 |
| 12 |
A' |
316 |
316 |
2.27 |
1.81 |
0.70 |
0.82 |
| 13 |
A' |
188 |
188 |
0.35 |
0.73 |
0.70 |
0.82 |
| 14 |
A" |
3152 |
3152 |
7.87 |
34.87 |
0.75 |
0.86 |
| 15 |
A" |
3109 |
3109 |
2.44 |
36.22 |
0.75 |
0.86 |
| 16 |
A" |
3007 |
3007 |
23.19 |
27.39 |
0.75 |
0.86 |
| 17 |
A" |
1480 |
1480 |
0.34 |
6.44 |
0.75 |
0.86 |
| 18 |
A" |
1465 |
1465 |
5.74 |
2.88 |
0.75 |
0.86 |
| 19 |
A" |
1375 |
1375 |
0.23 |
0.75 |
0.75 |
0.86 |
| 20 |
A" |
1148 |
1148 |
0.14 |
9.28 |
0.75 |
0.86 |
| 21 |
A" |
964 |
964 |
2.04 |
0.17 |
0.75 |
0.86 |
| 22 |
A" |
956 |
956 |
0.16 |
1.32 |
0.75 |
0.86 |
| 23 |
A" |
356 |
356 |
3.63 |
0.42 |
0.75 |
0.86 |
| 24 |
A" |
174 |
174 |
0.05 |
0.10 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17943.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 17943.7 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 M06-2X/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.211 |
0.220 |
0.000 |
| O2 |
-0.637 |
1.228 |
0.000 |
| C3 |
0.211 |
-0.553 |
1.296 |
| C4 |
0.211 |
-0.553 |
-1.296 |
| H5 |
-0.715 |
-1.129 |
1.412 |
| H6 |
-0.715 |
-1.129 |
-1.412 |
| H7 |
1.055 |
-1.241 |
1.291 |
| H8 |
0.308 |
0.117 |
2.149 |
| H9 |
1.055 |
-1.241 |
-1.291 |
| H10 |
0.308 |
0.117 |
-2.149 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.3179 | 1.5094 | 1.5094 | 2.1610 | 2.1610 | 2.1246 | 2.1534 | 2.1246 | 2.1534 |
O2 | 1.3179 | | 2.3609 | 2.3609 | 2.7488 | 2.7488 | 3.2602 | 2.5976 | 3.2602 | 2.5976 | C3 | 1.5094 | 2.3609 | | 2.5929 | 1.0965 | 2.9193 | 1.0886 | 1.0882 | 2.8075 | 3.5110 | C4 | 1.5094 | 2.3609 | 2.5929 | | 2.9193 | 1.0965 | 2.8075 | 3.5110 | 1.0886 | 1.0882 | H5 | 2.1610 | 2.7488 | 1.0965 | 2.9193 | | 2.8231 | 1.7770 | 1.7726 | 3.2326 | 3.9082 | H6 | 2.1610 | 2.7488 | 2.9193 | 1.0965 | 2.8231 | | 3.2326 | 3.9082 | 1.7770 | 1.7726 | H7 | 2.1246 | 3.2602 | 1.0886 | 2.8075 | 1.7770 | 3.2326 | | 1.7706 | 2.5829 | 3.7729 | H8 | 2.1534 | 2.5976 | 1.0882 | 3.5110 | 1.7726 | 3.9082 | 1.7706 | | 3.7729 | 4.2974 | H9 | 2.1246 | 3.2602 | 2.8075 | 1.0886 | 3.2326 | 1.7770 | 2.5829 | 3.7729 | | 1.7706 | H10 | 2.1534 | 2.5976 | 3.5110 | 1.0882 | 3.9082 | 1.7726 | 3.7729 | 4.2974 | 1.7706 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.345 |
|
|
|
| 2 |
O |
-0.409 |
|
|
|
| 3 |
C |
-0.583 |
|
|
|
| 4 |
C |
-0.583 |
|
|
|
| 5 |
H |
0.212 |
|
|
|
| 6 |
H |
0.212 |
|
|
|
| 7 |
H |
0.209 |
|
|
|
| 8 |
H |
0.194 |
|
|
|
| 9 |
H |
0.209 |
|
|
|
| 10 |
H |
0.194 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.470 |
-1.761 |
0.000 |
1.823 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.685 |
0.218 |
0.000 |
| y |
0.218 |
-27.168 |
0.000 |
| z |
0.000 |
0.000 |
-23.134 |
|
| Traceless |
| | x | y | z |
| x |
-1.534 |
0.218 |
0.000 |
| y |
0.218 |
-2.258 |
0.000 |
| z |
0.000 |
0.000 |
3.792 |
|
| Polar |
| 3z2-r2 | 7.585 |
| x2-y2 | 0.483 |
| xy | 0.218 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.885 |
-0.384 |
0.000 |
| y |
-0.384 |
6.505 |
0.000 |
| z |
0.000 |
0.000 |
6.888 |
<r2> (average value of r
2) Å
2
| <r2> |
81.929 |
| (<r2>)1/2 |
9.051 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at M06-2X/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -193.003802 |
| Energy at 298.15K | |
| HF Energy | -193.003802 |
| Nuclear repulsion energy | 118.083974 |
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 M06-2X/6-311+G(3df,2p)
Geometric Data calculated at M06-2X/6-311+G(3df,2p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability