Jump to
S1C2
Energy calculated at BLYP/3-21G*
| hartrees |
Energy at 0K | -954.585296 |
Energy at 298.15K | |
HF Energy | -954.585296 |
Nuclear repulsion energy | 123.455265 |
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/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 |
3201 |
3180 |
0.00 |
|
|
|
2 |
A1 |
689 |
685 |
8.99 |
|
|
|
3 |
A1 |
297 |
295 |
0.24 |
|
|
|
4 |
B1 |
284i |
282i |
80.79 |
|
|
|
5 |
B2 |
1222 |
1214 |
35.48 |
|
|
|
6 |
B2 |
815 |
810 |
172.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2970.0 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 2950.7 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 BLYP/3-21G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.684 |
H2 |
0.000 |
0.000 |
1.768 |
Cl3 |
0.000 |
1.504 |
-0.173 |
Cl4 |
0.000 |
-1.504 |
-0.173 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0840 | 1.7310 | 1.7310 |
H2 | 1.0840 | | 2.4553 | 2.4553 | Cl3 | 1.7310 | 2.4553 | | 3.0084 | Cl4 | 1.7310 | 2.4553 | 3.0084 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.659 |
|
Cl3 |
C1 |
Cl4 |
120.683 |
Cl4 |
C1 |
H2 |
119.659 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.407 |
|
|
|
2 |
H |
0.255 |
|
|
|
3 |
Cl |
0.076 |
|
|
|
4 |
Cl |
0.076 |
|
|
|
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 |
-32.029 |
0.000 |
0.000 |
y |
0.000 |
-30.878 |
0.000 |
z |
0.000 |
0.000 |
-28.919 |
|
Traceless |
| x | y | z |
x |
-2.131 |
0.000 |
0.000 |
y |
0.000 |
-0.403 |
0.000 |
z |
0.000 |
0.000 |
2.534 |
|
Polar |
3z2-r2 | 5.068 |
x2-y2 | -1.152 |
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 |
1.997 |
0.000 |
0.000 |
y |
0.000 |
6.827 |
0.000 |
z |
0.000 |
0.000 |
3.511 |
<r2> (average value of r
2) Å
2
<r2> |
102.994 |
(<r2>)1/2 |
10.149 |
Jump to
S1C1
Energy calculated at BLYP/3-21G*
| hartrees |
Energy at 0K | -954.585754 |
Energy at 298.15K | -954.586373 |
HF Energy | -954.585754 |
Nuclear repulsion energy | 123.107267 |
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/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' |
3160 |
3140 |
1.59 |
|
|
|
2 |
A' |
701 |
696 |
17.70 |
|
|
|
3 |
A' |
381 |
378 |
41.48 |
|
|
|
4 |
A' |
292 |
290 |
1.21 |
|
|
|
5 |
A" |
1228 |
1220 |
28.77 |
|
|
|
6 |
A" |
779 |
774 |
191.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3270.6 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 3249.3 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/3-21G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
0.707 |
0.000 |
H2 |
-0.462 |
1.686 |
0.000 |
Cl3 |
0.012 |
-0.174 |
1.503 |
Cl4 |
0.012 |
-0.174 |
-1.503 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0875 | 1.7427 | 1.7427 |
H2 | 1.0875 | | 2.4384 | 2.4384 | Cl3 | 1.7427 | 2.4384 | | 3.0067 | Cl4 | 1.7427 | 2.4384 | 3.0067 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
117.089 |
|
Cl3 |
C1 |
Cl4 |
119.231 |
Cl4 |
C1 |
H2 |
117.089 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.388 |
|
|
|
2 |
H |
0.254 |
|
|
|
3 |
Cl |
0.067 |
|
|
|
4 |
Cl |
0.067 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.583 |
0.822 |
0.000 |
1.007 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.775 |
-0.956 |
0.000 |
y |
-0.956 |
-29.367 |
0.000 |
z |
0.000 |
0.000 |
-31.050 |
|
Traceless |
| x | y | z |
x |
-1.567 |
-0.956 |
0.000 |
y |
-0.956 |
2.045 |
0.000 |
z |
0.000 |
0.000 |
-0.478 |
|
Polar |
3z2-r2 | -0.957 |
x2-y2 | -2.408 |
xy | -0.956 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.096 |
-0.214 |
0.000 |
y |
-0.214 |
3.527 |
0.000 |
z |
0.000 |
0.000 |
6.928 |
<r2> (average value of r
2) Å
2
<r2> |
103.131 |
(<r2>)1/2 |
10.155 |