Jump to
S1C2
Energy calculated at B3LYPultrafine/6-31+G**
| | hartrees |
| Energy at 0K | -959.039348 |
| Energy at 298.15K | |
| HF Energy | -959.039348 |
| Nuclear repulsion energy | 124.851901 |
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 B3LYPultrafine/6-31+G**
| 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 |
3275 |
3152 |
0.38 |
|
|
|
| 2 |
A1 |
745 |
717 |
8.59 |
|
|
|
| 3 |
A1 |
311 |
300 |
0.27 |
|
|
|
| 4 |
B1 |
346i |
333i |
57.31 |
|
|
|
| 5 |
B2 |
1252 |
1205 |
52.82 |
|
|
|
| 6 |
B2 |
908 |
874 |
172.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3071.8 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 2957.2 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 B3LYPultrafine/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.672 |
| H2 |
0.000 |
0.000 |
1.752 |
| Cl3 |
0.000 |
1.488 |
-0.170 |
| Cl4 |
0.000 |
-1.488 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0796 | 1.7101 | 1.7101 |
H2 | 1.0796 | | 2.4308 | 2.4308 | Cl3 | 1.7101 | 2.4308 | | 2.9764 | Cl4 | 1.7101 | 2.4308 | 2.9764 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.511 |
|
Cl3 |
C1 |
Cl4 |
120.978 |
| Cl4 |
C1 |
H2 |
119.511 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.336 |
|
|
|
| 2 |
H |
0.218 |
|
|
|
| 3 |
Cl |
0.059 |
|
|
|
| 4 |
Cl |
0.059 |
|
|
|
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 |
0.981 |
0.981 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.304 |
0.000 |
0.000 |
| y |
0.000 |
-31.460 |
0.000 |
| z |
0.000 |
0.000 |
-29.290 |
|
| Traceless |
| | x | y | z |
| x |
-1.929 |
0.000 |
0.000 |
| y |
0.000 |
-0.663 |
0.000 |
| z |
0.000 |
0.000 |
2.592 |
|
| Polar |
| 3z2-r2 | 5.184 |
| x2-y2 | -0.844 |
| 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 |
3.399 |
0.000 |
0.000 |
| y |
0.000 |
7.360 |
0.000 |
| z |
0.000 |
0.000 |
4.437 |
<r2> (average value of r
2) Å
2
| <r2> |
101.439 |
| (<r2>)1/2 |
10.072 |
Jump to
S1C1
Energy calculated at B3LYPultrafine/6-31+G**
| | hartrees |
| Energy at 0K | -959.040028 |
| Energy at 298.15K | -959.040793 |
| HF Energy | -959.040028 |
| Nuclear repulsion energy | 124.664131 |
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 B3LYPultrafine/6-31+G**
| 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' |
3237 |
3116 |
0.88 |
|
|
|
| 2 |
A' |
751 |
723 |
14.07 |
|
|
|
| 3 |
A' |
462 |
445 |
29.20 |
|
|
|
| 4 |
A' |
305 |
293 |
0.71 |
|
|
|
| 5 |
A" |
1256 |
1209 |
45.10 |
|
|
|
| 6 |
A" |
876 |
844 |
198.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3443.1 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 3314.7 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 B3LYPultrafine/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.695 |
0.000 |
| H2 |
-0.468 |
1.665 |
0.000 |
| Cl3 |
0.012 |
-0.172 |
1.485 |
| Cl4 |
0.012 |
-0.172 |
-1.485 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0826 | 1.7195 | 1.7195 |
H2 | 1.0826 | | 2.4106 | 2.4106 | Cl3 | 1.7195 | 2.4106 | | 2.9703 | Cl4 | 1.7195 | 2.4106 | 2.9703 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.859 |
|
Cl3 |
C1 |
Cl4 |
119.470 |
| Cl4 |
C1 |
H2 |
116.859 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.315 |
|
|
|
| 2 |
H |
0.213 |
|
|
|
| 3 |
Cl |
0.051 |
|
|
|
| 4 |
Cl |
0.051 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.511 |
0.902 |
0.000 |
1.037 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.027 |
-0.955 |
0.000 |
| y |
-0.955 |
-29.714 |
0.000 |
| z |
0.000 |
0.000 |
-31.615 |
|
| Traceless |
| | x | y | z |
| x |
-1.363 |
-0.955 |
0.000 |
| y |
-0.955 |
2.107 |
0.000 |
| z |
0.000 |
0.000 |
-0.745 |
|
| Polar |
| 3z2-r2 | -1.489 |
| x2-y2 | -2.313 |
| xy | -0.955 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.467 |
-0.080 |
0.000 |
| y |
-0.080 |
4.480 |
0.000 |
| z |
0.000 |
0.000 |
7.464 |
<r2> (average value of r
2) Å
2
| <r2> |
101.327 |
| (<r2>)1/2 |
10.066 |