Jump to
S1C2
Energy calculated at B1B95/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -151.923333 |
| Energy at 298.15K | |
| HF Energy | -151.923333 |
| Nuclear repulsion energy | 52.794749 |
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/daug-cc-pVTZ
| 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 |
3478 |
3478 |
118.50 |
49.89 |
0.23 |
0.38 |
| 2 |
Σ |
2116 |
2116 |
259.79 |
13.64 |
0.36 |
0.53 |
| 3 |
Σ |
1326 |
1326 |
24.25 |
46.61 |
0.13 |
0.23 |
| 4 |
Π |
575 |
575 |
0.62 |
0.23 |
0.75 |
0.86 |
| 4 |
Π |
528 |
528 |
10.25 |
0.72 |
0.75 |
0.86 |
| 5 |
Π |
462 |
462 |
18.94 |
0.16 |
0.75 |
0.86 |
| 5 |
Π |
336i |
336i |
117.07 |
6.35 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4074.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4074.9 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/daug-cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.020 |
| C2 |
0.000 |
0.000 |
-1.234 |
| O3 |
0.000 |
0.000 |
1.197 |
| H4 |
0.000 |
0.000 |
-2.293 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2535 | 1.1778 | 2.3128 |
C2 | 1.2535 | | 2.4313 | 1.0592 | O3 | 1.1778 | 2.4313 | | 3.4905 | H4 | 2.3128 | 1.0592 | 3.4905 | |
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/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.222 |
|
|
|
| 2 |
C |
-0.390 |
|
|
|
| 3 |
O |
-0.811 |
|
|
|
| 4 |
H |
0.979 |
|
|
|
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 |
-2.145 |
2.145 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.207 |
0.000 |
0.000 |
| y |
0.000 |
-17.897 |
0.000 |
| z |
0.000 |
0.000 |
-14.837 |
|
| Traceless |
| | x | y | z |
| x |
0.160 |
0.000 |
0.000 |
| y |
0.000 |
-2.375 |
0.000 |
| z |
0.000 |
0.000 |
2.215 |
|
| Polar |
| 3z2-r2 | 4.430 |
| x2-y2 | 1.690 |
| 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 |
2.748 |
0.000 |
0.000 |
| y |
0.000 |
3.058 |
0.000 |
| z |
0.000 |
0.000 |
6.230 |
<r2> (average value of r
2) Å
2
| <r2> |
36.055 |
| (<r2>)1/2 |
6.005 |
Jump to
S1C1
Energy calculated at B1B95/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -151.925104 |
| Energy at 298.15K | |
| HF Energy | -151.925104 |
| Nuclear repulsion energy | 52.675607 |
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/daug-cc-pVTZ
| 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' |
3364 |
3364 |
47.85 |
75.67 |
0.30 |
0.46 |
| 2 |
A' |
2109 |
2109 |
347.64 |
9.79 |
0.62 |
0.77 |
| 3 |
A' |
1279 |
1279 |
6.31 |
40.64 |
0.14 |
0.25 |
| 4 |
A' |
573 |
573 |
6.44 |
3.05 |
0.71 |
0.83 |
| 5 |
A' |
449 |
449 |
235.03 |
1.23 |
0.20 |
0.34 |
| 6 |
A" |
509 |
509 |
2.42 |
0.74 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4141.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4141.1 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/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.046 |
0.000 |
| C2 |
1.043 |
-0.703 |
0.000 |
| O3 |
-1.045 |
0.565 |
0.000 |
| H4 |
2.104 |
-0.572 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2844 | 1.1670 | 2.1930 |
C2 | 1.2844 | | 2.4434 | 1.0689 | O3 | 1.1670 | 2.4434 | | 3.3483 | H4 | 2.1930 | 1.0689 | 3.3483 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
137.262 |
|
C2 |
C1 |
O3 |
170.698 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.327 |
|
|
|
| 2 |
C |
-0.654 |
|
|
|
| 3 |
O |
-0.645 |
|
|
|
| 4 |
H |
0.972 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.666 |
0.251 |
0.000 |
1.684 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.129 |
0.713 |
0.000 |
| y |
0.713 |
-19.057 |
0.000 |
| z |
0.000 |
0.000 |
-16.333 |
|
| Traceless |
| | x | y | z |
| x |
2.566 |
0.713 |
0.000 |
| y |
0.713 |
-3.325 |
0.000 |
| z |
0.000 |
0.000 |
0.760 |
|
| Polar |
| 3z2-r2 | 1.520 |
| x2-y2 | 3.927 |
| xy | 0.713 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.305 |
-1.481 |
0.000 |
| y |
-1.481 |
4.142 |
0.000 |
| z |
0.000 |
0.000 |
3.129 |
<r2> (average value of r
2) Å
2
| <r2> |
36.076 |
| (<r2>)1/2 |
6.006 |