Jump to
S1C2
Energy calculated at B1B95/6-31G**
| | hartrees |
| Energy at 0K | -959.097039 |
| Energy at 298.15K | |
| HF Energy | -959.097039 |
| Nuclear repulsion energy | 126.098767 |
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 B1B95/6-31G**
| 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 |
3316 |
3166 |
0.06 |
|
|
|
| 2 |
A1 |
778 |
742 |
10.34 |
|
|
|
| 3 |
A1 |
319 |
305 |
0.40 |
|
|
|
| 4 |
B1 |
340i |
324i |
61.23 |
|
|
|
| 5 |
B2 |
1275 |
1218 |
56.58 |
|
|
|
| 6 |
B2 |
958 |
915 |
162.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3153.0 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 3010.5 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 B1B95/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.665 |
| H2 |
0.000 |
0.000 |
1.742 |
| Cl3 |
0.000 |
1.473 |
-0.169 |
| Cl4 |
0.000 |
-1.473 |
-0.169 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0778 | 1.6924 | 1.6924 |
H2 | 1.0778 | | 2.4128 | 2.4128 | Cl3 | 1.6924 | 2.4128 | | 2.9461 | Cl4 | 1.6924 | 2.4128 | 2.9461 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.494 |
|
Cl3 |
C1 |
Cl4 |
121.012 |
| Cl4 |
C1 |
H2 |
119.494 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.394 |
|
|
|
| 2 |
H |
0.250 |
|
|
|
| 3 |
Cl |
0.072 |
|
|
|
| 4 |
Cl |
0.072 |
|
|
|
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 |
0.971 |
0.971 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.550 |
0.000 |
0.000 |
| y |
0.000 |
-30.694 |
0.000 |
| z |
0.000 |
0.000 |
-28.557 |
|
| Traceless |
| | x | y | z |
| x |
-1.925 |
0.000 |
0.000 |
| y |
0.000 |
-0.640 |
0.000 |
| z |
0.000 |
0.000 |
2.565 |
|
| Polar |
| 3z2-r2 | 5.130 |
| x2-y2 | -0.856 |
| 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 |
2.248 |
0.000 |
0.000 |
| y |
0.000 |
6.516 |
0.000 |
| z |
0.000 |
0.000 |
3.623 |
<r2> (average value of r
2) Å
2
| <r2> |
99.335 |
| (<r2>)1/2 |
9.967 |
Jump to
S1C1
Energy calculated at B1B95/6-31G**
| | hartrees |
| Energy at 0K | -959.097642 |
| Energy at 298.15K | -959.098435 |
| HF Energy | -959.097642 |
| Nuclear repulsion energy | 125.955125 |
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 B1B95/6-31G**
| 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' |
3278 |
3130 |
1.76 |
|
|
|
| 2 |
A' |
782 |
747 |
15.61 |
|
|
|
| 3 |
A' |
457 |
437 |
33.69 |
|
|
|
| 4 |
A' |
311 |
297 |
1.23 |
|
|
|
| 5 |
A" |
1281 |
1223 |
48.11 |
|
|
|
| 6 |
A" |
930 |
888 |
185.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3519.7 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 3360.6 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 B1B95/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.686 |
0.000 |
| H2 |
-0.453 |
1.662 |
0.000 |
| Cl3 |
0.011 |
-0.170 |
1.470 |
| Cl4 |
0.011 |
-0.170 |
-1.470 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0806 | 1.7008 | 1.7008 |
H2 | 1.0806 | | 2.3938 | 2.3938 | Cl3 | 1.7008 | 2.3938 | | 2.9394 | Cl4 | 1.7008 | 2.3938 | 2.9394 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.026 |
|
Cl3 |
C1 |
Cl4 |
119.571 |
| Cl4 |
C1 |
H2 |
117.026 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.373 |
|
|
|
| 2 |
H |
0.245 |
|
|
|
| 3 |
Cl |
0.064 |
|
|
|
| 4 |
Cl |
0.064 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.511 |
0.885 |
0.000 |
1.022 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.298 |
-0.875 |
0.000 |
| y |
-0.875 |
-28.974 |
0.000 |
| z |
0.000 |
0.000 |
-30.842 |
|
| Traceless |
| | x | y | z |
| x |
-1.390 |
-0.875 |
0.000 |
| y |
-0.875 |
2.096 |
0.000 |
| z |
0.000 |
0.000 |
-0.706 |
|
| Polar |
| 3z2-r2 | -1.412 |
| x2-y2 | -2.324 |
| xy | -0.875 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.336 |
-0.189 |
0.000 |
| y |
-0.189 |
3.624 |
0.000 |
| z |
0.000 |
0.000 |
6.576 |
<r2> (average value of r
2) Å
2
| <r2> |
99.188 |
| (<r2>)1/2 |
9.959 |