Jump to
S1C2
Energy calculated at B3PW91/6-311G**
| hartrees |
Energy at 0K | -958.977526 |
Energy at 298.15K | |
HF Energy | -958.977526 |
Nuclear repulsion energy | 125.638478 |
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 B3PW91/6-311G**
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 |
3271 |
3151 |
0.00 |
|
|
|
2 |
A1 |
757 |
730 |
8.56 |
|
|
|
3 |
A1 |
317 |
305 |
0.14 |
|
|
|
4 |
B1 |
330i |
317i |
60.68 |
|
|
|
5 |
B2 |
1250 |
1204 |
47.31 |
|
|
|
6 |
B2 |
924 |
890 |
177.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3095.1 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 2980.9 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 B3PW91/6-311G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.669 |
H2 |
0.000 |
0.000 |
1.746 |
Cl3 |
0.000 |
1.478 |
-0.169 |
Cl4 |
0.000 |
-1.478 |
-0.169 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0774 | 1.6993 | 1.6993 |
H2 | 1.0774 | | 2.4197 | 2.4197 | Cl3 | 1.6993 | 2.4197 | | 2.9564 | Cl4 | 1.6993 | 2.4197 | 2.9564 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
119.559 |
|
Cl3 |
C1 |
Cl4 |
120.883 |
Cl4 |
C1 |
H2 |
119.559 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.301 |
|
|
|
2 |
H |
0.224 |
|
|
|
3 |
Cl |
0.038 |
|
|
|
4 |
Cl |
0.038 |
|
|
|
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 |
0.961 |
0.961 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.328 |
0.000 |
0.000 |
y |
0.000 |
-31.385 |
0.000 |
z |
0.000 |
0.000 |
-29.231 |
|
Traceless |
| x | y | z |
x |
-2.020 |
0.000 |
0.000 |
y |
0.000 |
-0.605 |
0.000 |
z |
0.000 |
0.000 |
2.625 |
|
Polar |
3z2-r2 | 5.250 |
x2-y2 | -0.943 |
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 |
2.222 |
0.000 |
0.000 |
y |
0.000 |
6.972 |
0.000 |
z |
0.000 |
0.000 |
3.663 |
<r2> (average value of r
2) Å
2
<r2> |
100.351 |
(<r2>)1/2 |
10.018 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G**
| hartrees |
Energy at 0K | -958.978077 |
Energy at 298.15K | -958.978847 |
HF Energy | -958.978077 |
Nuclear repulsion energy | 125.483869 |
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 B3PW91/6-311G**
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' |
3237 |
3118 |
1.60 |
|
|
|
2 |
A' |
762 |
734 |
13.28 |
|
|
|
3 |
A' |
442 |
426 |
35.34 |
|
|
|
4 |
A' |
310 |
299 |
1.18 |
|
|
|
5 |
A" |
1256 |
1210 |
40.90 |
|
|
|
6 |
A" |
896 |
863 |
200.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3452.1 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 3324.7 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 B3PW91/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.011 |
0.689 |
0.000 |
H2 |
-0.448 |
1.666 |
0.000 |
Cl3 |
0.011 |
-0.171 |
1.476 |
Cl4 |
0.011 |
-0.171 |
-1.476 |
Atom - Atom Distances (Å)
|
C1 |
H2 |
Cl3 |
Cl4 |
C1 | | 1.0802 | 1.7074 | 1.7074 |
H2 | 1.0802 | | 2.4004 | 2.4004 | Cl3 | 1.7074 | 2.4004 | | 2.9510 | Cl4 | 1.7074 | 2.4004 | 2.9510 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl3 |
C1 |
H2 |
117.087 |
|
Cl3 |
C1 |
Cl4 |
119.580 |
Cl4 |
C1 |
H2 |
117.087 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.284 |
|
|
|
2 |
H |
0.221 |
|
|
|
3 |
Cl |
0.032 |
|
|
|
4 |
Cl |
0.032 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.508 |
0.880 |
0.000 |
1.016 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.069 |
-0.879 |
0.000 |
y |
-0.879 |
-29.632 |
0.000 |
z |
0.000 |
0.000 |
-31.540 |
|
Traceless |
| x | y | z |
x |
-1.483 |
-0.879 |
0.000 |
y |
-0.879 |
2.173 |
0.000 |
z |
0.000 |
0.000 |
-0.689 |
|
Polar |
3z2-r2 | -1.379 |
x2-y2 | -2.438 |
xy | -0.879 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.297 |
-0.144 |
0.000 |
y |
-0.144 |
3.687 |
0.000 |
z |
0.000 |
0.000 |
7.041 |
<r2> (average value of r
2) Å
2
<r2> |
100.251 |
(<r2>)1/2 |
10.013 |