Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -190.623369 |
| Energy at 298.15K | |
| HF Energy | -190.623369 |
| Nuclear repulsion energy | 87.012020 |
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/LANL2DZ
| 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 |
3098 |
2978 |
27.30 |
185.05 |
0.12 |
0.21 |
| 2 |
A1 |
2291 |
2203 |
763.14 |
48.39 |
0.32 |
0.48 |
| 3 |
A1 |
1728 |
1661 |
59.81 |
0.26 |
0.72 |
0.84 |
| 4 |
A1 |
1485 |
1428 |
2.01 |
17.17 |
0.63 |
0.78 |
| 5 |
A1 |
901 |
866 |
10.98 |
47.73 |
0.28 |
0.44 |
| 6 |
B1 |
1039 |
999 |
42.59 |
2.66 |
0.75 |
0.86 |
| 7 |
B1 |
640 |
615 |
24.94 |
2.97 |
0.75 |
0.86 |
| 8 |
B1 |
231 |
222 |
0.85 |
3.79 |
0.75 |
0.86 |
| 9 |
B2 |
3189 |
3065 |
16.57 |
111.72 |
0.75 |
0.86 |
| 10 |
B2 |
1068 |
1026 |
0.27 |
0.15 |
0.75 |
0.86 |
| 11 |
B2 |
437 |
420 |
14.49 |
2.37 |
0.75 |
0.86 |
| 12 |
B2 |
90 |
87 |
21.99 |
0.23 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8098.7 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 7784.5 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/LANL2DZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.900 |
| C2 |
0.000 |
0.000 |
-0.566 |
| C3 |
0.000 |
0.000 |
0.719 |
| O4 |
0.000 |
0.000 |
1.931 |
| H5 |
0.000 |
0.927 |
-2.479 |
| H6 |
0.000 |
-0.927 |
-2.479 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3340 | 2.6190 | 3.8308 | 1.0932 | 1.0932 |
C2 | 1.3340 | | 1.2849 | 2.4968 | 2.1259 | 2.1259 | C3 | 2.6190 | 1.2849 | | 1.2118 | 3.3297 | 3.3297 | O4 | 3.8308 | 2.4968 | 1.2118 | | 4.5062 | 4.5062 | H5 | 1.0932 | 2.1259 | 3.3297 | 4.5062 | | 1.8546 | H6 | 1.0932 | 2.1259 | 3.3297 | 4.5062 | 1.8546 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
180.000 |
|
C2 |
C1 |
H5 |
121.981 |
| C2 |
C1 |
H6 |
121.981 |
|
C2 |
C3 |
O4 |
180.000 |
| H5 |
C1 |
H6 |
116.038 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.418 |
|
|
|
| 2 |
C |
-0.097 |
|
|
|
| 3 |
C |
0.218 |
|
|
|
| 4 |
O |
-0.171 |
|
|
|
| 5 |
H |
0.234 |
|
|
|
| 6 |
H |
0.234 |
|
|
|
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 |
-3.399 |
3.399 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.844 |
0.000 |
0.000 |
| y |
0.000 |
-22.418 |
0.000 |
| z |
0.000 |
0.000 |
-22.295 |
|
| Traceless |
| | x | y | z |
| x |
-0.488 |
0.000 |
0.000 |
| y |
0.000 |
0.152 |
0.000 |
| z |
0.000 |
0.000 |
0.336 |
|
| Polar |
| 3z2-r2 | 0.671 |
| x2-y2 | -0.426 |
| 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 |
1.859 |
0.000 |
0.000 |
| y |
0.000 |
2.527 |
0.000 |
| z |
0.000 |
0.000 |
10.739 |
<r2> (average value of r
2) Å
2
| <r2> |
84.582 |
| (<r2>)1/2 |
9.197 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -190.623369 |
| Energy at 298.15K | |
| HF Energy | -190.623369 |
| Nuclear repulsion energy | 87.011607 |
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/LANL2DZ
| 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' |
3189 |
3066 |
16.54 |
111.66 |
0.75 |
0.86 |
| 2 |
A' |
3098 |
2978 |
27.26 |
184.99 |
0.12 |
0.21 |
| 3 |
A' |
2291 |
2202 |
763.18 |
48.41 |
0.32 |
0.48 |
| 4 |
A' |
1728 |
1660 |
59.76 |
0.26 |
0.72 |
0.84 |
| 5 |
A' |
1485 |
1428 |
2.01 |
17.16 |
0.64 |
0.78 |
| 6 |
A' |
1068 |
1027 |
0.27 |
0.15 |
0.75 |
0.86 |
| 7 |
A' |
901 |
866 |
10.97 |
47.73 |
0.28 |
0.44 |
| 8 |
A' |
437 |
420 |
14.49 |
2.37 |
0.75 |
0.86 |
| 9 |
A' |
90 |
87 |
21.99 |
0.23 |
0.75 |
0.86 |
| 10 |
A" |
1039 |
999 |
42.60 |
2.67 |
0.75 |
0.86 |
| 11 |
A" |
640 |
615 |
24.95 |
2.97 |
0.75 |
0.86 |
| 12 |
A" |
231 |
222 |
0.86 |
3.79 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8098.7 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 7784.5 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/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.001 |
-1.900 |
0.000 |
| C2 |
0.000 |
-0.566 |
0.000 |
| C3 |
0.000 |
0.719 |
0.000 |
| O4 |
0.001 |
1.931 |
0.000 |
| H5 |
0.926 |
-2.480 |
0.000 |
| H6 |
-0.929 |
-2.479 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3341 | 2.6190 | 3.8308 | 1.0932 | 1.0932 |
C2 | 1.3341 | | 1.2850 | 2.4968 | 2.1258 | 2.1258 | C3 | 2.6190 | 1.2850 | | 1.2118 | 3.3297 | 3.3294 | O4 | 3.8308 | 2.4968 | 1.2118 | | 4.5062 | 4.5060 | H5 | 1.0932 | 2.1258 | 3.3297 | 4.5062 | | 1.8548 | H6 | 1.0932 | 2.1258 | 3.3294 | 4.5060 | 1.8548 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
179.969 |
|
C2 |
C1 |
H5 |
121.966 |
| C2 |
C1 |
H6 |
121.973 |
|
C2 |
C3 |
O4 |
179.971 |
| H5 |
C1 |
H6 |
116.061 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.419 |
|
|
|
| 2 |
C |
-0.097 |
|
|
|
| 3 |
C |
0.218 |
|
|
|
| 4 |
O |
-0.171 |
|
|
|
| 5 |
H |
0.234 |
|
|
|
| 6 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.003 |
-3.399 |
0.000 |
3.399 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.417 |
0.001 |
0.000 |
| y |
0.001 |
-22.296 |
0.000 |
| z |
0.000 |
0.000 |
-22.844 |
|
| Traceless |
| | x | y | z |
| x |
0.153 |
0.001 |
0.000 |
| y |
0.001 |
0.334 |
0.000 |
| z |
0.000 |
0.000 |
-0.488 |
|
| Polar |
| 3z2-r2 | -0.975 |
| x2-y2 | -0.121 |
| 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 |
2.527 |
0.003 |
0.000 |
| y |
0.003 |
10.739 |
0.000 |
| z |
0.000 |
0.000 |
1.859 |
<r2> (average value of r
2) Å
2
| <r2> |
84.583 |
| (<r2>)1/2 |
9.197 |