Jump to
S1C2
Energy calculated at BLYP/6-31G(2df,p)
| hartrees |
Energy at 0K | -958.989396 |
Energy at 298.15K | |
HF Energy | -958.989396 |
Nuclear repulsion energy | 124.226829 |
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/6-31G(2df,p)
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 |
3186 |
3169 |
0.08 |
|
|
|
2 |
A1 |
713 |
710 |
7.50 |
|
|
|
3 |
A1 |
295 |
294 |
0.34 |
|
|
|
4 |
B1 |
374i |
372i |
37.90 |
|
|
|
5 |
B2 |
1180 |
1173 |
45.43 |
|
|
|
6 |
B2 |
858 |
853 |
155.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2929.1 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 2913.0 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/6-31G(2df,p)
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 |
1.761 |
Cl3 |
0.000 |
1.496 |
-0.171 |
Cl4 |
0.000 |
-1.496 |
-0.171 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0848 | 1.7187 | 1.7187 |
H2 | 1.0848 | | 2.4430 | 2.4430 | Cl3 | 1.7187 | 2.4430 | | 2.9913 | Cl4 | 1.7187 | 2.4430 | 2.9913 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.518 |
|
Cl3 |
C1 |
Cl4 |
120.964 |
Cl4 |
C1 |
H2 |
119.518 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.052 |
|
|
|
2 |
H |
0.160 |
|
|
|
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 |
|
0.000 |
0.000 |
0.912 |
0.912 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.496 |
0.000 |
0.000 |
y |
0.000 |
-30.605 |
0.000 |
z |
0.000 |
0.000 |
-28.695 |
|
Traceless |
| x | y | z |
x |
-1.846 |
0.000 |
0.000 |
y |
0.000 |
-0.509 |
0.000 |
z |
0.000 |
0.000 |
2.356 |
|
Polar |
3z2-r2 | 4.711 |
x2-y2 | -0.891 |
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 |
3.188 |
0.000 |
0.000 |
y |
0.000 |
7.519 |
0.000 |
z |
0.000 |
0.000 |
4.398 |
<r2> (average value of r
2) Å
2
<r2> |
101.793 |
(<r2>)1/2 |
10.089 |
Jump to
S1C1
Energy calculated at BLYP/6-31G(2df,p)
| hartrees |
Energy at 0K | -958.990412 |
Energy at 298.15K | -958.991138 |
HF Energy | -958.990412 |
Nuclear repulsion energy | 123.923298 |
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/6-31G(2df,p)
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' |
3137 |
3119 |
1.80 |
|
|
|
2 |
A' |
726 |
722 |
13.94 |
|
|
|
3 |
A' |
476 |
474 |
19.06 |
|
|
|
4 |
A' |
290 |
288 |
0.31 |
|
|
|
5 |
A" |
1184 |
1178 |
36.41 |
|
|
|
6 |
A" |
817 |
812 |
182.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3314.4 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 3296.2 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 BLYP/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.013 |
0.705 |
0.000 |
H2 |
-0.523 |
1.653 |
0.000 |
Cl3 |
0.013 |
-0.173 |
1.492 |
Cl4 |
0.013 |
-0.173 |
-1.492 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0891 | 1.7318 | 1.7318 |
H2 | 1.0891 | | 2.4189 | 2.4189 | Cl3 | 1.7318 | 2.4189 | | 2.9849 | Cl4 | 1.7318 | 2.4189 | 2.9849 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
116.199 |
|
Cl3 |
C1 |
Cl4 |
119.031 |
Cl4 |
C1 |
H2 |
116.199 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.053 |
|
|
|
2 |
H |
0.163 |
|
|
|
3 |
Cl |
-0.055 |
|
|
|
4 |
Cl |
-0.055 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.475 |
0.808 |
0.000 |
0.937 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.218 |
-0.860 |
0.000 |
y |
-0.860 |
-29.158 |
0.000 |
z |
0.000 |
0.000 |
-30.737 |
|
Traceless |
| x | y | z |
x |
-1.271 |
-0.860 |
0.000 |
y |
-0.860 |
1.820 |
0.000 |
z |
0.000 |
0.000 |
-0.549 |
|
Polar |
3z2-r2 | -1.097 |
x2-y2 | -2.060 |
xy | -0.860 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.294 |
-0.196 |
0.000 |
y |
-0.196 |
4.414 |
0.000 |
z |
0.000 |
0.000 |
7.650 |
<r2> (average value of r
2) Å
2
<r2> |
101.719 |
(<r2>)1/2 |
10.086 |