Jump to
S1C2
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -149.866964 |
| Energy at 298.15K | |
| HF Energy | -149.866964 |
| Nuclear repulsion energy | 51.023281 |
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 B1B95/STO-3G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3689 |
3257 |
149.27 |
34.71 |
0.30 |
0.46 |
| 2 |
Σ |
2032 |
1794 |
7.37 |
3.06 |
0.12 |
0.22 |
| 3 |
Σ |
1239 |
1094 |
0.24 |
15.02 |
0.30 |
0.46 |
| 4 |
Π |
571 |
504 |
8.38 |
0.27 |
0.75 |
0.86 |
| 4 |
Π |
517 |
456 |
2.82 |
1.02 |
0.75 |
0.86 |
| 5 |
Π |
430 |
380 |
0.51 |
0.90 |
0.75 |
0.86 |
| 5 |
Π |
145 |
128 |
64.55 |
0.44 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4310.4 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 3806.1 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 B1B95/STO-3G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.017 |
| C2 |
0.000 |
0.000 |
-1.259 |
| O3 |
0.000 |
0.000 |
1.249 |
| H4 |
0.000 |
0.000 |
-2.336 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2427 | 1.2657 | 2.3192 |
C2 | 1.2427 | | 2.5084 | 1.0765 | O3 | 1.2657 | 2.5084 | | 3.5849 | H4 | 2.3192 | 1.0765 | 3.5849 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
180.000 |
|
C2 |
C1 |
O3 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.079 |
|
|
|
| 2 |
C |
-0.116 |
|
|
|
| 3 |
O |
-0.095 |
|
|
|
| 4 |
H |
0.133 |
|
|
|
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 |
-1.364 |
1.364 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.529 |
0.000 |
0.000 |
| y |
0.000 |
-14.460 |
0.000 |
| z |
0.000 |
0.000 |
-13.199 |
|
| Traceless |
| | x | y | z |
| x |
-1.700 |
0.000 |
0.000 |
| y |
0.000 |
-0.096 |
0.000 |
| z |
0.000 |
0.000 |
1.795 |
|
| Polar |
| 3z2-r2 | 3.590 |
| x2-y2 | -1.069 |
| 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 |
0.338 |
0.000 |
0.000 |
| y |
0.000 |
0.516 |
0.000 |
| z |
0.000 |
0.000 |
3.733 |
<r2> (average value of r
2) Å
2
| <r2> |
36.447 |
| (<r2>)1/2 |
6.037 |
Jump to
S1C1
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -149.866964 |
| Energy at 298.15K | |
| HF Energy | -149.866964 |
| Nuclear repulsion energy | 51.023074 |
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 B1B95/STO-3G
| 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' |
3689 |
3257 |
149.17 |
34.69 |
0.30 |
0.46 |
| 2 |
A' |
2032 |
1795 |
7.47 |
3.09 |
0.12 |
0.22 |
| 3 |
A' |
1238 |
1093 |
0.23 |
15.00 |
0.30 |
0.46 |
| 4 |
A' |
517 |
456 |
2.86 |
1.02 |
0.75 |
0.86 |
| 5 |
A' |
147 |
130 |
64.45 |
0.47 |
0.71 |
0.83 |
| 6 |
A" |
432 |
381 |
0.13 |
1.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4027.0 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 3555.8 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 B1B95/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
-0.017 |
0.000 |
| C2 |
-0.004 |
-1.259 |
0.000 |
| O3 |
0.004 |
1.249 |
0.000 |
| H4 |
-0.006 |
-2.336 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2425 | 1.2659 | 2.3191 |
C2 | 1.2425 | | 2.5084 | 1.0765 | O3 | 1.2659 | 2.5084 | | 3.5849 | H4 | 2.3191 | 1.0765 | 3.5849 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
179.927 |
|
C2 |
C1 |
O3 |
179.986 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.079 |
|
|
|
| 2 |
C |
-0.116 |
|
|
|
| 3 |
O |
-0.095 |
|
|
|
| 4 |
H |
0.133 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.003 |
-1.364 |
0.000 |
1.364 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.529 |
0.004 |
0.000 |
| y |
0.004 |
-13.198 |
0.000 |
| z |
0.000 |
0.000 |
-14.460 |
|
| Traceless |
| | x | y | z |
| x |
-1.700 |
0.004 |
0.000 |
| y |
0.004 |
1.796 |
0.000 |
| z |
0.000 |
0.000 |
-0.096 |
|
| Polar |
| 3z2-r2 | -0.193 |
| x2-y2 | -2.331 |
| xy | 0.004 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.338 |
0.011 |
0.000 |
| y |
0.011 |
3.733 |
0.000 |
| z |
0.000 |
0.000 |
0.516 |
<r2> (average value of r
2) Å
2
| <r2> |
36.446 |
| (<r2>)1/2 |
6.037 |