Jump to
S1C2
Energy calculated at LSDA/cc-pVTZ
| hartrees |
Energy at 0K | -684.152722 |
Energy at 298.15K | |
HF Energy | -684.152722 |
Nuclear repulsion energy | 193.147779 |
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 LSDA/cc-pVTZ
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' |
3584 |
3545 |
86.56 |
|
|
|
2 |
A' |
1128 |
1116 |
75.43 |
|
|
|
3 |
A' |
1031 |
1020 |
31.58 |
|
|
|
4 |
A' |
619 |
612 |
203.96 |
|
|
|
5 |
A' |
510 |
504 |
22.82 |
|
|
|
6 |
A' |
393 |
388 |
6.27 |
|
|
|
7 |
A" |
1181 |
1169 |
221.80 |
|
|
|
8 |
A" |
377 |
373 |
25.87 |
|
|
|
9 |
A" |
142i |
141i |
63.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4340.2 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 4292.9 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 LSDA/cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.360 |
0.122 |
0.000 |
O2 |
-0.206 |
-1.497 |
0.000 |
H3 |
-1.184 |
-1.381 |
0.000 |
O4 |
-0.206 |
0.705 |
1.213 |
O5 |
-0.206 |
0.705 |
-1.213 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7151 | 2.1552 | 1.4603 | 1.4603 |
O2 | 1.7151 | | 0.9851 | 2.5142 | 2.5142 | H3 | 2.1552 | 0.9851 | | 2.6042 | 2.6042 | O4 | 1.4603 | 2.5142 | 2.6042 | | 2.4263 | O5 | 1.4603 | 2.5142 | 2.6042 | 2.4263 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.231 |
|
O2 |
Cl1 |
O3 |
26.499 |
O2 |
Cl1 |
O4 |
104.417 |
|
O3 |
Cl1 |
O4 |
90.039 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.793 |
|
|
|
2 |
O |
-0.309 |
|
|
|
3 |
H |
0.210 |
|
|
|
4 |
O |
-0.347 |
|
|
|
5 |
O |
-0.347 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.015 |
-0.959 |
0.000 |
0.959 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.902 |
3.023 |
0.000 |
y |
3.023 |
-30.432 |
0.000 |
z |
0.000 |
0.000 |
-32.632 |
|
Traceless |
| x | y | z |
x |
6.630 |
3.023 |
0.000 |
y |
3.023 |
-1.665 |
0.000 |
z |
0.000 |
0.000 |
-4.965 |
|
Polar |
3z2-r2 | -9.930 |
x2-y2 | 5.530 |
xy | 3.023 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.222 |
0.293 |
0.000 |
y |
0.293 |
4.840 |
0.000 |
z |
0.000 |
0.000 |
4.607 |
<r2> (average value of r
2) Å
2
<r2> |
74.534 |
(<r2>)1/2 |
8.633 |
Jump to
S1C1
Energy calculated at LSDA/cc-pVTZ
| hartrees |
Energy at 0K | -684.153047 |
Energy at 298.15K | -684.155655 |
HF Energy | -684.153047 |
Nuclear repulsion energy | 193.288774 |
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 LSDA/cc-pVTZ
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 |
3592 |
3553 |
98.54 |
|
|
|
2 |
A |
1201 |
1187 |
187.37 |
|
|
|
3 |
A |
1117 |
1105 |
106.40 |
|
|
|
4 |
A |
1023 |
1012 |
36.00 |
|
|
|
5 |
A |
631 |
624 |
193.59 |
|
|
|
6 |
A |
514 |
509 |
27.62 |
|
|
|
7 |
A |
399 |
394 |
5.71 |
|
|
|
8 |
A |
341 |
337 |
6.90 |
|
|
|
9 |
A |
162 |
160 |
85.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4489.5 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 4440.6 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 LSDA/cc-pVTZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.169 |
0.021 |
-0.345 |
O2 |
-1.414 |
-0.502 |
0.072 |
O3 |
0.208 |
1.363 |
0.244 |
O4 |
1.052 |
-0.924 |
0.319 |
H5 |
-1.644 |
0.143 |
0.779 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
O3 |
O4 |
H5 |
Cl1 | | 1.7191 | 1.4658 | 1.4539 | 2.1371 |
O2 | 1.7191 | | 2.4782 | 2.5148 | 0.9844 | O3 | 1.4658 | 2.4782 | | 2.4388 | 2.2818 | O4 | 1.4539 | 2.5148 | 2.4388 | | 2.9367 | H5 | 2.1371 | 0.9844 | 2.2818 | 2.9367 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
100.946 |
|
O2 |
Cl1 |
O3 |
101.880 |
O2 |
Cl1 |
O4 |
104.540 |
|
O3 |
Cl1 |
O4 |
113.287 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.795 |
|
|
|
2 |
O |
-0.314 |
|
|
|
3 |
O |
-0.369 |
|
|
|
4 |
O |
-0.325 |
|
|
|
5 |
H |
0.213 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.120 |
0.479 |
-0.518 |
1.323 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-28.642 |
-0.865 |
-3.073 |
y |
-0.865 |
-32.491 |
0.373 |
z |
-3.073 |
0.373 |
-26.736 |
|
Traceless |
| x | y | z |
x |
0.972 |
-0.865 |
-3.073 |
y |
-0.865 |
-4.802 |
0.373 |
z |
-3.073 |
0.373 |
3.830 |
|
Polar |
3z2-r2 | 7.660 |
x2-y2 | 3.849 |
xy | -0.865 |
xz | -3.073 |
yz | 0.373 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.973 |
-0.124 |
-0.125 |
y |
-0.124 |
4.669 |
0.100 |
z |
-0.125 |
0.100 |
2.986 |
<r2> (average value of r
2) Å
2
<r2> |
74.391 |
(<r2>)1/2 |
8.625 |