Jump to
S1C2
Energy calculated at BLYP/6-311G*
| | hartrees |
| Energy at 0K | -959.051192 |
| Energy at 298.15K | |
| HF Energy | -959.051192 |
| Nuclear repulsion energy | 123.725976 |
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 BLYP/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 |
3180 |
3172 |
0.54 |
|
|
|
| 2 |
A1 |
706 |
704 |
7.35 |
|
|
|
| 3 |
A1 |
301 |
300 |
0.07 |
|
|
|
| 4 |
B1 |
378i |
377i |
64.91 |
|
|
|
| 5 |
B2 |
1213 |
1210 |
43.13 |
|
|
|
| 6 |
B2 |
841 |
839 |
188.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2930.7 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 2923.4 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 BLYP/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.676 |
| H2 |
0.000 |
0.000 |
1.760 |
| Cl3 |
0.000 |
1.503 |
-0.171 |
| Cl4 |
0.000 |
-1.503 |
-0.171 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0836 | 1.7255 | 1.7255 |
H2 | 1.0836 | | 2.4471 | 2.4471 | Cl3 | 1.7255 | 2.4471 | | 3.0058 | Cl4 | 1.7255 | 2.4471 | 3.0058 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.422 |
|
Cl3 |
C1 |
Cl4 |
121.155 |
| Cl4 |
C1 |
H2 |
119.422 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.382 |
|
|
|
| 2 |
H |
0.287 |
|
|
|
| 3 |
Cl |
0.047 |
|
|
|
| 4 |
Cl |
0.047 |
|
|
|
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 |
0.918 |
0.918 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.736 |
0.000 |
0.000 |
| y |
0.000 |
-31.646 |
0.000 |
| z |
0.000 |
0.000 |
-29.630 |
|
| Traceless |
| | x | y | z |
| x |
-2.099 |
0.000 |
0.000 |
| y |
0.000 |
-0.462 |
0.000 |
| z |
0.000 |
0.000 |
2.561 |
|
| Polar |
| 3z2-r2 | 5.122 |
| x2-y2 | -1.091 |
| 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 |
2.238 |
0.000 |
0.000 |
| y |
0.000 |
7.532 |
0.000 |
| z |
0.000 |
0.000 |
3.783 |
<r2> (average value of r
2) Å
2
| <r2> |
103.209 |
| (<r2>)1/2 |
10.159 |
Jump to
S1C1
Energy calculated at BLYP/6-311G*
| | hartrees |
| Energy at 0K | -959.052268 |
| Energy at 298.15K | -959.052997 |
| HF Energy | -959.052268 |
| Nuclear repulsion energy | 123.401920 |
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 BLYP/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' |
3133 |
3126 |
4.07 |
|
|
|
| 2 |
A' |
720 |
718 |
16.26 |
|
|
|
| 3 |
A' |
482 |
481 |
29.85 |
|
|
|
| 4 |
A' |
295 |
294 |
0.32 |
|
|
|
| 5 |
A" |
1221 |
1218 |
33.77 |
|
|
|
| 6 |
A" |
797 |
795 |
220.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3323.8 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 3315.5 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.706 |
0.000 |
| H2 |
-0.530 |
1.648 |
0.000 |
| Cl3 |
0.013 |
-0.173 |
1.500 |
| Cl4 |
0.013 |
-0.173 |
-1.500 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0874 | 1.7390 | 1.7390 |
H2 | 1.0874 | | 2.4215 | 2.4215 | Cl3 | 1.7390 | 2.4215 | | 3.0002 | Cl4 | 1.7390 | 2.4215 | 3.0002 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
115.982 |
|
Cl3 |
C1 |
Cl4 |
119.227 |
| Cl4 |
C1 |
H2 |
115.982 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.361 |
|
|
|
| 2 |
H |
0.281 |
|
|
|
| 3 |
Cl |
0.040 |
|
|
|
| 4 |
Cl |
0.040 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.605 |
0.804 |
0.000 |
1.006 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.380 |
-1.013 |
0.000 |
| y |
-1.013 |
-30.189 |
0.000 |
| z |
0.000 |
0.000 |
-31.876 |
|
| Traceless |
| | x | y | z |
| x |
-1.348 |
-1.013 |
0.000 |
| y |
-1.013 |
1.940 |
0.000 |
| z |
0.000 |
0.000 |
-0.592 |
|
| Polar |
| 3z2-r2 | -1.183 |
| x2-y2 | -2.192 |
| xy | -1.013 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.354 |
-0.186 |
0.000 |
| y |
-0.186 |
3.830 |
0.000 |
| z |
0.000 |
0.000 |
7.676 |
<r2> (average value of r
2) Å
2
| <r2> |
103.192 |
| (<r2>)1/2 |
10.158 |