Jump to
S1C2
Energy calculated at HSEh1PBE/3-21G
| | hartrees |
| Energy at 0K | -89.969836 |
| Energy at 298.15K | -89.969530 |
| HF Energy | -89.969836 |
| Nuclear repulsion energy | 17.425614 |
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 HSEh1PBE/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' |
3914 |
3770 |
180.72 |
125.36 |
0.37 |
0.54 |
| 2 |
A' |
1405 |
1354 |
66.61 |
14.54 |
0.28 |
0.44 |
| 3 |
A' |
246 |
237 |
212.70 |
3.64 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 2782.7 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 2680.5 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 HSEh1PBE/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
-0.355 |
0.000 |
| Be2 |
0.000 |
1.040 |
0.000 |
| H3 |
-0.001 |
-1.319 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
Be2 |
H3 |
| O1 | | 1.3955 | 0.9634 |
Be2 | 1.3955 | | 2.3590 | H3 | 0.9634 | 2.3590 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be2 |
O1 |
H3 |
179.953 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.669 |
|
|
|
| 2 |
Be |
0.261 |
|
|
|
| 3 |
H |
0.408 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.002 |
-2.027 |
0.000 |
2.027 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.825 |
0.003 |
0.000 |
| y |
0.003 |
-11.164 |
0.000 |
| z |
0.000 |
0.000 |
-11.825 |
|
| Traceless |
| | x | y | z |
| x |
-0.331 |
0.003 |
0.000 |
| y |
0.003 |
0.661 |
0.000 |
| z |
0.000 |
0.000 |
-0.331 |
|
| Polar |
| 3z2-r2 | -0.661 |
| x2-y2 | -0.661 |
| xy | 0.003 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.523 |
0.000 |
0.000 |
| y |
0.000 |
3.499 |
0.000 |
| z |
0.000 |
0.000 |
3.523 |
<r2> (average value of r
2) Å
2
| <r2> |
14.325 |
| (<r2>)1/2 |
3.785 |
Jump to
S1C1
Energy calculated at HSEh1PBE/3-21G
| | hartrees |
| Energy at 0K | -89.969838 |
| Energy at 298.15K | -89.969481 |
| HF Energy | -89.969838 |
| Nuclear repulsion energy | 17.420239 |
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 HSEh1PBE/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 |
Σ |
3909 |
3765 |
180.54 |
|
|
|
| 2 |
Σ |
1404 |
1353 |
66.57 |
|
|
|
| 3 |
Π |
247 |
238 |
213.15 |
|
|
|
| 3 |
Π |
247 |
238 |
213.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2903.7 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 2797.1 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 HSEh1PBE/3-21G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
0.355 |
| Be2 |
0.000 |
0.000 |
-1.041 |
| H3 |
0.000 |
0.000 |
1.319 |
Atom - Atom Distances (Å)
| |
O1 |
Be2 |
H3 |
| O1 | | 1.3960 | 0.9637 |
Be2 | 1.3960 | | 2.3597 | H3 | 0.9637 | 2.3597 | |
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 HSEh1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.669 |
|
|
|
| 2 |
Be |
0.261 |
|
|
|
| 3 |
H |
0.408 |
|
|
|
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 |
2.026 |
2.026 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.825 |
0.000 |
0.000 |
| y |
0.000 |
-11.825 |
0.000 |
| z |
0.000 |
0.000 |
-11.162 |
|
| Traceless |
| | x | y | z |
| x |
-0.332 |
0.000 |
0.000 |
| y |
0.000 |
-0.332 |
0.000 |
| z |
0.000 |
0.000 |
0.663 |
|
| Polar |
| 3z2-r2 | 1.327 |
| 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 |
3.521 |
0.000 |
0.000 |
| y |
0.000 |
3.521 |
0.000 |
| z |
0.000 |
0.000 |
3.503 |
<r2> (average value of r
2) Å
2
| <r2> |
14.330 |
| (<r2>)1/2 |
3.785 |