Jump to
S1C2
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -418.372060 |
Energy at 298.15K | -418.376143 |
HF Energy | -418.372060 |
Nuclear repulsion energy | 60.596478 |
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 BLYP/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' |
3617 |
3608 |
14.79 |
|
|
|
2 |
A' |
2168 |
2162 |
165.36 |
|
|
|
3 |
A' |
1142 |
1139 |
18.77 |
|
|
|
4 |
A' |
1105 |
1103 |
75.71 |
|
|
|
5 |
A' |
884 |
882 |
55.38 |
|
|
|
6 |
A' |
738 |
736 |
131.07 |
|
|
|
7 |
A" |
2172 |
2166 |
203.08 |
|
|
|
8 |
A" |
867 |
865 |
21.30 |
|
|
|
9 |
A" |
438 |
436 |
142.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6564.4 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 6548.0 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
-0.108 |
-0.576 |
0.000 |
O2 |
-0.108 |
1.108 |
0.000 |
H3 |
0.768 |
1.534 |
0.000 |
H4 |
0.863 |
-0.880 |
1.034 |
H5 |
0.863 |
-0.880 |
-1.034 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6839 | 2.2852 | 1.4506 | 1.4506 |
O2 | 1.6839 | | 0.9750 | 2.4419 | 2.4419 | H3 | 2.2852 | 0.9750 | | 2.6279 | 2.6279 | H4 | 1.4506 | 2.4419 | 2.6279 | | 2.0681 | H5 | 1.4506 | 2.4419 | 2.6279 | 2.0681 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
115.930 |
|
O2 |
P1 |
H4 |
102.089 |
O2 |
P1 |
H5 |
102.089 |
|
H4 |
P1 |
H5 |
90.933 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.281 |
|
|
|
2 |
O |
-0.686 |
|
|
|
3 |
H |
0.401 |
|
|
|
4 |
H |
0.002 |
|
|
|
5 |
H |
0.002 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.240 |
0.067 |
0.000 |
2.241 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.983 |
1.949 |
0.000 |
y |
1.949 |
-19.874 |
0.000 |
z |
0.000 |
0.000 |
-20.674 |
|
Traceless |
| x | y | z |
x |
-0.708 |
1.949 |
0.000 |
y |
1.949 |
0.954 |
0.000 |
z |
0.000 |
0.000 |
-0.246 |
|
Polar |
3z2-r2 | -0.491 |
x2-y2 | -1.108 |
xy | 1.949 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.898 |
-0.322 |
0.000 |
y |
-0.322 |
3.976 |
0.000 |
z |
0.000 |
0.000 |
3.895 |
<r2> (average value of r
2) Å
2
<r2> |
35.996 |
(<r2>)1/2 |
6.000 |
Jump to
S1C1
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -418.372176 |
Energy at 298.15K | -418.376040 |
HF Energy | -418.372176 |
Nuclear repulsion energy | 60.362450 |
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 BLYP/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' |
3668 |
3659 |
50.25 |
|
|
|
2 |
A' |
2240 |
2234 |
128.31 |
|
|
|
3 |
A' |
1142 |
1139 |
52.48 |
|
|
|
4 |
A' |
1139 |
1136 |
101.10 |
|
|
|
5 |
A' |
893 |
890 |
15.22 |
|
|
|
6 |
A' |
721 |
719 |
99.39 |
|
|
|
7 |
A" |
2237 |
2232 |
150.34 |
|
|
|
8 |
A" |
903 |
901 |
0.18 |
|
|
|
9 |
A" |
234 |
234 |
107.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6588.3 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 6571.8 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
0.040 |
-0.586 |
0.000 |
O2 |
0.040 |
1.118 |
0.000 |
H3 |
0.959 |
1.439 |
0.000 |
H4 |
-0.940 |
-0.799 |
1.033 |
H5 |
-0.940 |
-0.799 |
-1.033 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.7037 | 2.2229 | 1.4400 | 1.4400 |
O2 | 1.7037 | | 0.9728 | 2.3880 | 2.3880 | H3 | 2.2229 | 0.9728 | | 3.1110 | 3.1110 | H4 | 1.4400 | 2.3880 | 3.1110 | | 2.0665 | H5 | 1.4400 | 2.3880 | 3.1110 | 2.0665 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
109.243 |
|
O2 |
P1 |
H4 |
98.515 |
O2 |
P1 |
H5 |
98.515 |
|
H4 |
P1 |
H5 |
91.705 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.224 |
|
|
|
2 |
O |
-0.687 |
|
|
|
3 |
H |
0.399 |
|
|
|
4 |
H |
0.032 |
|
|
|
5 |
H |
0.032 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.989 |
-0.262 |
0.000 |
1.024 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.889 |
4.010 |
0.000 |
y |
4.010 |
-20.506 |
0.000 |
z |
0.000 |
0.000 |
-20.474 |
|
Traceless |
| x | y | z |
x |
0.601 |
4.010 |
0.000 |
y |
4.010 |
-0.325 |
0.000 |
z |
0.000 |
0.000 |
-0.276 |
|
Polar |
3z2-r2 | -0.553 |
x2-y2 | 0.617 |
xy | 4.010 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.011 |
0.713 |
0.000 |
y |
0.713 |
3.896 |
0.000 |
z |
0.000 |
0.000 |
3.897 |
<r2> (average value of r
2) Å
2
<r2> |
36.021 |
(<r2>)1/2 |
6.002 |