Jump to
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -959.039071 |
| Energy at 298.15K | |
| HF Energy | -959.039071 |
| Nuclear repulsion energy | 122.100798 |
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 |
3356 |
3201 |
0.77 |
|
|
|
| 2 |
A1 |
707 |
675 |
14.61 |
|
|
|
| 3 |
A1 |
298 |
284 |
0.70 |
|
|
|
| 4 |
B1 |
353i |
337i |
98.86 |
|
|
|
| 5 |
B2 |
1242 |
1185 |
54.06 |
|
|
|
| 6 |
B2 |
885 |
844 |
166.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3067.5 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 2925.4 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 |
0.697 |
| H2 |
0.000 |
0.000 |
1.771 |
| Cl3 |
0.000 |
1.521 |
-0.175 |
| Cl4 |
0.000 |
-1.521 |
-0.175 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0746 | 1.7529 | 1.7529 |
H2 | 1.0746 | | 2.4700 | 2.4700 | Cl3 | 1.7529 | 2.4700 | | 3.0417 | Cl4 | 1.7529 | 2.4700 | 3.0417 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.818 |
|
Cl3 |
C1 |
Cl4 |
120.365 |
| Cl4 |
C1 |
H2 |
119.818 |
|
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 |
-0.525 |
|
|
|
| 2 |
H |
0.256 |
|
|
|
| 3 |
Cl |
0.134 |
|
|
|
| 4 |
Cl |
0.134 |
|
|
|
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 |
1.260 |
1.260 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.918 |
0.000 |
0.000 |
| y |
0.000 |
-32.173 |
0.000 |
| z |
0.000 |
0.000 |
-28.691 |
|
| Traceless |
| | x | y | z |
| x |
-1.486 |
0.000 |
0.000 |
| y |
0.000 |
-1.868 |
0.000 |
| z |
0.000 |
0.000 |
3.354 |
|
| Polar |
| 3z2-r2 | 6.708 |
| x2-y2 | 0.255 |
| 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 |
1.605 |
0.000 |
0.000 |
| y |
0.000 |
6.632 |
0.000 |
| z |
0.000 |
0.000 |
3.212 |
<r2> (average value of r
2) Å
2
| <r2> |
105.050 |
| (<r2>)1/2 |
10.249 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -959.039849 |
| Energy at 298.15K | -959.040578 |
| HF Energy | -959.039849 |
| Nuclear repulsion energy | 121.815867 |
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' |
3309 |
3155 |
1.12 |
|
|
|
| 2 |
A' |
721 |
687 |
25.57 |
|
|
|
| 3 |
A' |
463 |
442 |
39.74 |
|
|
|
| 4 |
A' |
293 |
279 |
0.91 |
|
|
|
| 5 |
A" |
1254 |
1196 |
42.38 |
|
|
|
| 6 |
A" |
849 |
810 |
191.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3443.9 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 3284.4 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 |
0.012 |
0.722 |
0.000 |
| H2 |
-0.486 |
1.678 |
0.000 |
| Cl3 |
0.012 |
-0.177 |
1.519 |
| Cl4 |
0.012 |
-0.177 |
-1.519 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0784 | 1.7646 | 1.7646 |
H2 | 1.0784 | | 2.4484 | 2.4484 | Cl3 | 1.7646 | 2.4484 | | 3.0376 | Cl4 | 1.7646 | 2.4484 | 3.0376 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.835 |
|
Cl3 |
C1 |
Cl4 |
118.795 |
| Cl4 |
C1 |
H2 |
116.835 |
|
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 |
-0.489 |
|
|
|
| 2 |
H |
0.252 |
|
|
|
| 3 |
Cl |
0.119 |
|
|
|
| 4 |
Cl |
0.119 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.683 |
1.167 |
0.000 |
1.353 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.610 |
-1.049 |
0.000 |
| y |
-1.049 |
-29.217 |
0.000 |
| z |
0.000 |
0.000 |
-32.429 |
|
| Traceless |
| | x | y | z |
| x |
-0.788 |
-1.049 |
0.000 |
| y |
-1.049 |
2.803 |
0.000 |
| z |
0.000 |
0.000 |
-2.015 |
|
| Polar |
| 3z2-r2 | -4.030 |
| x2-y2 | -2.393 |
| xy | -1.049 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.704 |
-0.208 |
0.000 |
| y |
-0.208 |
3.237 |
0.000 |
| z |
0.000 |
0.000 |
6.731 |
<r2> (average value of r
2) Å
2
| <r2> |
105.090 |
| (<r2>)1/2 |
10.251 |