Jump to
S1C2
Energy calculated at M06-2X/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -90.541485 |
| Energy at 298.15K | -90.541289 |
| HF Energy | -90.541485 |
| Nuclear repulsion energy | 17.567725 |
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/6-31G(2df,p)
| 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' |
4068 |
3875 |
154.76 |
74.87 |
0.28 |
0.43 |
| 2 |
A' |
1310 |
1248 |
104.85 |
5.74 |
0.26 |
0.42 |
| 3 |
A' |
340 |
324 |
174.96 |
5.99 |
0.66 |
0.79 |
Unscaled Zero Point Vibrational Energy (zpe) 2859.3 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 2723.2 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/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.047 |
-0.372 |
0.000 |
| Be2 |
0.047 |
1.021 |
0.000 |
| H3 |
-0.559 |
-1.105 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
Be2 |
H3 |
| O1 | | 1.3933 | 0.9499 |
Be2 | 1.3933 | | 2.2100 | H3 | 0.9499 | 2.2100 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be2 |
O1 |
H3 |
140.426 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.202 |
|
|
|
| 2 |
Be |
-0.132 |
|
|
|
| 3 |
H |
0.334 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.031 |
-0.755 |
0.000 |
1.277 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.670 |
1.470 |
0.000 |
| y |
1.470 |
-11.231 |
0.000 |
| z |
0.000 |
0.000 |
-11.595 |
|
| Traceless |
| | x | y | z |
| x |
0.743 |
1.470 |
0.000 |
| y |
1.470 |
-0.099 |
0.000 |
| z |
0.000 |
0.000 |
-0.644 |
|
| Polar |
| 3z2-r2 | -1.288 |
| x2-y2 | 0.561 |
| xy | 1.470 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.958 |
0.120 |
0.000 |
| y |
0.120 |
3.409 |
0.000 |
| z |
0.000 |
0.000 |
3.771 |
<r2> (average value of r
2) Å
2
| <r2> |
13.811 |
| (<r2>)1/2 |
3.716 |
Jump to
S1C1
Energy calculated at M06-2X/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -90.540808 |
| Energy at 298.15K | |
| HF Energy | -90.540808 |
| Nuclear repulsion energy | 17.722549 |
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/6-31G(2df,p)
| 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 |
4163 |
3965 |
222.52 |
|
|
|
| 2 |
Σ |
1359 |
1294 |
121.02 |
|
|
|
| 3 |
Π |
157i |
150i |
145.10 |
|
|
|
| 3 |
Π |
157i |
150i |
145.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2603.4 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 2479.5 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 M06-2X/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
0.350 |
| Be2 |
0.000 |
0.000 |
-1.024 |
| H3 |
0.000 |
0.000 |
1.295 |
Atom - Atom Distances (Å)
| |
O1 |
Be2 |
H3 |
| O1 | | 1.3736 | 0.9446 |
Be2 | 1.3736 | | 2.3182 | H3 | 0.9446 | 2.3182 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be2 |
O1 |
H3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.155 |
|
|
|
| 2 |
Be |
-0.191 |
|
|
|
| 3 |
H |
0.346 |
|
|
|
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 |
1.360 |
1.360 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.563 |
0.000 |
0.000 |
| y |
0.000 |
-11.563 |
0.000 |
| z |
0.000 |
0.000 |
-10.084 |
|
| Traceless |
| | x | y | z |
| x |
-0.739 |
0.000 |
0.000 |
| y |
0.000 |
-0.739 |
0.000 |
| z |
0.000 |
0.000 |
1.479 |
|
| Polar |
| 3z2-r2 | 2.958 |
| x2-y2 | 0.000 |
| 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 |
3.791 |
0.000 |
0.000 |
| y |
0.000 |
3.791 |
0.000 |
| z |
0.000 |
0.000 |
3.397 |
<r2> (average value of r
2) Å
2
| <r2> |
13.761 |
| (<r2>)1/2 |
3.710 |