Jump to
S1C2
Energy calculated at LSDA/6-31G(2df,p)
| hartrees |
Energy at 0K | -165.668783 |
Energy at 298.15K | |
HF Energy | -165.668783 |
Nuclear repulsion energy | 49.372316 |
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 LSDA/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 |
3944 |
3881 |
61.89 |
|
|
|
2 |
A1 |
768 |
756 |
4.90 |
|
|
|
3 |
A1 |
534 |
526 |
145.20 |
|
|
|
4 |
A1 |
299 |
294 |
0.97 |
|
|
|
5 |
A2 |
229i |
225i |
0.00 |
|
|
|
6 |
B1 |
346 |
340 |
44.33 |
|
|
|
7 |
B2 |
3941 |
3877 |
199.66 |
|
|
|
8 |
B2 |
1603 |
1577 |
297.77 |
|
|
|
9 |
B2 |
413 |
406 |
283.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5809.1 cm
-1
Scaled (by 0.984) Zero Point Vibrational Energy (zpe) 5716.2 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 LSDA/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Be1 |
0.000 |
0.000 |
0.009 |
O2 |
0.000 |
1.407 |
0.075 |
O3 |
0.000 |
-1.407 |
0.075 |
H4 |
0.000 |
2.073 |
-0.615 |
H5 |
0.000 |
-2.073 |
-0.615 |
Atom - Atom Distances (Å)
|
Be1 |
O2 |
O3 |
H4 |
H5 |
Be1 | | 1.4087 | 1.4087 | 2.1654 | 2.1654 |
O2 | 1.4087 | | 2.8143 | 0.9592 | 3.5483 | O3 | 1.4087 | 2.8143 | | 3.5483 | 0.9592 | H4 | 2.1654 | 0.9592 | 3.5483 | | 4.1469 | H5 | 2.1654 | 3.5483 | 0.9592 | 4.1469 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Be1 |
O2 |
H4 |
131.325 |
|
Be1 |
O3 |
H5 |
131.325 |
O2 |
Be1 |
O3 |
174.648 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Be |
-0.312 |
|
|
|
2 |
O |
-0.171 |
|
|
|
3 |
O |
-0.171 |
|
|
|
4 |
H |
0.327 |
|
|
|
5 |
H |
0.327 |
|
|
|
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 |
-2.282 |
2.282 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.716 |
0.000 |
0.000 |
y |
0.000 |
-12.784 |
0.000 |
z |
0.000 |
0.000 |
-14.497 |
|
Traceless |
| x | y | z |
x |
-3.076 |
0.000 |
0.000 |
y |
0.000 |
2.822 |
0.000 |
z |
0.000 |
0.000 |
0.253 |
|
Polar |
3z2-r2 | 0.507 |
x2-y2 | -3.932 |
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 |
2.487 |
0.000 |
0.000 |
y |
0.000 |
3.865 |
0.000 |
z |
0.000 |
0.000 |
2.626 |
<r2> (average value of r
2) Å
2
<r2> |
50.285 |
(<r2>)1/2 |
7.091 |
Jump to
S1C1
Energy calculated at LSDA/6-31G(2df,p)
| hartrees |
Energy at 0K | -165.669631 |
Energy at 298.15K | -165.671103 |
HF Energy | -165.669631 |
Nuclear repulsion energy | 49.327473 |
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 LSDA/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 |
3920 |
3857 |
33.93 |
|
|
|
2 |
A |
763 |
750 |
1.87 |
|
|
|
3 |
A |
538 |
529 |
80.02 |
|
|
|
4 |
A |
312 |
307 |
22.75 |
|
|
|
5 |
A |
235 |
232 |
102.15 |
|
|
|
6 |
B |
3918 |
3855 |
202.29 |
|
|
|
7 |
B |
1598 |
1573 |
286.24 |
|
|
|
8 |
B |
528 |
519 |
315.96 |
|
|
|
9 |
B |
311 |
306 |
69.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6060.6 cm
-1
Scaled (by 0.984) Zero Point Vibrational Energy (zpe) 5963.7 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 LSDA/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Be1 |
0.000 |
0.000 |
-0.014 |
O2 |
0.000 |
1.411 |
-0.055 |
O3 |
0.000 |
-1.411 |
-0.055 |
H4 |
0.532 |
2.019 |
0.465 |
H5 |
-0.532 |
-2.019 |
0.465 |
Atom - Atom Distances (Å)
|
Be1 |
O2 |
O3 |
H4 |
H5 |
Be1 | | 1.4114 | 1.4114 | 2.1422 | 2.1422 |
O2 | 1.4114 | | 2.8216 | 0.9608 | 3.5094 | O3 | 1.4114 | 2.8216 | | 3.5094 | 0.9608 | H4 | 2.1422 | 0.9608 | 3.5094 | | 4.1757 | H5 | 2.1422 | 3.5094 | 0.9608 | 4.1757 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Be1 |
O2 |
H4 |
128.111 |
|
Be1 |
O3 |
H5 |
128.111 |
O2 |
Be1 |
O3 |
176.720 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Be |
-0.298 |
|
|
|
2 |
O |
-0.177 |
|
|
|
3 |
O |
-0.177 |
|
|
|
4 |
H |
0.326 |
|
|
|
5 |
H |
0.326 |
|
|
|
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 |
1.689 |
1.689 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-15.208 |
4.208 |
0.000 |
y |
4.208 |
-13.784 |
0.000 |
z |
0.000 |
0.000 |
-15.482 |
|
Traceless |
| x | y | z |
x |
-0.575 |
4.208 |
0.000 |
y |
4.208 |
1.561 |
0.000 |
z |
0.000 |
0.000 |
-0.986 |
|
Polar |
3z2-r2 | -1.971 |
x2-y2 | -1.424 |
xy | 4.208 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.585 |
0.158 |
0.000 |
y |
0.158 |
3.837 |
0.000 |
z |
0.000 |
0.000 |
2.584 |
<r2> (average value of r
2) Å
2
<r2> |
50.303 |
(<r2>)1/2 |
7.092 |