Jump to
S1C2
Energy calculated at B2PLYP/6-31G(2df,p)
| hartrees |
Energy at 0K | -166.409889 |
Energy at 298.15K | |
HF Energy | -166.249291 |
Nuclear repulsion energy | 49.168928 |
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/6-31G(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 |
4022 |
3841 |
55.61 |
|
|
|
2 |
A1 |
760 |
726 |
8.62 |
|
|
|
3 |
A1 |
589 |
563 |
143.11 |
|
|
|
4 |
A1 |
305 |
291 |
7.30 |
|
|
|
5 |
A2 |
231i |
220i |
0.00 |
|
|
|
6 |
B1 |
350 |
335 |
56.67 |
|
|
|
7 |
B2 |
4019 |
3838 |
162.78 |
|
|
|
8 |
B2 |
1574 |
1503 |
313.77 |
|
|
|
9 |
B2 |
473 |
452 |
294.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5930.9 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 5664.0 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/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Be1 |
0.000 |
0.000 |
0.006 |
O2 |
0.000 |
1.419 |
0.078 |
O3 |
0.000 |
-1.419 |
0.078 |
H4 |
0.000 |
2.050 |
-0.634 |
H5 |
0.000 |
-2.050 |
-0.634 |
Atom - Atom Distances (Å)
|
Be1 |
O2 |
O3 |
H4 |
H5 |
Be1 | | 1.4205 | 1.4205 | 2.1475 | 2.1475 |
O2 | 1.4205 | | 2.8375 | 0.9513 | 3.5408 | O3 | 1.4205 | 2.8375 | | 3.5408 | 0.9513 | H4 | 2.1475 | 0.9513 | 3.5408 | | 4.0996 | H5 | 2.1475 | 3.5408 | 0.9513 | 4.0996 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Be1 |
O2 |
H4 |
128.683 |
|
Be1 |
O3 |
H5 |
128.683 |
O2 |
Be1 |
O3 |
174.251 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Be |
-0.100 |
|
|
|
2 |
O |
-0.264 |
|
|
|
3 |
O |
-0.264 |
|
|
|
4 |
H |
0.314 |
|
|
|
5 |
H |
0.314 |
|
|
|
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 |
-2.399 |
2.399 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.577 |
0.000 |
0.000 |
y |
0.000 |
-14.219 |
0.000 |
z |
0.000 |
0.000 |
-14.204 |
|
Traceless |
| x | y | z |
x |
-2.365 |
0.000 |
0.000 |
y |
0.000 |
1.172 |
0.000 |
z |
0.000 |
0.000 |
1.194 |
|
Polar |
3z2-r2 | 2.387 |
x2-y2 | -2.358 |
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 |
2.367 |
0.000 |
0.000 |
y |
0.000 |
3.627 |
0.000 |
z |
0.000 |
0.000 |
2.517 |
<r2> (average value of r
2) Å
2
<r2> |
50.879 |
(<r2>)1/2 |
7.133 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31G(2df,p)
| hartrees |
Energy at 0K | -166.410861 |
Energy at 298.15K | -166.412399 |
HF Energy | -166.250097 |
Nuclear repulsion energy | 49.140996 |
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/6-31G(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 |
4003 |
3822 |
27.55 |
|
|
|
2 |
A |
755 |
721 |
2.80 |
|
|
|
3 |
A |
586 |
559 |
72.17 |
|
|
|
4 |
A |
319 |
304 |
36.39 |
|
|
|
5 |
A |
229 |
219 |
117.88 |
|
|
|
6 |
B |
4001 |
3821 |
174.33 |
|
|
|
7 |
B |
1572 |
1502 |
305.80 |
|
|
|
8 |
B |
580 |
554 |
332.50 |
|
|
|
9 |
B |
313 |
299 |
73.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6178.5 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 5900.5 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 B2PLYP/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Be1 |
0.000 |
0.000 |
-0.012 |
O2 |
0.000 |
1.422 |
-0.054 |
O3 |
0.000 |
-1.422 |
-0.054 |
H4 |
0.562 |
2.000 |
0.454 |
H5 |
-0.562 |
-2.000 |
0.454 |
Atom - Atom Distances (Å)
|
Be1 |
O2 |
O3 |
H4 |
H5 |
Be1 | | 1.4224 | 1.4224 | 2.1287 | 2.1287 |
O2 | 1.4224 | | 2.8436 | 0.9525 | 3.5044 | O3 | 1.4224 | 2.8436 | | 3.5044 | 0.9525 | H4 | 2.1287 | 0.9525 | 3.5044 | | 4.1545 | H5 | 2.1287 | 3.5044 | 0.9525 | 4.1545 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Be1 |
O2 |
H4 |
126.217 |
|
Be1 |
O3 |
H5 |
126.217 |
O2 |
Be1 |
O3 |
176.614 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Be |
-0.090 |
|
|
|
2 |
O |
-0.268 |
|
|
|
3 |
O |
-0.268 |
|
|
|
4 |
H |
0.313 |
|
|
|
5 |
H |
0.313 |
|
|
|
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 |
1.680 |
1.680 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.884 |
4.350 |
0.000 |
y |
4.350 |
-15.094 |
0.000 |
z |
0.000 |
0.000 |
-15.392 |
|
Traceless |
| x | y | z |
x |
0.359 |
4.350 |
0.000 |
y |
4.350 |
0.045 |
0.000 |
z |
0.000 |
0.000 |
-0.403 |
|
Polar |
3z2-r2 | -0.807 |
x2-y2 | 0.209 |
xy | 4.350 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.474 |
0.160 |
0.000 |
y |
0.160 |
3.598 |
0.000 |
z |
0.000 |
0.000 |
2.459 |
<r2> (average value of r
2) Å
2
<r2> |
50.878 |
(<r2>)1/2 |
7.133 |