Jump to
S1C2
Energy calculated at LSDA/6-31G*
| hartrees |
Energy at 0K | -956.504917 |
Energy at 298.15K | |
HF Energy | -956.504917 |
Nuclear repulsion energy | 126.434085 |
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 LSDA/6-31G*
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 |
3218 |
3158 |
0.75 |
|
|
|
2 |
A1 |
774 |
760 |
7.45 |
|
|
|
3 |
A1 |
315 |
309 |
0.27 |
|
|
|
4 |
B1 |
232i |
227i |
70.26 |
|
|
|
5 |
B2 |
1223 |
1200 |
42.53 |
|
|
|
6 |
B2 |
951 |
933 |
158.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3124.7 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 3066.3 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 LSDA/6-31G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.662 |
H2 |
0.000 |
0.000 |
1.752 |
Cl3 |
0.000 |
1.468 |
-0.168 |
Cl4 |
0.000 |
-1.468 |
-0.168 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0893 | 1.6870 | 1.6870 |
H2 | 1.0893 | | 2.4171 | 2.4171 | Cl3 | 1.6870 | 2.4171 | | 2.9363 | Cl4 | 1.6870 | 2.4171 | 2.9363 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.507 |
|
Cl3 |
C1 |
Cl4 |
120.985 |
Cl4 |
C1 |
H2 |
119.507 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.432 |
|
|
|
2 |
H |
0.253 |
|
|
|
3 |
Cl |
0.090 |
|
|
|
4 |
Cl |
0.090 |
|
|
|
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 |
0.872 |
0.872 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.682 |
0.000 |
0.000 |
y |
0.000 |
-30.487 |
0.000 |
z |
0.000 |
0.000 |
-28.675 |
|
Traceless |
| x | y | z |
x |
-2.101 |
0.000 |
0.000 |
y |
0.000 |
-0.309 |
0.000 |
z |
0.000 |
0.000 |
2.409 |
|
Polar |
3z2-r2 | 4.819 |
x2-y2 | -1.194 |
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 |
2.273 |
0.000 |
0.000 |
y |
0.000 |
6.811 |
0.000 |
z |
0.000 |
0.000 |
3.704 |
<r2> (average value of r
2) Å
2
<r2> |
98.865 |
(<r2>)1/2 |
9.943 |
Jump to
S1C1
Energy calculated at LSDA/6-31G*
| hartrees |
Energy at 0K | -956.505090 |
Energy at 298.15K | -956.505732 |
HF Energy | -956.505090 |
Nuclear repulsion energy | 126.350490 |
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 LSDA/6-31G*
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' |
3195 |
3136 |
0.87 |
|
|
|
2 |
A' |
776 |
761 |
10.08 |
|
|
|
3 |
A' |
342 |
336 |
31.08 |
|
|
|
4 |
A' |
290 |
284 |
23.15 |
|
|
|
5 |
A" |
1225 |
1202 |
37.97 |
|
|
|
6 |
A" |
934 |
916 |
172.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3380.8 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 3317.6 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 LSDA/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.009 |
0.675 |
0.000 |
H2 |
-0.358 |
1.703 |
0.000 |
Cl3 |
0.009 |
-0.169 |
1.466 |
Cl4 |
0.009 |
-0.169 |
-1.466 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0910 | 1.6919 | 1.6919 |
H2 | 1.0910 | | 2.4058 | 2.4058 | Cl3 | 1.6919 | 2.4058 | | 2.9322 | Cl4 | 1.6919 | 2.4058 | 2.9322 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
118.034 |
|
Cl3 |
C1 |
Cl4 |
120.120 |
Cl4 |
C1 |
H2 |
118.034 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.422 |
|
|
|
2 |
H |
0.251 |
|
|
|
3 |
Cl |
0.085 |
|
|
|
4 |
Cl |
0.085 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.435 |
0.809 |
0.000 |
0.918 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.517 |
-0.762 |
0.000 |
y |
-0.762 |
-28.952 |
0.000 |
z |
0.000 |
0.000 |
-30.563 |
|
Traceless |
| x | y | z |
x |
-1.760 |
-0.762 |
0.000 |
y |
-0.762 |
2.088 |
0.000 |
z |
0.000 |
0.000 |
-0.328 |
|
Polar |
3z2-r2 | -0.657 |
x2-y2 | -2.565 |
xy | -0.762 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.329 |
-0.158 |
0.000 |
y |
-0.158 |
3.704 |
0.000 |
z |
0.000 |
0.000 |
6.849 |
<r2> (average value of r
2) Å
2
<r2> |
98.773 |
(<r2>)1/2 |
9.938 |