Jump to
S1C2
Energy calculated at B3PW91/cc-pVDZ
| hartrees |
Energy at 0K | -418.310207 |
Energy at 298.15K | -418.314302 |
HF Energy | -418.310207 |
Nuclear repulsion energy | 60.738368 |
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/cc-pVDZ
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' |
3805 |
3672 |
55.48 |
|
|
|
2 |
A' |
2297 |
2217 |
109.89 |
|
|
|
3 |
A' |
1127 |
1088 |
6.14 |
|
|
|
4 |
A' |
1099 |
1060 |
47.42 |
|
|
|
5 |
A' |
896 |
865 |
33.78 |
|
|
|
6 |
A' |
795 |
767 |
125.51 |
|
|
|
7 |
A" |
2306 |
2225 |
157.98 |
|
|
|
8 |
A" |
894 |
863 |
14.53 |
|
|
|
9 |
A" |
412 |
397 |
102.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6815.2 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 6576.7 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/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
-0.109 |
-0.576 |
0.000 |
O2 |
-0.109 |
1.110 |
0.000 |
H3 |
0.788 |
1.474 |
0.000 |
H4 |
0.861 |
-0.860 |
1.034 |
H5 |
0.861 |
-0.860 |
-1.034 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6854 | 2.2368 | 1.4461 | 1.4461 |
O2 | 1.6854 | | 0.9677 | 2.4267 | 2.4267 | H3 | 2.2368 | 0.9677 | | 2.5529 | 2.5529 | H4 | 1.4461 | 2.4267 | 2.5529 | | 2.0672 | H5 | 1.4461 | 2.4267 | 2.5529 | 2.0672 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
112.079 |
|
O2 |
P1 |
H4 |
101.324 |
O2 |
P1 |
H5 |
101.324 |
|
H4 |
P1 |
H5 |
91.248 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.239 |
|
|
|
2 |
O |
-0.382 |
|
|
|
3 |
H |
0.177 |
|
|
|
4 |
H |
-0.017 |
|
|
|
5 |
H |
-0.017 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.072 |
-0.036 |
0.000 |
2.073 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.838 |
1.573 |
0.000 |
y |
1.573 |
-19.469 |
0.000 |
z |
0.000 |
0.000 |
-19.867 |
|
Traceless |
| x | y | z |
x |
-0.170 |
1.573 |
0.000 |
y |
1.573 |
0.383 |
0.000 |
z |
0.000 |
0.000 |
-0.213 |
|
Polar |
3z2-r2 | -0.427 |
x2-y2 | -0.369 |
xy | 1.573 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.650 |
-0.348 |
0.000 |
y |
-0.348 |
3.839 |
0.000 |
z |
0.000 |
0.000 |
3.826 |
<r2> (average value of r
2) Å
2
<r2> |
35.307 |
(<r2>)1/2 |
5.942 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVDZ
| hartrees |
Energy at 0K | -418.310816 |
Energy at 298.15K | -418.314720 |
HF Energy | -418.310816 |
Nuclear repulsion energy | 60.635162 |
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/cc-pVDZ
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' |
3830 |
3696 |
94.28 |
|
|
|
2 |
A' |
2348 |
2265 |
89.35 |
|
|
|
3 |
A' |
1144 |
1104 |
90.02 |
|
|
|
4 |
A' |
1124 |
1085 |
18.85 |
|
|
|
5 |
A' |
898 |
866 |
14.36 |
|
|
|
6 |
A' |
790 |
762 |
94.01 |
|
|
|
7 |
A" |
2351 |
2269 |
124.01 |
|
|
|
8 |
A" |
916 |
884 |
1.34 |
|
|
|
9 |
A" |
238 |
230 |
81.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6819.4 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 6580.7 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/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
0.040 |
-0.582 |
0.000 |
O2 |
0.040 |
1.115 |
0.000 |
H3 |
0.967 |
1.389 |
0.000 |
H4 |
-0.940 |
-0.791 |
1.033 |
H5 |
-0.940 |
-0.791 |
-1.033 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6970 | 2.1778 | 1.4390 | 1.4390 |
O2 | 1.6970 | | 0.9666 | 2.3795 | 2.3795 | H3 | 2.1778 | 0.9666 | | 3.0750 | 3.0750 | H4 | 1.4390 | 2.3795 | 3.0750 | | 2.0668 | H5 | 1.4390 | 2.3795 | 3.0750 | 2.0668 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
106.447 |
|
O2 |
P1 |
H4 |
98.375 |
O2 |
P1 |
H5 |
98.375 |
|
H4 |
P1 |
H5 |
91.799 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.201 |
|
|
|
2 |
O |
-0.379 |
|
|
|
3 |
H |
0.176 |
|
|
|
4 |
H |
0.001 |
|
|
|
5 |
H |
0.001 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.771 |
-0.228 |
0.000 |
0.804 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.965 |
3.649 |
0.000 |
y |
3.649 |
-20.009 |
0.000 |
z |
0.000 |
0.000 |
-19.717 |
|
Traceless |
| x | y | z |
x |
0.898 |
3.649 |
0.000 |
y |
3.649 |
-0.668 |
0.000 |
z |
0.000 |
0.000 |
-0.230 |
|
Polar |
3z2-r2 | -0.459 |
x2-y2 | 1.044 |
xy | 3.649 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.805 |
0.700 |
0.000 |
y |
0.700 |
3.787 |
0.000 |
z |
0.000 |
0.000 |
3.805 |
<r2> (average value of r
2) Å
2
<r2> |
35.299 |
(<r2>)1/2 |
5.941 |