Jump to
S1C2
Energy calculated at PBE1PBE/cc-pVDZ
| hartrees |
Energy at 0K | -418.156248 |
Energy at 298.15K | -418.160351 |
HF Energy | -418.156248 |
Nuclear repulsion energy | 60.863367 |
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 PBE1PBE/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' |
3838 |
3690 |
60.06 |
|
|
|
2 |
A' |
2317 |
2227 |
104.65 |
|
|
|
3 |
A' |
1130 |
1086 |
4.61 |
|
|
|
4 |
A' |
1100 |
1058 |
48.79 |
|
|
|
5 |
A' |
899 |
864 |
31.34 |
|
|
|
6 |
A' |
807 |
776 |
129.84 |
|
|
|
7 |
A" |
2325 |
2236 |
152.39 |
|
|
|
8 |
A" |
899 |
864 |
15.48 |
|
|
|
9 |
A" |
414 |
398 |
103.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6863.9 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 6599.7 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 PBE1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
-0.109 |
-0.574 |
0.000 |
O2 |
-0.109 |
1.107 |
0.000 |
H3 |
0.786 |
1.470 |
0.000 |
H4 |
0.860 |
-0.857 |
1.033 |
H5 |
0.860 |
-0.857 |
-1.033 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6813 | 2.2313 | 1.4448 | 1.4448 |
O2 | 1.6813 | | 0.9660 | 2.4218 | 2.4218 | H3 | 2.2313 | 0.9660 | | 2.5468 | 2.5468 | H4 | 1.4448 | 2.4218 | 2.5468 | | 2.0667 | H5 | 1.4448 | 2.4218 | 2.5468 | 2.0667 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
112.039 |
|
O2 |
P1 |
H4 |
101.285 |
O2 |
P1 |
H5 |
101.285 |
|
H4 |
P1 |
H5 |
91.319 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.235 |
|
|
|
2 |
O |
-0.383 |
|
|
|
3 |
H |
0.176 |
|
|
|
4 |
H |
-0.014 |
|
|
|
5 |
H |
-0.014 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.095 |
-0.029 |
0.000 |
2.096 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.879 |
1.550 |
0.000 |
y |
1.550 |
-19.520 |
0.000 |
z |
0.000 |
0.000 |
-19.897 |
|
Traceless |
| x | y | z |
x |
-0.170 |
1.550 |
0.000 |
y |
1.550 |
0.368 |
0.000 |
z |
0.000 |
0.000 |
-0.198 |
|
Polar |
3z2-r2 | -0.395 |
x2-y2 | -0.359 |
xy | 1.550 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.637 |
-0.348 |
0.000 |
y |
-0.348 |
3.812 |
0.000 |
z |
0.000 |
0.000 |
3.820 |
<r2> (average value of r
2) Å
2
<r2> |
35.233 |
(<r2>)1/2 |
5.936 |
Jump to
S1C1
Energy calculated at PBE1PBE/cc-pVDZ
| hartrees |
Energy at 0K | -418.156822 |
Energy at 298.15K | -418.160739 |
HF Energy | -418.156822 |
Nuclear repulsion energy | 60.774786 |
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 PBE1PBE/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' |
3860 |
3711 |
100.58 |
|
|
|
2 |
A' |
2364 |
2273 |
85.01 |
|
|
|
3 |
A' |
1148 |
1104 |
91.26 |
|
|
|
4 |
A' |
1125 |
1082 |
18.23 |
|
|
|
5 |
A' |
900 |
865 |
16.14 |
|
|
|
6 |
A' |
803 |
772 |
95.21 |
|
|
|
7 |
A" |
2368 |
2277 |
119.32 |
|
|
|
8 |
A" |
920 |
884 |
1.60 |
|
|
|
9 |
A" |
243 |
233 |
82.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6865.9 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 6601.6 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 PBE1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
P1 |
0.040 |
-0.580 |
0.000 |
O2 |
0.040 |
1.112 |
0.000 |
H3 |
0.965 |
1.386 |
0.000 |
H4 |
-0.938 |
-0.791 |
1.033 |
H5 |
-0.938 |
-0.791 |
-1.033 |
Atom - Atom Distances (Å)
|
P1 |
O2 |
H3 |
H4 |
H5 |
P1 | | 1.6919 | 2.1728 | 1.4383 | 1.4383 |
O2 | 1.6919 | | 0.9650 | 2.3763 | 2.3763 | H3 | 2.1728 | 0.9650 | | 3.0710 | 3.0710 | H4 | 1.4383 | 2.3763 | 3.0710 | | 2.0667 | H5 | 1.4383 | 2.3763 | 3.0710 | 2.0667 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
P1 |
O2 |
H3 |
106.502 |
|
O2 |
P1 |
H4 |
98.459 |
O2 |
P1 |
H5 |
98.459 |
|
H4 |
P1 |
H5 |
91.857 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
P |
0.197 |
|
|
|
2 |
O |
-0.380 |
|
|
|
3 |
H |
0.175 |
|
|
|
4 |
H |
0.004 |
|
|
|
5 |
H |
0.004 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.759 |
-0.215 |
0.000 |
0.789 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.010 |
3.685 |
0.000 |
y |
3.685 |
-20.053 |
0.000 |
z |
0.000 |
0.000 |
-19.750 |
|
Traceless |
| x | y | z |
x |
0.892 |
3.685 |
0.000 |
y |
3.685 |
-0.673 |
0.000 |
z |
0.000 |
0.000 |
-0.218 |
|
Polar |
3z2-r2 | -0.437 |
x2-y2 | 1.044 |
xy | 3.685 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.791 |
0.699 |
0.000 |
y |
0.699 |
3.763 |
0.000 |
z |
0.000 |
0.000 |
3.801 |
<r2> (average value of r
2) Å
2
<r2> |
35.218 |
(<r2>)1/2 |
5.934 |