Jump to
S1C2
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -418.347407 |
Energy at 298.15K | -418.351541 |
HF Energy | -418.347407 |
Nuclear repulsion energy | 61.574793 |
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 B1B95/6-31G*
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' |
3819 |
3625 |
45.77 |
|
|
|
2 |
A' |
2358 |
2238 |
144.95 |
|
|
|
3 |
A' |
1181 |
1121 |
12.99 |
|
|
|
4 |
A' |
1135 |
1078 |
71.52 |
|
|
|
5 |
A' |
918 |
872 |
47.38 |
|
|
|
6 |
A' |
823 |
781 |
149.17 |
|
|
|
7 |
A" |
2363 |
2243 |
202.17 |
|
|
|
8 |
A" |
906 |
860 |
21.74 |
|
|
|
9 |
A" |
440 |
418 |
124.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6970.8 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 6617.3 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
-0.107 |
-0.567 |
0.000 |
O2 |
-0.107 |
1.091 |
0.000 |
H3 |
0.776 |
1.480 |
0.000 |
H4 |
0.847 |
-0.853 |
1.024 |
H5 |
0.847 |
-0.853 |
-1.024 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6578 | 2.2292 | 1.4284 | 1.4284 |
O2 | 1.6578 | | 0.9651 | 2.3951 | 2.3951 | H3 | 2.2292 | 0.9651 | | 2.5486 | 2.5486 | H4 | 1.4284 | 2.3951 | 2.5486 | | 2.0481 | H5 | 1.4284 | 2.3951 | 2.5486 | 2.0481 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
113.771 |
|
O2 |
P1 |
H4 |
101.547 |
O2 |
P1 |
H5 |
101.547 |
|
H4 |
P1 |
H5 |
91.598 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.323 |
|
|
|
2 |
O |
-0.707 |
|
|
|
3 |
H |
0.428 |
|
|
|
4 |
H |
-0.022 |
|
|
|
5 |
H |
-0.022 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.324 |
0.052 |
0.000 |
2.325 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.024 |
1.588 |
0.000 |
y |
1.588 |
-19.338 |
0.000 |
z |
0.000 |
0.000 |
-19.849 |
|
Traceless |
| x | y | z |
x |
-0.430 |
1.588 |
0.000 |
y |
1.588 |
0.599 |
0.000 |
z |
0.000 |
0.000 |
-0.168 |
|
Polar |
3z2-r2 | -0.336 |
x2-y2 | -0.686 |
xy | 1.588 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.216 |
-0.290 |
0.000 |
y |
-0.290 |
3.561 |
0.000 |
z |
0.000 |
0.000 |
3.446 |
<r2> (average value of r
2) Å
2
<r2> |
34.711 |
(<r2>)1/2 |
5.892 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| hartrees |
Energy at 0K | -418.348523 |
Energy at 298.15K | -418.352484 |
HF Energy | -418.348523 |
Nuclear repulsion energy | 61.486600 |
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 B1B95/6-31G*
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' |
3849 |
3654 |
89.41 |
|
|
|
2 |
A' |
2425 |
2302 |
115.79 |
|
|
|
3 |
A' |
1182 |
1122 |
92.04 |
|
|
|
4 |
A' |
1175 |
1115 |
80.02 |
|
|
|
5 |
A' |
927 |
880 |
23.58 |
|
|
|
6 |
A' |
819 |
777 |
106.63 |
|
|
|
7 |
A" |
2426 |
2303 |
152.76 |
|
|
|
8 |
A" |
940 |
892 |
1.98 |
|
|
|
9 |
A" |
268 |
254 |
102.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7005.0 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 6649.9 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
0.039 |
-0.572 |
0.000 |
O2 |
0.039 |
1.096 |
0.000 |
H3 |
0.955 |
1.396 |
0.000 |
H4 |
-0.923 |
-0.789 |
1.023 |
H5 |
-0.923 |
-0.789 |
-1.023 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6685 | 2.1712 | 1.4208 | 1.4208 |
O2 | 1.6685 | | 0.9637 | 2.3508 | 2.3508 | H3 | 2.1712 | 0.9637 | | 3.0574 | 3.0574 | H4 | 1.4208 | 2.3508 | 3.0574 | | 2.0466 | H5 | 1.4208 | 2.3508 | 3.0574 | 2.0466 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
108.143 |
|
O2 |
P1 |
H4 |
98.776 |
O2 |
P1 |
H5 |
98.776 |
|
H4 |
P1 |
H5 |
92.147 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.287 |
|
|
|
2 |
O |
-0.708 |
|
|
|
3 |
H |
0.431 |
|
|
|
4 |
H |
-0.005 |
|
|
|
5 |
H |
-0.005 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.778 |
-0.123 |
0.000 |
0.788 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.078 |
4.019 |
0.000 |
y |
4.019 |
-19.961 |
0.000 |
z |
0.000 |
0.000 |
-19.742 |
|
Traceless |
| x | y | z |
x |
0.774 |
4.019 |
0.000 |
y |
4.019 |
-0.551 |
0.000 |
z |
0.000 |
0.000 |
-0.223 |
|
Polar |
3z2-r2 | -0.445 |
x2-y2 | 0.884 |
xy | 4.019 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.358 |
0.663 |
0.000 |
y |
0.663 |
3.548 |
0.000 |
z |
0.000 |
0.000 |
3.465 |
<r2> (average value of r
2) Å
2
<r2> |
34.703 |
(<r2>)1/2 |
5.891 |