Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/3-21G*
| | hartrees |
| Energy at 0K | -191.765482 |
| Energy at 298.15K | |
| HF Energy | -191.632437 |
| Nuclear repulsion energy | 125.285967 |
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=FULLultrafine/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 |
3133 |
3133 |
16.93 |
|
|
|
| 2 |
A1 |
3104 |
3104 |
5.90 |
|
|
|
| 3 |
A1 |
1618 |
1618 |
0.17 |
|
|
|
| 4 |
A1 |
1555 |
1555 |
3.07 |
|
|
|
| 5 |
A1 |
1379 |
1379 |
0.05 |
|
|
|
| 6 |
A1 |
1001 |
1001 |
0.00 |
|
|
|
| 7 |
A1 |
852 |
852 |
7.43 |
|
|
|
| 8 |
A1 |
801 |
801 |
7.37 |
|
|
|
| 9 |
A2 |
3151 |
3151 |
0.00 |
|
|
|
| 10 |
A2 |
1287 |
1287 |
0.00 |
|
|
|
| 11 |
A2 |
1142 |
1142 |
0.00 |
|
|
|
| 12 |
A2 |
887 |
887 |
0.00 |
|
|
|
| 13 |
B1 |
3195 |
3195 |
39.33 |
|
|
|
| 14 |
B1 |
3149 |
3149 |
52.54 |
|
|
|
| 15 |
B1 |
1226 |
1226 |
2.24 |
|
|
|
| 16 |
B1 |
1105 |
1105 |
0.37 |
|
|
|
| 17 |
B1 |
776 |
776 |
0.99 |
|
|
|
| 18 |
B1 |
86 |
86 |
3.23 |
|
|
|
| 19 |
B2 |
3096 |
3096 |
105.28 |
|
|
|
| 20 |
B2 |
1589 |
1589 |
2.42 |
|
|
|
| 21 |
B2 |
1322 |
1322 |
20.01 |
|
|
|
| 22 |
B2 |
1296 |
1296 |
0.62 |
|
|
|
| 23 |
B2 |
970 |
970 |
39.96 |
|
|
|
| 24 |
B2 |
915 |
915 |
20.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19317.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19317.1 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=FULLultrafine/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.116 |
| C2 |
0.000 |
0.000 |
-1.084 |
| C3 |
0.000 |
1.072 |
0.050 |
| C4 |
0.000 |
-1.072 |
0.050 |
| H5 |
0.894 |
0.000 |
-1.707 |
| H6 |
-0.894 |
0.000 |
-1.707 |
| H7 |
0.896 |
1.691 |
0.100 |
| H8 |
-0.896 |
1.691 |
0.100 |
| H9 |
-0.896 |
-1.691 |
0.100 |
| H10 |
0.896 |
-1.691 |
0.100 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1997 | 1.5122 | 1.5122 | 2.9604 | 2.9604 | 2.1670 | 2.1670 | 2.1670 | 2.1670 |
C2 | 2.1997 | | 1.5606 | 1.5606 | 1.0892 | 1.0892 | 2.2508 | 2.2508 | 2.2508 | 2.2508 | C3 | 1.5122 | 1.5606 | | 2.1450 | 2.2435 | 2.2435 | 1.0905 | 1.0905 | 2.9060 | 2.9060 | C4 | 1.5122 | 1.5606 | 2.1450 | | 2.2435 | 2.2435 | 2.9060 | 2.9060 | 1.0905 | 1.0905 | H5 | 2.9604 | 1.0892 | 2.2435 | 2.2435 | | 1.7876 | 2.4747 | 3.0544 | 3.0544 | 2.4747 | H6 | 2.9604 | 1.0892 | 2.2435 | 2.2435 | 1.7876 | | 3.0544 | 2.4747 | 2.4747 | 3.0544 | H7 | 2.1670 | 2.2508 | 1.0905 | 2.9060 | 2.4747 | 3.0544 | | 1.7930 | 3.8285 | 3.3827 | H8 | 2.1670 | 2.2508 | 1.0905 | 2.9060 | 3.0544 | 2.4747 | 1.7930 | | 3.3827 | 3.8285 | H9 | 2.1670 | 2.2508 | 2.9060 | 1.0905 | 3.0544 | 2.4747 | 3.8285 | 3.3827 | | 1.7930 | H10 | 2.1670 | 2.2508 | 2.9060 | 1.0905 | 2.4747 | 3.0544 | 3.3827 | 3.8285 | 1.7930 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.416 |
|
O1 |
C3 |
H7 |
111.711 |
| O1 |
C3 |
H8 |
111.711 |
|
O1 |
C4 |
C2 |
91.416 |
| O1 |
C4 |
H9 |
111.711 |
|
O1 |
C4 |
H10 |
111.711 |
| C2 |
C3 |
H7 |
115.059 |
|
C2 |
C3 |
H8 |
115.059 |
| C2 |
C4 |
H9 |
115.059 |
|
C2 |
C4 |
H10 |
115.059 |
| C3 |
O1 |
C4 |
90.345 |
|
C3 |
C2 |
C4 |
86.823 |
| C3 |
C2 |
H5 |
114.531 |
|
C3 |
C2 |
H6 |
114.531 |
| C4 |
C2 |
H5 |
114.531 |
|
C4 |
C2 |
H6 |
114.531 |
| H5 |
C2 |
H6 |
110.284 |
|
H7 |
C3 |
H8 |
110.587 |
| H9 |
C4 |
H10 |
110.587 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/3-21G*
