Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G(2df,p)
| hartrees |
Energy at 0K | -166.356904 |
Energy at 298.15K | |
HF Energy | -166.356904 |
Nuclear repulsion energy | 49.251313 |
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/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 |
A1 |
4049 |
3878 |
59.67 |
|
|
|
2 |
A1 |
762 |
730 |
8.46 |
|
|
|
3 |
A1 |
588 |
563 |
145.86 |
|
|
|
4 |
A1 |
305 |
292 |
7.23 |
|
|
|
5 |
A2 |
223i |
214i |
0.00 |
|
|
|
6 |
B1 |
352 |
337 |
61.43 |
|
|
|
7 |
B2 |
4046 |
3875 |
158.65 |
|
|
|
8 |
B2 |
1577 |
1510 |
325.42 |
|
|
|
9 |
B2 |
473 |
453 |
288.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5964.3 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5712.0 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/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Be1 |
0.000 |
0.000 |
0.011 |
O2 |
0.000 |
1.416 |
0.076 |
O3 |
0.000 |
-1.416 |
0.076 |
H4 |
0.000 |
2.049 |
-0.632 |
H5 |
0.000 |
-2.049 |
-0.632 |
Atom - Atom Distances (Å)
|
Be1 |
O2 |
O3 |
H4 |
H5 |
Be1 | | 1.4178 | 1.4178 | 2.1476 | 2.1476 |
O2 | 1.4178 | | 2.8327 | 0.9498 | 3.5369 | O3 | 1.4178 | 2.8327 | | 3.5369 | 0.9498 | H4 | 2.1476 | 0.9498 | 3.5369 | | 4.0976 | H5 | 2.1476 | 3.5369 | 0.9498 | 4.0976 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Be1 |
O2 |
H4 |
129.134 |
|
Be1 |
O3 |
H5 |
129.134 |
O2 |
Be1 |
O3 |
174.767 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Be |
-0.117 |
|
|
|
2 |
O |
-0.257 |
|
|
|
3 |
O |
-0.257 |
|
|
|
4 |
H |
0.315 |
|
|
|
5 |
H |
0.315 |
|
|
|
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 |
-2.354 |
2.354 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.460 |
0.000 |
0.000 |
y |
0.000 |
-14.045 |
0.000 |
z |
0.000 |
0.000 |
-14.097 |
|
Traceless |
| x | y | z |
x |
-2.389 |
0.000 |
0.000 |
y |
0.000 |
1.234 |
0.000 |
z |
0.000 |
0.000 |
1.155 |
|
Polar |
3z2-r2 | 2.310 |
x2-y2 | -2.416 |
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 |
2.382 |
0.000 |
0.000 |
y |
0.000 |
3.581 |
0.000 |
z |
0.000 |
0.000 |
2.519 |
<r2> (average value of r
2) Å
2
<r2> |
50.671 |
(<r2>)1/2 |
7.118 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G(2df,p)
| hartrees |
Energy at 0K | -166.357780 |
Energy at 298.15K | -166.359309 |
HF Energy | -166.357780 |
Nuclear repulsion energy | 49.233038 |
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/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 |
4032 |
3862 |
30.01 |
|
|
|
2 |
A |
758 |
726 |
2.80 |
|
|
|
3 |
A |
583 |
559 |
75.94 |
|
|
|
4 |
A |
320 |
306 |
37.72 |
|
|
|
5 |
A |
222 |
213 |
112.67 |
|
|
|
6 |
B |
4031 |
3860 |
172.24 |
|
|
|
7 |
B |
1576 |
1510 |
317.36 |
|
|
|
8 |
B |
577 |
553 |
330.85 |
|
|
|
9 |
B |
315 |
301 |
73.88 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6207.0 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 5944.4 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 HSEh1PBE/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Be1 |
0.000 |
0.000 |
-0.015 |
O2 |
0.000 |
1.419 |
-0.053 |
O3 |
0.000 |
-1.419 |
-0.053 |
H4 |
0.555 |
2.001 |
0.455 |
H5 |
-0.555 |
-2.001 |
0.455 |
Atom - Atom Distances (Å)
|
Be1 |
O2 |
O3 |
H4 |
H5 |
Be1 | | 1.4194 | 1.4194 | 2.1289 | 2.1289 |
O2 | 1.4194 | | 2.8377 | 0.9510 | 3.5014 | O3 | 1.4194 | 2.8377 | | 3.5014 | 0.9510 | H4 | 2.1289 | 0.9510 | 3.5014 | | 4.1526 | H5 | 2.1289 | 3.5014 | 0.9510 | 4.1526 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Be1 |
O2 |
H4 |
126.693 |
|
Be1 |
O3 |
H5 |
126.693 |
O2 |
Be1 |
O3 |
176.962 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Be |
-0.108 |
|
|
|
2 |
O |
-0.261 |
|
|
|
3 |
O |
-0.261 |
|
|
|
4 |
H |
0.315 |
|
|
|
5 |
H |
0.315 |
|
|
|
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 |
1.658 |
1.658 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.805 |
4.300 |
0.000 |
y |
4.300 |
-14.878 |
0.000 |
z |
0.000 |
0.000 |
-15.266 |
|
Traceless |
| x | y | z |
x |
0.267 |
4.300 |
0.000 |
y |
4.300 |
0.158 |
0.000 |
z |
0.000 |
0.000 |
-0.424 |
|
Polar |
3z2-r2 | -0.849 |
x2-y2 | 0.073 |
xy | 4.300 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.479 |
0.156 |
0.000 |
y |
0.156 |
3.555 |
0.000 |
z |
0.000 |
0.000 |
2.467 |
<r2> (average value of r
2) Å
2
<r2> |
50.650 |
(<r2>)1/2 |
7.117 |