Jump to
S1C2
Energy calculated at B3PW91/6-31G**
| hartrees |
Energy at 0K | -418.291090 |
Energy at 298.15K | -418.295207 |
HF Energy | -418.291090 |
Nuclear repulsion energy | 61.359725 |
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 B3PW91/6-31G**
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' |
3857 |
3696 |
44.48 |
|
|
|
2 |
A' |
2324 |
2228 |
141.92 |
|
|
|
3 |
A' |
1158 |
1110 |
9.14 |
|
|
|
4 |
A' |
1121 |
1074 |
72.31 |
|
|
|
5 |
A' |
912 |
874 |
45.10 |
|
|
|
6 |
A' |
809 |
776 |
144.96 |
|
|
|
7 |
A" |
2332 |
2235 |
194.58 |
|
|
|
8 |
A" |
899 |
862 |
19.92 |
|
|
|
9 |
A" |
427 |
409 |
120.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6919.7 cm
-1
Scaled (by 0.9584) Zero Point Vibrational Energy (zpe) 6631.8 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 B3PW91/6-31G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
-0.108 |
-0.568 |
0.000 |
O2 |
-0.108 |
1.096 |
0.000 |
H3 |
0.776 |
1.483 |
0.000 |
H4 |
0.849 |
-0.862 |
1.027 |
H5 |
0.849 |
-0.862 |
-1.027 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6640 | 2.2333 | 1.4343 | 1.4343 |
O2 | 1.6640 | | 0.9643 | 2.4092 | 2.4092 | H3 | 2.2333 | 0.9643 | | 2.5614 | 2.5614 | H4 | 1.4343 | 2.4092 | 2.5614 | | 2.0549 | H5 | 1.4343 | 2.4092 | 2.5614 | 2.0549 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
113.678 |
|
O2 |
P1 |
H4 |
101.822 |
O2 |
P1 |
H5 |
101.822 |
|
H4 |
P1 |
H5 |
91.504 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.389 |
|
|
|
2 |
O |
-0.620 |
|
|
|
3 |
H |
0.338 |
|
|
|
4 |
H |
-0.053 |
|
|
|
5 |
H |
-0.053 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.318 |
0.068 |
0.000 |
2.319 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.047 |
1.542 |
0.000 |
y |
1.542 |
-19.354 |
0.000 |
z |
0.000 |
0.000 |
-19.839 |
|
Traceless |
| x | y | z |
x |
-0.451 |
1.542 |
0.000 |
y |
1.542 |
0.590 |
0.000 |
z |
0.000 |
0.000 |
-0.138 |
|
Polar |
3z2-r2 | -0.277 |
x2-y2 | -0.694 |
xy | 1.542 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.294 |
-0.298 |
0.000 |
y |
-0.298 |
3.678 |
0.000 |
z |
0.000 |
0.000 |
3.528 |
<r2> (average value of r
2) Å
2
<r2> |
34.889 |
(<r2>)1/2 |
5.907 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G**
| hartrees |
Energy at 0K | -418.292354 |
Energy at 298.15K | -418.296299 |
HF Energy | -418.292354 |
Nuclear repulsion energy | 61.270700 |
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 B3PW91/6-31G**
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' |
3887 |
3726 |
87.92 |
|
|
|
2 |
A' |
2383 |
2284 |
113.27 |
|
|
|
3 |
A' |
1161 |
1112 |
106.31 |
|
|
|
4 |
A' |
1154 |
1106 |
53.87 |
|
|
|
5 |
A' |
915 |
877 |
22.81 |
|
|
|
6 |
A' |
804 |
771 |
106.33 |
|
|
|
7 |
A" |
2386 |
2287 |
147.65 |
|
|
|
8 |
A" |
927 |
889 |
1.72 |
|
|
|
9 |
A" |
262 |
251 |
98.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6939.6 cm
-1
Scaled (by 0.9584) Zero Point Vibrational Energy (zpe) 6650.9 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 B3PW91/6-31G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
0.039 |
-0.574 |
0.000 |
O2 |
0.039 |
1.101 |
0.000 |
H3 |
0.956 |
1.397 |
0.000 |
H4 |
-0.925 |
-0.798 |
1.027 |
H5 |
-0.925 |
-0.798 |
-1.027 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6750 | 2.1733 | 1.4265 | 1.4265 |
O2 | 1.6750 | | 0.9631 | 2.3647 | 2.3647 | H3 | 2.1733 | 0.9631 | | 3.0675 | 3.0675 | H4 | 1.4265 | 2.3647 | 3.0675 | | 2.0539 | H5 | 1.4265 | 2.3647 | 3.0675 | 2.0539 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
107.863 |
|
O2 |
P1 |
H4 |
99.042 |
O2 |
P1 |
H5 |
99.042 |
|
H4 |
P1 |
H5 |
92.094 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.351 |
|
|
|
2 |
O |
-0.622 |
|
|
|
3 |
H |
0.342 |
|
|
|
4 |
H |
-0.036 |
|
|
|
5 |
H |
-0.036 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.731 |
-0.103 |
0.000 |
0.738 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.099 |
3.983 |
0.000 |
y |
3.983 |
-19.989 |
0.000 |
z |
0.000 |
0.000 |
-19.732 |
|
Traceless |
| x | y | z |
x |
0.761 |
3.983 |
0.000 |
y |
3.983 |
-0.573 |
0.000 |
z |
0.000 |
0.000 |
-0.188 |
|
Polar |
3z2-r2 | -0.376 |
x2-y2 | 0.890 |
xy | 3.983 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.436 |
0.679 |
0.000 |
y |
0.679 |
3.657 |
0.000 |
z |
0.000 |
0.000 |
3.545 |
<r2> (average value of r
2) Å
2
<r2> |
34.881 |
(<r2>)1/2 |
5.906 |