Jump to
S1C2
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -958.914461 |
| Energy at 298.15K | |
| HF Energy | -958.914461 |
| Nuclear repulsion energy | 125.523147 |
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 B3PW91/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3298 |
3155 |
0.05 |
|
|
|
| 2 |
A1 |
764 |
731 |
10.31 |
|
|
|
| 3 |
A1 |
316 |
303 |
0.39 |
|
|
|
| 4 |
B1 |
335i |
321i |
60.25 |
|
|
|
| 5 |
B2 |
1268 |
1213 |
54.06 |
|
|
|
| 6 |
B2 |
939 |
898 |
160.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3125.0 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 2989.7 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 B3PW91/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.667 |
| H2 |
0.000 |
0.000 |
1.748 |
| Cl3 |
0.000 |
1.480 |
-0.169 |
| Cl4 |
0.000 |
-1.480 |
-0.169 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0801 | 1.7002 | 1.7002 |
H2 | 1.0801 | | 2.4217 | 2.4217 | Cl3 | 1.7002 | 2.4217 | | 2.9603 | Cl4 | 1.7002 | 2.4217 | 2.9603 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.475 |
|
Cl3 |
C1 |
Cl4 |
121.049 |
| Cl4 |
C1 |
H2 |
119.475 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.396 |
|
|
|
| 2 |
H |
0.255 |
|
|
|
| 3 |
Cl |
0.070 |
|
|
|
| 4 |
Cl |
0.070 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
1.003 |
1.003 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.646 |
0.000 |
0.000 |
| y |
0.000 |
-30.818 |
0.000 |
| z |
0.000 |
0.000 |
-28.587 |
|
| Traceless |
| | x | y | z |
| x |
-1.943 |
0.000 |
0.000 |
| y |
0.000 |
-0.702 |
0.000 |
| z |
0.000 |
0.000 |
2.645 |
|
| Polar |
| 3z2-r2 | 5.290 |
| x2-y2 | -0.828 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.250 |
0.000 |
0.000 |
| y |
0.000 |
6.535 |
0.000 |
| z |
0.000 |
0.000 |
3.634 |
<r2> (average value of r
2) Å
2
| <r2> |
100.145 |
| (<r2>)1/2 |
10.007 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -958.915035 |
| Energy at 298.15K | -958.915804 |
| HF Energy | -958.915035 |
| Nuclear repulsion energy | 125.383938 |
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 B3PW91/6-31G*
| 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' |
3263 |
3122 |
1.77 |
|
|
|
| 2 |
A' |
770 |
737 |
15.55 |
|
|
|
| 3 |
A' |
451 |
431 |
33.58 |
|
|
|
| 4 |
A' |
309 |
295 |
1.21 |
|
|
|
| 5 |
A" |
1274 |
1219 |
46.11 |
|
|
|
| 6 |
A" |
911 |
871 |
182.98 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3488.6 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 3337.5 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 B3PW91/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.688 |
0.000 |
| H2 |
-0.451 |
1.667 |
0.000 |
| Cl3 |
0.011 |
-0.170 |
1.477 |
| Cl4 |
0.011 |
-0.170 |
-1.477 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0828 | 1.7083 | 1.7083 |
H2 | 1.0828 | | 2.4025 | 2.4025 | Cl3 | 1.7083 | 2.4025 | | 2.9540 | Cl4 | 1.7083 | 2.4025 | 2.9540 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.023 |
|
Cl3 |
C1 |
Cl4 |
119.672 |
| Cl4 |
C1 |
H2 |
117.023 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.376 |
|
|
|
| 2 |
H |
0.251 |
|
|
|
| 3 |
Cl |
0.063 |
|
|
|
| 4 |
Cl |
0.063 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.509 |
0.917 |
0.000 |
1.049 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.393 |
-0.878 |
0.000 |
| y |
-0.878 |
-29.001 |
0.000 |
| z |
0.000 |
0.000 |
-30.962 |
|
| Traceless |
| | x | y | z |
| x |
-1.411 |
-0.878 |
0.000 |
| y |
-0.878 |
2.176 |
0.000 |
| z |
0.000 |
0.000 |
-0.764 |
|
| Polar |
| 3z2-r2 | -1.529 |
| x2-y2 | -2.391 |
| xy | -0.878 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.337 |
-0.187 |
0.000 |
| y |
-0.187 |
3.636 |
0.000 |
| z |
0.000 |
0.000 |
6.603 |
<r2> (average value of r
2) Å
2
| <r2> |
100.007 |
| (<r2>)1/2 |
10.000 |