Jump to
S1C2
Energy calculated at B2PLYP/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -166.480101 |
Energy at 298.15K | |
HF Energy | -166.306695 |
Nuclear repulsion energy | 49.035721 |
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 B2PLYP/6-311+G(3df,2p)
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 |
4032 |
4032 |
50.06 |
|
|
|
2 |
A1 |
749 |
749 |
4.31 |
|
|
|
3 |
A1 |
535 |
535 |
190.16 |
|
|
|
4 |
A1 |
295 |
295 |
8.32 |
|
|
|
5 |
A2 |
190i |
190i |
0.00 |
|
|
|
6 |
B1 |
336 |
336 |
51.67 |
|
|
|
7 |
B2 |
4030 |
4030 |
198.32 |
|
|
|
8 |
B2 |
1535 |
1535 |
423.41 |
|
|
|
9 |
B2 |
440 |
440 |
264.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5881.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5881.0 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 B2PLYP/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Be1 |
0.000 |
0.000 |
-0.015 |
O2 |
0.000 |
1.421 |
0.075 |
O3 |
0.000 |
-1.421 |
0.075 |
H4 |
0.000 |
2.118 |
-0.570 |
H5 |
0.000 |
-2.118 |
-0.570 |
Atom - Atom Distances (Å)
|
Be1 |
O2 |
O3 |
H4 |
H5 |
Be1 | | 1.4234 | 1.4234 | 2.1898 | 2.1898 |
O2 | 1.4234 | | 2.8410 | 0.9503 | 3.5972 | O3 | 1.4234 | 2.8410 | | 3.5972 | 0.9503 | H4 | 2.1898 | 0.9503 | 3.5972 | | 4.2367 | H5 | 2.1898 | 3.5972 | 0.9503 | 4.2367 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Be1 |
O2 |
H4 |
133.611 |
|
Be1 |
O3 |
H5 |
133.611 |
O2 |
Be1 |
O3 |
172.723 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Be |
-0.047 |
|
|
|
2 |
O |
-0.184 |
|
|
|
3 |
O |
-0.184 |
|
|
|
4 |
H |
0.207 |
|
|
|
5 |
H |
0.207 |
|
|
|
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 |
-2.321 |
2.321 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-17.225 |
0.000 |
0.000 |
y |
0.000 |
-14.717 |
0.000 |
z |
0.000 |
0.000 |
-15.178 |
|
Traceless |
| x | y | z |
x |
-2.277 |
0.000 |
0.000 |
y |
0.000 |
1.485 |
0.000 |
z |
0.000 |
0.000 |
0.792 |
|
Polar |
3z2-r2 | 1.585 |
x2-y2 | -2.508 |
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 |
3.023 |
0.000 |
0.000 |
y |
0.000 |
4.163 |
0.000 |
z |
0.000 |
0.000 |
3.050 |
<r2> (average value of r
2) Å
2
<r2> |
51.812 |
(<r2>)1/2 |
7.198 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -166.480711 |
Energy at 298.15K | -166.482080 |
HF Energy | -166.307285 |
Nuclear repulsion energy | 49.010851 |
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 B2PLYP/6-311+G(3df,2p)
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 |
4019 |
4019 |
23.63 |
|
|
|
2 |
A |
746 |
746 |
1.39 |
|
|
|
3 |
A |
526 |
526 |
90.79 |
|
|
|
4 |
A |
308 |
308 |
29.26 |
|
|
|
5 |
A |
185 |
185 |
144.30 |
|
|
|
6 |
B |
4017 |
4017 |
209.98 |
|
|
|
7 |
B |
1535 |
1535 |
416.25 |
|
|
|
8 |
B |
519 |
519 |
342.23 |
|
|
|
9 |
B |
301 |
301 |
64.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6077.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6077.6 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 B2PLYP/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Be1 |
0.000 |
0.000 |
0.006 |
O2 |
0.000 |
1.424 |
-0.051 |
O3 |
0.000 |
-1.424 |
-0.051 |
H4 |
0.531 |
2.072 |
0.399 |
H5 |
-0.531 |
-2.072 |
0.399 |
Atom - Atom Distances (Å)
|
Be1 |
O2 |
O3 |
H4 |
H5 |
Be1 | | 1.4248 | 1.4248 | 2.1747 | 2.1747 |
O2 | 1.4248 | | 2.8473 | 0.9512 | 3.5645 | O3 | 1.4248 | 2.8473 | | 3.5645 | 0.9512 | H4 | 2.1747 | 0.9512 | 3.5645 | | 4.2782 | H5 | 2.1747 | 3.5645 | 0.9512 | 4.2782 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Be1 |
O2 |
H4 |
131.460 |
|
Be1 |
O3 |
H5 |
131.460 |
O2 |
Be1 |
O3 |
175.347 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Be |
-0.054 |
|
|
|
2 |
O |
-0.182 |
|
|
|
3 |
O |
-0.182 |
|
|
|
4 |
H |
0.209 |
|
|
|
5 |
H |
0.209 |
|
|
|
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 |
1.598 |
1.598 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-15.617 |
4.433 |
0.000 |
y |
4.433 |
-15.605 |
0.000 |
z |
0.000 |
0.000 |
-16.238 |
|
Traceless |
| x | y | z |
x |
0.304 |
4.433 |
0.000 |
y |
4.433 |
0.323 |
0.000 |
z |
0.000 |
0.000 |
-0.627 |
|
Polar |
3z2-r2 | -1.253 |
x2-y2 | -0.013 |
xy | 4.433 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.040 |
0.037 |
0.000 |
y |
0.037 |
4.151 |
0.000 |
z |
0.000 |
0.000 |
3.043 |
<r2> (average value of r
2) Å
2
<r2> |
51.822 |
(<r2>)1/2 |
7.199 |