Jump to
S1C2
Energy calculated at B3LYP/6-311G*
| hartrees |
Energy at 0K | -959.098803 |
Energy at 298.15K | |
HF Energy | -959.098803 |
Nuclear repulsion energy | 124.942279 |
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 B3LYP/6-311G*
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 |
3261 |
3151 |
0.28 |
|
|
|
2 |
A1 |
739 |
714 |
8.52 |
|
|
|
3 |
A1 |
312 |
302 |
0.14 |
|
|
|
4 |
B1 |
366i |
353i |
62.43 |
|
|
|
5 |
B2 |
1255 |
1213 |
48.17 |
|
|
|
6 |
B2 |
896 |
865 |
179.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3048.7 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 2945.9 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 B3LYP/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.671 |
H2 |
0.000 |
0.000 |
1.749 |
Cl3 |
0.000 |
1.487 |
-0.170 |
Cl4 |
0.000 |
-1.487 |
-0.170 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0770 | 1.7089 | 1.7089 |
H2 | 1.0770 | | 2.4275 | 2.4275 | Cl3 | 1.7089 | 2.4275 | | 2.9747 | Cl4 | 1.7089 | 2.4275 | 2.9747 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.497 |
|
Cl3 |
C1 |
Cl4 |
121.005 |
Cl4 |
C1 |
H2 |
119.497 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.382 |
|
|
|
2 |
H |
0.300 |
|
|
|
3 |
Cl |
0.041 |
|
|
|
4 |
Cl |
0.041 |
|
|
|
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 |
0.983 |
0.983 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.593 |
0.000 |
0.000 |
y |
0.000 |
-31.693 |
0.000 |
z |
0.000 |
0.000 |
-29.459 |
|
Traceless |
| x | y | z |
x |
-2.018 |
0.000 |
0.000 |
y |
0.000 |
-0.667 |
0.000 |
z |
0.000 |
0.000 |
2.684 |
|
Polar |
3z2-r2 | 5.369 |
x2-y2 | -0.901 |
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 |
2.201 |
0.000 |
0.000 |
y |
0.000 |
7.097 |
0.000 |
z |
0.000 |
0.000 |
3.673 |
<r2> (average value of r
2) Å
2
<r2> |
101.478 |
(<r2>)1/2 |
10.074 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G*
| hartrees |
Energy at 0K | -959.099637 |
Energy at 298.15K | -959.100412 |
HF Energy | -959.099637 |
Nuclear repulsion energy | 124.727708 |
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 B3LYP/6-311G*
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' |
3223 |
3115 |
3.01 |
|
|
|
2 |
A' |
748 |
723 |
15.21 |
|
|
|
3 |
A' |
478 |
462 |
32.14 |
|
|
|
4 |
A' |
306 |
296 |
0.60 |
|
|
|
5 |
A" |
1264 |
1222 |
40.16 |
|
|
|
6 |
A" |
861 |
832 |
208.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3440.1 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 3324.2 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 B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
0.696 |
0.000 |
H2 |
-0.488 |
1.654 |
0.000 |
Cl3 |
0.012 |
-0.172 |
1.484 |
Cl4 |
0.012 |
-0.172 |
-1.484 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0802 | 1.7193 | 1.7193 |
H2 | 1.0802 | | 2.4051 | 2.4051 | Cl3 | 1.7193 | 2.4051 | | 2.9684 | Cl4 | 1.7193 | 2.4051 | 2.9684 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
116.577 |
|
Cl3 |
C1 |
Cl4 |
119.368 |
Cl4 |
C1 |
H2 |
116.577 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.361 |
|
|
|
2 |
H |
0.293 |
|
|
|
3 |
Cl |
0.034 |
|
|
|
4 |
Cl |
0.034 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.556 |
0.887 |
0.000 |
1.047 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.285 |
-0.950 |
0.000 |
y |
-0.950 |
-29.937 |
0.000 |
z |
0.000 |
0.000 |
-31.884 |
|
Traceless |
| x | y | z |
x |
-1.374 |
-0.950 |
0.000 |
y |
-0.950 |
2.148 |
0.000 |
z |
0.000 |
0.000 |
-0.773 |
|
Polar |
3z2-r2 | -1.547 |
x2-y2 | -2.348 |
xy | -0.950 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.294 |
-0.166 |
0.000 |
y |
-0.166 |
3.705 |
0.000 |
z |
0.000 |
0.000 |
7.190 |
<r2> (average value of r
2) Å
2
<r2> |
101.378 |
(<r2>)1/2 |
10.069 |