Jump to
S1C2
S1C3
Energy calculated at B97D3/6-31G
| | hartrees |
| Energy at 0K | -166.383564 |
| Energy at 298.15K | |
| HF Energy | -166.383564 |
| Nuclear repulsion energy | 49.198383 |
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 B97D3/6-31G
Geometric Data calculated at B97D3/6-31G
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C3
Energy calculated at B97D3/6-31G
| | hartrees |
| Energy at 0K | -166.383759 |
| Energy at 298.15K | |
| HF Energy | -166.383759 |
| Nuclear repulsion energy | 49.070862 |
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 B97D3/6-31G
| 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 |
4013 |
4013 |
0.62 |
|
|
|
| 2 |
A |
766 |
766 |
0.32 |
|
|
|
| 3 |
A |
382 |
382 |
59.93 |
|
|
|
| 4 |
A |
38 |
38 |
431.25 |
|
|
|
| 5 |
A |
64i |
64i |
44.69 |
|
|
|
| 6 |
B |
4012 |
4012 |
314.76 |
|
|
|
| 7 |
B |
1644 |
1644 |
399.51 |
|
|
|
| 8 |
B |
382 |
382 |
58.20 |
|
|
|
| 9 |
B |
19 |
19 |
258.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5595.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5595.4 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 B97D3/6-31G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
0.000 |
| O2 |
0.000 |
1.411 |
-0.008 |
| O3 |
0.000 |
-1.411 |
-0.008 |
| H4 |
0.080 |
2.356 |
0.064 |
| H5 |
-0.080 |
-2.356 |
0.064 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.4105 | 1.4105 | 2.3579 | 2.3579 |
O2 | 1.4105 | | 2.8210 | 0.9513 | 3.7677 | O3 | 1.4105 | 2.8210 | | 3.7677 | 0.9513 | H4 | 2.3579 | 0.9513 | 3.7677 | | 4.7141 | H5 | 2.3579 | 3.7677 | 0.9513 | 4.7141 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
173.253 |
|
Be1 |
O3 |
H5 |
173.253 |
| O2 |
Be1 |
O3 |
179.298 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Be |
0.634 |
|
|
|
| 2 |
O |
-0.702 |
|
|
|
| 3 |
O |
-0.702 |
|
|
|
| 4 |
H |
0.386 |
|
|
|
| 5 |
H |
0.386 |
|
|
|
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 |
0.340 |
0.340 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.448 |
0.923 |
0.000 |
| y |
0.923 |
-7.265 |
0.000 |
| z |
0.000 |
0.000 |
-16.460 |
|
| Traceless |
| | x | y | z |
| x |
-4.585 |
0.923 |
0.000 |
| y |
0.923 |
9.189 |
0.000 |
| z |
0.000 |
0.000 |
-4.603 |
|
| Polar |
| 3z2-r2 | -9.207 |
| x2-y2 | -9.183 |
| xy | 0.923 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.389 |
0.029 |
0.000 |
| y |
0.029 |
3.874 |
0.000 |
| z |
0.000 |
0.000 |
1.389 |
<r2> (average value of r
2) Å
2
| <r2> |
51.317 |
| (<r2>)1/2 |
7.164 |
Jump to
S1C1
S1C2
Energy calculated at B97D3/6-31G
| | hartrees |
| Energy at 0K | -166.383759 |
| Energy at 298.15K | |
| HF Energy | -166.383759 |
| Nuclear repulsion energy | 49.088593 |
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 B97D3/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σg |
4020 |
4020 |
0.00 |
|
|
|
| 2 |
Σg |
767 |
767 |
0.00 |
|
|
|
| 3 |
Σu |
4019 |
4019 |
320.78 |
|
|
|
| 4 |
Σu |
1646 |
1646 |
402.45 |
|
|
|
| 5 |
Πg |
28i |
28i |
0.00 |
|
|
|
| 5 |
Πg |
28i |
28i |
0.00 |
|
|
|
| 6 |
Πu |
383 |
383 |
56.15 |
|
|
|
| 6 |
Πu |
383 |
383 |
56.15 |
|
|
|
| 7 |
Πu |
60 |
60 |
485.06 |
|
|
|
| 7 |
Πu |
60 |
60 |
485.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5639.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5639.9 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 B97D3/6-31G
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
0.000 |
| O2 |
0.000 |
0.000 |
1.410 |
| O3 |
0.000 |
0.000 |
-1.410 |
| H4 |
0.000 |
0.000 |
2.361 |
| H5 |
0.000 |
0.000 |
-2.361 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.4098 | 1.4098 | 2.3608 | 2.3608 |
O2 | 1.4098 | | 2.8196 | 0.9510 | 3.7706 | O3 | 1.4098 | 2.8196 | | 3.7706 | 0.9510 | H4 | 2.3608 | 0.9510 | 3.7706 | | 4.7216 | H5 | 2.3608 | 3.7706 | 0.9510 | 4.7216 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
180.000 |
|
Be1 |
O3 |
H5 |
180.000 |
| O2 |
Be1 |
O3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Be |
0.633 |
|
|
|
| 2 |
O |
-0.702 |
|
|
|
| 3 |
O |
-0.702 |
|
|
|
| 4 |
H |
0.386 |
|
|
|
| 5 |
H |
0.386 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.478 |
0.000 |
0.000 |
| y |
0.000 |
-16.478 |
0.000 |
| z |
0.000 |
0.000 |
-7.109 |
|
| Traceless |
| | x | y | z |
| x |
-4.684 |
0.000 |
0.000 |
| y |
0.000 |
-4.684 |
0.000 |
| z |
0.000 |
0.000 |
9.369 |
|
| Polar |
| 3z2-r2 | 18.737 |
| 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 |
1.381 |
0.000 |
0.000 |
| y |
0.000 |
1.381 |
0.000 |
| z |
0.000 |
0.000 |
3.870 |
<r2> (average value of r
2) Å
2
| <r2> |
51.287 |
| (<r2>)1/2 |
7.162 |