Jump to
S1C2
Energy calculated at B3PW91/6-311G**
| hartrees |
Energy at 0K | -418.339235 |
Energy at 298.15K | -418.343357 |
HF Energy | -418.339235 |
Nuclear repulsion energy | 61.438990 |
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 B3PW91/6-311G**
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' |
3860 |
3718 |
58.25 |
|
|
|
2 |
A' |
2316 |
2231 |
124.27 |
|
|
|
3 |
A' |
1144 |
1102 |
17.35 |
|
|
|
4 |
A' |
1097 |
1057 |
67.21 |
|
|
|
5 |
A' |
905 |
871 |
39.48 |
|
|
|
6 |
A' |
796 |
767 |
157.10 |
|
|
|
7 |
A" |
2320 |
2235 |
166.00 |
|
|
|
8 |
A" |
909 |
876 |
24.48 |
|
|
|
9 |
A" |
432 |
416 |
128.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6890.0 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 6635.7 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 B3PW91/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
-0.107 |
-0.568 |
0.000 |
O2 |
-0.107 |
1.093 |
0.000 |
H3 |
0.765 |
1.496 |
0.000 |
H4 |
0.851 |
-0.860 |
1.027 |
H5 |
0.851 |
-0.860 |
-1.027 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6608 | 2.2409 | 1.4345 | 1.4345 |
O2 | 1.6608 | | 0.9607 | 2.4056 | 2.4056 | H3 | 2.2409 | 0.9607 | | 2.5721 | 2.5721 | H4 | 1.4345 | 2.4056 | 2.5721 | | 2.0544 | H5 | 1.4345 | 2.4056 | 2.5721 | 2.0544 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
114.834 |
|
O2 |
P1 |
H4 |
101.753 |
O2 |
P1 |
H5 |
101.753 |
|
H4 |
P1 |
H5 |
91.461 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.385 |
|
|
|
2 |
O |
-0.579 |
|
|
|
3 |
H |
0.289 |
|
|
|
4 |
H |
-0.047 |
|
|
|
5 |
H |
-0.047 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.254 |
0.016 |
0.000 |
2.254 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.507 |
1.722 |
0.000 |
y |
1.722 |
-19.708 |
0.000 |
z |
0.000 |
0.000 |
-20.160 |
|
Traceless |
| x | y | z |
x |
-0.573 |
1.722 |
0.000 |
y |
1.722 |
0.626 |
0.000 |
z |
0.000 |
0.000 |
-0.052 |
|
Polar |
3z2-r2 | -0.105 |
x2-y2 | -0.799 |
xy | 1.722 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.774 |
-0.306 |
0.000 |
y |
-0.306 |
3.817 |
0.000 |
z |
0.000 |
0.000 |
3.854 |
<r2> (average value of r
2) Å
2
<r2> |
35.088 |
(<r2>)1/2 |
5.924 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G**
| hartrees |
Energy at 0K | -418.339403 |
Energy at 298.15K | -418.343341 |
HF Energy | -418.339403 |
Nuclear repulsion energy | 61.297123 |
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 B3PW91/6-311G**
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' |
3892 |
3748 |
98.59 |
|
|
|
2 |
A' |
2373 |
2285 |
97.57 |
|
|
|
3 |
A' |
1145 |
1102 |
48.95 |
|
|
|
4 |
A' |
1129 |
1088 |
88.67 |
|
|
|
5 |
A' |
908 |
874 |
23.98 |
|
|
|
6 |
A' |
788 |
758 |
111.65 |
|
|
|
7 |
A" |
2372 |
2284 |
121.95 |
|
|
|
8 |
A" |
933 |
899 |
2.10 |
|
|
|
9 |
A" |
258 |
248 |
104.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6898.4 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 6643.9 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 B3PW91/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
0.039 |
-0.574 |
0.000 |
O2 |
0.039 |
1.100 |
0.000 |
H3 |
0.949 |
1.405 |
0.000 |
H4 |
-0.927 |
-0.794 |
1.026 |
H5 |
-0.927 |
-0.794 |
-1.026 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6744 | 2.1786 | 1.4267 | 1.4267 |
O2 | 1.6744 | | 0.9595 | 2.3613 | 2.3613 | H3 | 2.1786 | 0.9595 | | 3.0676 | 3.0676 | H4 | 1.4267 | 2.3613 | 3.0676 | | 2.0530 | H5 | 1.4267 | 2.3613 | 3.0676 | 2.0530 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
108.548 |
|
O2 |
P1 |
H4 |
98.868 |
O2 |
P1 |
H5 |
98.868 |
|
H4 |
P1 |
H5 |
92.021 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.340 |
|
|
|
2 |
O |
-0.577 |
|
|
|
3 |
H |
0.283 |
|
|
|
4 |
H |
-0.023 |
|
|
|
5 |
H |
-0.023 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.848 |
-0.265 |
0.000 |
0.889 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.484 |
3.946 |
0.000 |
y |
3.946 |
-20.281 |
0.000 |
z |
0.000 |
0.000 |
-20.006 |
|
Traceless |
| x | y | z |
x |
0.659 |
3.946 |
0.000 |
y |
3.946 |
-0.536 |
0.000 |
z |
0.000 |
0.000 |
-0.123 |
|
Polar |
3z2-r2 | -0.247 |
x2-y2 | 0.797 |
xy | 3.946 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.888 |
0.670 |
0.000 |
y |
0.670 |
3.742 |
0.000 |
z |
0.000 |
0.000 |
3.871 |
<r2> (average value of r
2) Å
2
<r2> |
35.070 |
(<r2>)1/2 |
5.922 |