Jump to
S1C2
Energy calculated at HF/6-31G(2df,p)
| hartrees |
Energy at 0K | -417.342506 |
Energy at 298.15K | -417.346731 |
HF Energy | -417.342506 |
Nuclear repulsion energy | 62.711536 |
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 HF/6-31G(2df,p)
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' |
4180 |
3785 |
95.96 |
|
|
|
2 |
A' |
2489 |
2254 |
112.32 |
|
|
|
3 |
A' |
1251 |
1133 |
20.87 |
|
|
|
4 |
A' |
1205 |
1091 |
67.77 |
|
|
|
5 |
A' |
993 |
899 |
56.40 |
|
|
|
6 |
A' |
899 |
814 |
175.07 |
|
|
|
7 |
A" |
2481 |
2247 |
183.78 |
|
|
|
8 |
A" |
1003 |
908 |
31.75 |
|
|
|
9 |
A" |
451 |
409 |
110.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7475.6 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 6769.1 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 HF/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
-0.104 |
-0.556 |
0.000 |
O2 |
-0.104 |
1.068 |
0.000 |
H3 |
0.743 |
1.476 |
0.000 |
H4 |
0.824 |
-0.838 |
1.028 |
H5 |
0.824 |
-0.838 |
-1.028 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6241 | 2.2020 | 1.4127 | 1.4127 |
O2 | 1.6241 | | 0.9406 | 2.3556 | 2.3556 | H3 | 2.2020 | 0.9406 | | 2.5335 | 2.5335 | H4 | 1.4127 | 2.3556 | 2.5335 | | 2.0555 | H5 | 1.4127 | 2.3556 | 2.5335 | 2.0555 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
115.727 |
|
O2 |
P1 |
H4 |
101.508 |
O2 |
P1 |
H5 |
101.508 |
|
H4 |
P1 |
H5 |
93.353 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.192 |
|
|
|
2 |
O |
-0.562 |
|
|
|
3 |
H |
0.346 |
|
|
|
4 |
H |
0.012 |
|
|
|
5 |
H |
0.012 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.182 |
0.230 |
0.000 |
2.194 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.262 |
1.383 |
0.000 |
y |
1.383 |
-19.411 |
0.000 |
z |
0.000 |
0.000 |
-19.847 |
|
Traceless |
| x | y | z |
x |
-0.633 |
1.383 |
0.000 |
y |
1.383 |
0.643 |
0.000 |
z |
0.000 |
0.000 |
-0.010 |
|
Polar |
3z2-r2 | -0.021 |
x2-y2 | -0.851 |
xy | 1.383 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.479 |
-0.170 |
0.000 |
y |
-0.170 |
3.666 |
0.000 |
z |
0.000 |
0.000 |
3.733 |
<r2> (average value of r
2) Å
2
<r2> |
34.009 |
(<r2>)1/2 |
5.832 |
Jump to
S1C1
Energy calculated at HF/6-31G(2df,p)
| hartrees |
Energy at 0K | -417.342301 |
Energy at 298.15K | -417.346370 |
HF Energy | -417.342301 |
Nuclear repulsion energy | 62.643591 |
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 HF/6-31G(2df,p)
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' |
4200 |
3803 |
143.01 |
|
|
|
2 |
A' |
2530 |
2291 |
94.23 |
|
|
|
3 |
A' |
1255 |
1136 |
34.88 |
|
|
|
4 |
A' |
1232 |
1115 |
153.00 |
|
|
|
5 |
A' |
1002 |
907 |
31.56 |
|
|
|
6 |
A' |
890 |
806 |
136.83 |
|
|
|
7 |
A" |
2521 |
2283 |
144.48 |
|
|
|
8 |
A" |
1011 |
915 |
9.35 |
|
|
|
9 |
A" |
296 |
268 |
105.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7467.9 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 6762.2 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 HF/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
0.038 |
-0.560 |
0.000 |
O2 |
0.038 |
1.071 |
0.000 |
H3 |
0.913 |
1.413 |
0.000 |
H4 |
-0.894 |
-0.792 |
1.028 |
H5 |
-0.894 |
-0.792 |
-1.028 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6313 | 2.1586 | 1.4068 | 1.4068 |
O2 | 1.6313 | | 0.9397 | 2.3235 | 2.3235 | H3 | 2.1586 | 0.9397 | | 3.0310 | 3.0310 | H4 | 1.4068 | 2.3235 | 3.0310 | | 2.0561 | H5 | 1.4068 | 2.3235 | 3.0310 | 2.0561 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
111.326 |
|
O2 |
P1 |
H4 |
99.510 |
O2 |
P1 |
H5 |
99.510 |
|
H4 |
P1 |
H5 |
93.907 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.163 |
|
|
|
2 |
O |
-0.562 |
|
|
|
3 |
H |
0.355 |
|
|
|
4 |
H |
0.022 |
|
|
|
5 |
H |
0.022 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.660 |
0.113 |
0.000 |
0.670 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.456 |
4.016 |
0.000 |
y |
4.016 |
-19.894 |
0.000 |
z |
0.000 |
0.000 |
-19.764 |
|
Traceless |
| x | y | z |
x |
0.373 |
4.016 |
0.000 |
y |
4.016 |
-0.285 |
0.000 |
z |
0.000 |
0.000 |
-0.088 |
|
Polar |
3z2-r2 | -0.177 |
x2-y2 | 0.439 |
xy | 4.016 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.585 |
0.495 |
0.000 |
y |
0.495 |
3.655 |
0.000 |
z |
0.000 |
0.000 |
3.766 |
<r2> (average value of r
2) Å
2
<r2> |
34.025 |
(<r2>)1/2 |
5.833 |