Jump to
S1C2
Energy calculated at B2PLYP/3-21G*
| | hartrees |
| Energy at 0K | -954.265789 |
| Energy at 298.15K | |
| HF Energy | -954.153090 |
| Nuclear repulsion energy | 124.955009 |
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 B2PLYP/3-21G*
| 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 |
3312 |
3312 |
0.25 |
|
|
|
| 2 |
A1 |
730 |
730 |
10.54 |
|
|
|
| 3 |
A1 |
313 |
313 |
0.44 |
|
|
|
| 4 |
B1 |
291i |
291i |
74.20 |
|
|
|
| 5 |
B2 |
1290 |
1290 |
41.76 |
|
|
|
| 6 |
B2 |
886 |
886 |
154.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3119.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3119.9 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 B2PLYP/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.678 |
| H2 |
0.000 |
0.000 |
1.753 |
| Cl3 |
0.000 |
1.485 |
-0.171 |
| Cl4 |
0.000 |
-1.485 |
-0.171 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0749 | 1.7107 | 1.7107 |
H2 | 1.0749 | | 2.4306 | 2.4306 | Cl3 | 1.7107 | 2.4306 | | 2.9699 | Cl4 | 1.7107 | 2.4306 | 2.9699 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.769 |
|
Cl3 |
C1 |
Cl4 |
120.463 |
| Cl4 |
C1 |
H2 |
119.769 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.397 |
|
|
|
| 2 |
H |
0.273 |
|
|
|
| 3 |
Cl |
0.062 |
|
|
|
| 4 |
Cl |
0.062 |
|
|
|
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 |
1.041 |
1.041 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.178 |
0.000 |
0.000 |
| y |
0.000 |
-31.404 |
0.000 |
| z |
0.000 |
0.000 |
-29.021 |
|
| Traceless |
| | x | y | z |
| x |
-1.966 |
0.000 |
0.000 |
| y |
0.000 |
-0.804 |
0.000 |
| z |
0.000 |
0.000 |
2.770 |
|
| Polar |
| 3z2-r2 | 5.540 |
| x2-y2 | -0.774 |
| 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 |
1.951 |
0.000 |
0.000 |
| y |
0.000 |
6.305 |
0.000 |
| z |
0.000 |
0.000 |
3.397 |
<r2> (average value of r
2) Å
2
| <r2> |
101.080 |
| (<r2>)1/2 |
10.054 |
Jump to
S1C1
Energy calculated at B2PLYP/3-21G*
| | hartrees |
| Energy at 0K | -954.266150 |
| Energy at 298.15K | -954.266851 |
| HF Energy | -954.153314 |
| Nuclear repulsion energy | 124.710887 |
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 B2PLYP/3-21G*
| 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' |
3283 |
3283 |
0.95 |
|
|
|
| 2 |
A' |
737 |
737 |
16.98 |
|
|
|
| 3 |
A' |
399 |
399 |
41.33 |
|
|
|
| 4 |
A' |
308 |
308 |
1.89 |
|
|
|
| 5 |
A" |
1295 |
1295 |
35.92 |
|
|
|
| 6 |
A" |
857 |
857 |
169.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3439.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3439.5 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 B2PLYP/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.010 |
0.697 |
0.000 |
| H2 |
-0.407 |
1.690 |
0.000 |
| Cl3 |
0.010 |
-0.173 |
1.484 |
| Cl4 |
0.010 |
-0.173 |
-1.484 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0774 | 1.7195 | 1.7195 |
H2 | 1.0774 | | 2.4174 | 2.4174 | Cl3 | 1.7195 | 2.4174 | | 2.9672 | Cl4 | 1.7195 | 2.4174 | 2.9672 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.777 |
|
Cl3 |
C1 |
Cl4 |
119.270 |
| Cl4 |
C1 |
H2 |
117.777 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.377 |
|
|
|
| 2 |
H |
0.269 |
|
|
|
| 3 |
Cl |
0.054 |
|
|
|
| 4 |
Cl |
0.054 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.506 |
0.969 |
0.000 |
1.093 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.976 |
-0.848 |
0.000 |
| y |
-0.848 |
-29.375 |
0.000 |
| z |
0.000 |
0.000 |
-31.549 |
|
| Traceless |
| | x | y | z |
| x |
-1.514 |
-0.848 |
0.000 |
| y |
-0.848 |
2.387 |
0.000 |
| z |
0.000 |
0.000 |
-0.873 |
|
| Polar |
| 3z2-r2 | -1.745 |
| x2-y2 | -2.601 |
| xy | -0.848 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.027 |
-0.188 |
0.000 |
| y |
-0.188 |
3.403 |
0.000 |
| z |
0.000 |
0.000 |
6.362 |
<r2> (average value of r
2) Å
2
| <r2> |
101.130 |
| (<r2>)1/2 |
10.056 |