Jump to
S1C2
Energy calculated at B3LYPultrafine/6-311G*
| hartrees |
Energy at 0K | -959.098802 |
Energy at 298.15K | |
HF Energy | -959.098802 |
Nuclear repulsion energy | 124.934037 |
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 B3LYPultrafine/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 |
3260 |
3150 |
0.28 |
|
|
|
2 |
A1 |
740 |
715 |
8.52 |
|
|
|
3 |
A1 |
312 |
302 |
0.14 |
|
|
|
4 |
B1 |
365i |
353i |
62.42 |
|
|
|
5 |
B2 |
1256 |
1214 |
48.28 |
|
|
|
6 |
B2 |
897 |
866 |
179.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3049.8 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 2947.0 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 B3LYPultrafine/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 |
1.748 |
Cl3 |
0.000 |
1.488 |
-0.170 |
Cl4 |
0.000 |
-1.488 |
-0.170 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0770 | 1.7090 | 1.7090 |
H2 | 1.0770 | | 2.4275 | 2.4275 | Cl3 | 1.7090 | 2.4275 | | 2.9750 | Cl4 | 1.7090 | 2.4275 | 2.9750 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.493 |
|
Cl3 |
C1 |
Cl4 |
121.015 |
Cl4 |
C1 |
H2 |
119.493 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/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 |
-32.594 |
0.000 |
0.000 |
y |
0.000 |
-31.692 |
0.000 |
z |
0.000 |
0.000 |
-29.459 |
|
Traceless |
| x | y | z |
x |
-2.018 |
0.000 |
0.000 |
y |
0.000 |
-0.666 |
0.000 |
z |
0.000 |
0.000 |
2.684 |
|
Polar |
3z2-r2 | 5.368 |
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 |
7.098 |
0.000 |
z |
0.000 |
0.000 |
3.673 |
<r2> (average value of r
2) Å
2
<r2> |
101.492 |
(<r2>)1/2 |
10.074 |
Jump to
S1C1
Energy calculated at B3LYPultrafine/6-311G*
| hartrees |
Energy at 0K | -959.099633 |
Energy at 298.15K | -959.100411 |
HF Energy | -959.099633 |
Nuclear repulsion energy | 124.721610 |
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 B3LYPultrafine/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' |
3222 |
3113 |
3.03 |
|
|
|
2 |
A' |
748 |
723 |
15.26 |
|
|
|
3 |
A' |
481 |
464 |
31.98 |
|
|
|
4 |
A' |
306 |
296 |
0.59 |
|
|
|
5 |
A" |
1265 |
1222 |
40.26 |
|
|
|
6 |
A" |
862 |
833 |
208.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3441.7 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 3325.7 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 B3LYPultrafine/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.012 |
0.696 |
0.000 |
H2 |
-0.490 |
1.653 |
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 | 1.7194 | 1.7194 |
H2 | 1.0802 | | 2.4050 | 2.4050 | Cl3 | 1.7194 | 2.4050 | | 2.9685 | Cl4 | 1.7194 | 2.4050 | 2.9685 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
116.553 |
|
Cl3 |
C1 |
Cl4 |
119.363 |
Cl4 |
C1 |
H2 |
116.553 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/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 |
|
-0.557 |
0.886 |
0.000 |
1.047 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.283 |
-0.952 |
0.000 |
y |
-0.952 |
-29.940 |
0.000 |
z |
0.000 |
0.000 |
-31.885 |
|
Traceless |
| x | y | z |
x |
-1.370 |
-0.952 |
0.000 |
y |
-0.952 |
2.144 |
0.000 |
z |
0.000 |
0.000 |
-0.774 |
|
Polar |
3z2-r2 | -1.547 |
x2-y2 | -2.343 |
xy | -0.952 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.295 |
-0.166 |
0.000 |
y |
-0.166 |
3.705 |
0.000 |
z |
0.000 |
0.000 |
7.191 |
<r2> (average value of r
2) Å
2
<r2> |
101.386 |
(<r2>)1/2 |
10.069 |