Jump to
S1C2
Energy calculated at B3LYP/6-31G**
| hartrees |
Energy at 0K | -418.370429 |
Energy at 298.15K | -418.374538 |
HF Energy | -418.370429 |
Nuclear repulsion energy | 61.200805 |
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 B3LYP/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' |
3815 |
3666 |
35.59 |
|
|
|
2 |
A' |
2306 |
2216 |
145.90 |
|
|
|
3 |
A' |
1162 |
1116 |
12.68 |
|
|
|
4 |
A' |
1125 |
1081 |
69.37 |
|
|
|
5 |
A' |
909 |
874 |
49.94 |
|
|
|
6 |
A' |
796 |
765 |
138.76 |
|
|
|
7 |
A" |
2312 |
2221 |
198.48 |
|
|
|
8 |
A" |
895 |
860 |
19.60 |
|
|
|
9 |
A" |
424 |
407 |
117.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6872.4 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 6603.0 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 B3LYP/6-31G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
-0.108 |
-0.570 |
0.000 |
O2 |
-0.108 |
1.099 |
0.000 |
H3 |
0.777 |
1.489 |
0.000 |
H4 |
0.849 |
-0.865 |
1.029 |
H5 |
0.849 |
-0.865 |
-1.029 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6691 | 2.2413 | 1.4355 | 1.4355 |
O2 | 1.6691 | | 0.9666 | 2.4151 | 2.4151 | H3 | 2.2413 | 0.9666 | | 2.5708 | 2.5708 | H4 | 1.4355 | 2.4151 | 2.5708 | | 2.0571 | H5 | 1.4355 | 2.4151 | 2.5708 | 2.0571 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
113.821 |
|
O2 |
P1 |
H4 |
101.877 |
O2 |
P1 |
H5 |
101.877 |
|
H4 |
P1 |
H5 |
91.539 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.410 |
|
|
|
2 |
O |
-0.610 |
|
|
|
3 |
H |
0.324 |
|
|
|
4 |
H |
-0.062 |
|
|
|
5 |
H |
-0.062 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.264 |
0.025 |
0.000 |
2.264 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.141 |
1.548 |
0.000 |
y |
1.548 |
-19.410 |
0.000 |
z |
0.000 |
0.000 |
-19.903 |
|
Traceless |
| x | y | z |
x |
-0.485 |
1.548 |
0.000 |
y |
1.548 |
0.611 |
0.000 |
z |
0.000 |
0.000 |
-0.127 |
|
Polar |
3z2-r2 | -0.253 |
x2-y2 | -0.731 |
xy | 1.548 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.290 |
-0.281 |
0.000 |
y |
-0.281 |
3.706 |
0.000 |
z |
0.000 |
0.000 |
3.511 |
<r2> (average value of r
2) Å
2
<r2> |
35.060 |
(<r2>)1/2 |
5.921 |
Jump to
S1C1
Energy calculated at B3LYP/6-31G**
| hartrees |
Energy at 0K | -418.371584 |
Energy at 298.15K | -418.375513 |
HF Energy | -418.371584 |
Nuclear repulsion energy | 61.097510 |
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 B3LYP/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' |
3850 |
3699 |
76.78 |
|
|
|
2 |
A' |
2367 |
2274 |
116.66 |
|
|
|
3 |
A' |
1163 |
1117 |
43.91 |
|
|
|
4 |
A' |
1159 |
1113 |
117.18 |
|
|
|
5 |
A' |
918 |
882 |
20.29 |
|
|
|
6 |
A' |
789 |
758 |
105.18 |
|
|
|
7 |
A" |
2367 |
2274 |
150.64 |
|
|
|
8 |
A" |
925 |
888 |
1.50 |
|
|
|
9 |
A" |
253 |
243 |
95.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6894.5 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 6624.2 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 B3LYP/6-31G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
0.039 |
-0.576 |
0.000 |
O2 |
0.039 |
1.105 |
0.000 |
H3 |
0.957 |
1.402 |
0.000 |
H4 |
-0.926 |
-0.799 |
1.028 |
H5 |
-0.926 |
-0.799 |
-1.028 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6811 | 2.1808 | 1.4272 | 1.4272 |
O2 | 1.6811 | | 0.9651 | 2.3693 | 2.3693 | H3 | 2.1808 | 0.9651 | | 3.0737 | 3.0737 | H4 | 1.4272 | 2.3693 | 3.0737 | | 2.0555 | H5 | 1.4272 | 2.3693 | 3.0737 | 2.0555 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
107.914 |
|
O2 |
P1 |
H4 |
98.998 |
O2 |
P1 |
H5 |
98.998 |
|
H4 |
P1 |
H5 |
92.127 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.370 |
|
|
|
2 |
O |
-0.611 |
|
|
|
3 |
H |
0.328 |
|
|
|
4 |
H |
-0.043 |
|
|
|
5 |
H |
-0.043 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.747 |
-0.151 |
0.000 |
0.762 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.201 |
3.915 |
0.000 |
y |
3.915 |
-20.053 |
0.000 |
z |
0.000 |
0.000 |
-19.790 |
|
Traceless |
| x | y | z |
x |
0.720 |
3.915 |
0.000 |
y |
3.915 |
-0.557 |
0.000 |
z |
0.000 |
0.000 |
-0.163 |
|
Polar |
3z2-r2 | -0.326 |
x2-y2 | 0.851 |
xy | 3.915 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.434 |
0.690 |
0.000 |
y |
0.690 |
3.680 |
0.000 |
z |
0.000 |
0.000 |
3.524 |
<r2> (average value of r
2) Å
2
<r2> |
35.061 |
(<r2>)1/2 |
5.921 |