| | hartrees |
| Energy at 0K | -191.765482 |
| Energy at 298.15K | |
| HF Energy | -191.632431 |
| Nuclear repulsion energy | 125.286829 |
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=FULLultrafine/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' |
3194 |
3194 |
39.72 |
|
|
|
| 2 |
A' |
3148 |
3148 |
52.19 |
|
|
|
| 3 |
A' |
3133 |
3133 |
16.92 |
|
|
|
| 4 |
A' |
3104 |
3104 |
5.95 |
|
|
|
| 5 |
A' |
1618 |
1618 |
0.17 |
|
|
|
| 6 |
A' |
1556 |
1556 |
3.07 |
|
|
|
| 7 |
A' |
1380 |
1380 |
0.05 |
|
|
|
| 8 |
A' |
1226 |
1226 |
2.24 |
|
|
|
| 9 |
A' |
1105 |
1105 |
0.37 |
|
|
|
| 10 |
A' |
1001 |
1001 |
0.00 |
|
|
|
| 11 |
A' |
852 |
852 |
7.42 |
|
|
|
| 12 |
A' |
801 |
801 |
7.38 |
|
|
|
| 13 |
A' |
777 |
777 |
0.99 |
|
|
|
| 14 |
A' |
86 |
86 |
3.23 |
|
|
|
| 15 |
A" |
3150 |
3150 |
0.00 |
|
|
|
| 16 |
A" |
3096 |
3096 |
105.30 |
|
|
|
| 17 |
A" |
1589 |
1589 |
2.41 |
|
|
|
| 18 |
A" |
1322 |
1322 |
20.09 |
|
|
|
| 19 |
A" |
1296 |
1296 |
0.57 |
|
|
|
| 20 |
A" |
1287 |
1287 |
0.00 |
|
|
|
| 21 |
A" |
1142 |
1142 |
0.00 |
|
|
|
| 22 |
A" |
970 |
970 |
39.48 |
|
|
|
| 23 |
A" |
915 |
915 |
21.12 |
|
|
|
| 24 |
A" |
888 |
888 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19317.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19317.4 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 B2PLYP=FULLultrafine/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.001 |
-1.116 |
0.000 |
| C2 |
-0.000 |
1.084 |
0.000 |
| C3 |
-0.000 |
-0.049 |
1.072 |
| C4 |
-0.000 |
-0.049 |
-1.072 |
| H5 |
0.893 |
1.707 |
0.000 |
| H6 |
-0.894 |
1.707 |
0.000 |
| H7 |
0.896 |
-0.099 |
1.692 |
| H8 |
-0.897 |
-0.100 |
1.691 |
| H9 |
0.896 |
-0.099 |
-1.692 |
| H10 |
-0.897 |
-0.100 |
-1.691 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1998 | 1.5123 | 1.5123 | 2.9604 | 2.9611 | 2.1673 | 2.1672 | 2.1673 | 2.1672 |
C2 | 2.1998 | | 1.5603 | 1.5603 | 1.0893 | 1.0893 | 2.2507 | 2.2505 | 2.2507 | 2.2505 | C3 | 1.5123 | 1.5603 | | 2.1447 | 2.2435 | 2.2435 | 1.0906 | 1.0906 | 2.9064 | 2.9054 | C4 | 1.5123 | 1.5603 | 2.1447 | | 2.2435 | 2.2435 | 2.9064 | 2.9054 | 1.0906 | 1.0906 | H5 | 2.9604 | 1.0893 | 2.2435 | 2.2435 | | 1.7872 | 2.4749 | 3.0544 | 2.4749 | 3.0544 | H6 | 2.9611 | 1.0893 | 2.2435 | 2.2435 | 1.7872 | | 3.0541 | 2.4746 | 3.0541 | 2.4746 | H7 | 2.1673 | 2.2507 | 1.0906 | 2.9064 | 2.4749 | 3.0541 | | 1.7929 | 3.3840 | 3.8285 | H8 | 2.1672 | 2.2505 | 1.0906 | 2.9054 | 3.0544 | 2.4746 | 1.7929 | | 3.8285 | 3.3815 | H9 | 2.1673 | 2.2507 | 2.9064 | 1.0906 | 2.4749 | 3.0541 | 3.3840 | 3.8285 | | 1.7929 | H10 | 2.1672 | 2.2505 | 2.9054 | 1.0906 | 3.0544 | 2.4746 | 3.8285 | 3.3815 | 1.7929 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.424 |
|
O1 |
C3 |
H7 |
111.720 |
| O1 |
C3 |
H8 |
111.715 |
|
O1 |
C4 |
C2 |
91.424 |
| O1 |
C4 |
H9 |
111.720 |
|
O1 |
C4 |
H10 |
111.715 |
| C2 |
C3 |
H7 |
115.066 |
|
C2 |
C3 |
H8 |
115.049 |
| C2 |
C4 |
H9 |
115.066 |
|
C2 |
C4 |
H10 |
115.049 |
| C3 |
O1 |
C4 |
90.322 |
|
C3 |
C2 |
C4 |
86.830 |
| C3 |
C2 |
H5 |
114.544 |
|
C3 |
C2 |
H6 |
114.543 |
| C4 |
C2 |
H5 |
114.544 |
|
C4 |
C2 |
H6 |
114.543 |
| H5 |
C2 |
H6 |
110.241 |
|
H7 |
C3 |
H8 |
110.574 |
| H9 |
C4 |
H10 |
110.574 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability