Jump to
S1C2
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -958.926137 |
| Energy at 298.15K | |
| HF Energy | -958.926137 |
| Nuclear repulsion energy | 126.056777 |
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 B3PW91/6-31G(2df,p)
| 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 |
3275 |
3149 |
0.42 |
|
|
|
| 2 |
A1 |
762 |
732 |
8.32 |
|
|
|
| 3 |
A1 |
309 |
298 |
0.45 |
|
|
|
| 4 |
B1 |
334i |
321i |
37.97 |
|
|
|
| 5 |
B2 |
1226 |
1178 |
50.36 |
|
|
|
| 6 |
B2 |
935 |
899 |
144.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3086.7 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 2967.5 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 B3PW91/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.668 |
| H2 |
0.000 |
0.000 |
1.747 |
| Cl3 |
0.000 |
1.472 |
-0.169 |
| Cl4 |
0.000 |
-1.472 |
-0.169 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0789 | 1.6937 | 1.6937 |
H2 | 1.0789 | | 2.4164 | 2.4164 | Cl3 | 1.6937 | 2.4164 | | 2.9449 | Cl4 | 1.6937 | 2.4164 | 2.9449 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.615 |
|
Cl3 |
C1 |
Cl4 |
120.770 |
| Cl4 |
C1 |
H2 |
119.615 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.135 |
|
|
|
| 2 |
H |
0.205 |
|
|
|
| 3 |
Cl |
-0.035 |
|
|
|
| 4 |
Cl |
-0.035 |
|
|
|
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 |
0.967 |
0.967 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.403 |
0.000 |
0.000 |
| y |
0.000 |
-30.535 |
0.000 |
| z |
0.000 |
0.000 |
-28.454 |
|
| Traceless |
| | x | y | z |
| x |
-1.909 |
0.000 |
0.000 |
| y |
0.000 |
-0.607 |
0.000 |
| z |
0.000 |
0.000 |
2.515 |
|
| Polar |
| 3z2-r2 | 5.031 |
| x2-y2 | -0.868 |
| 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 |
3.178 |
0.000 |
0.000 |
| y |
0.000 |
7.124 |
0.000 |
| z |
0.000 |
0.000 |
4.305 |
<r2> (average value of r
2) Å
2
| <r2> |
99.235 |
| (<r2>)1/2 |
9.962 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -958.926711 |
| Energy at 298.15K | -958.927474 |
| HF Energy | -958.926711 |
| Nuclear repulsion energy | 125.902667 |
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 B3PW91/6-31G(2df,p)
| 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' |
3239 |
3114 |
1.20 |
|
|
|
| 2 |
A' |
767 |
738 |
12.47 |
|
|
|
| 3 |
A' |
447 |
430 |
23.67 |
|
|
|
| 4 |
A' |
302 |
291 |
0.84 |
|
|
|
| 5 |
A" |
1229 |
1182 |
42.85 |
|
|
|
| 6 |
A" |
908 |
873 |
165.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3445.9 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 3312.9 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 B3PW91/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.689 |
0.000 |
| H2 |
-0.453 |
1.667 |
0.000 |
| Cl3 |
0.011 |
-0.171 |
1.469 |
| Cl4 |
0.011 |
-0.171 |
-1.469 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0820 | 1.7023 | 1.7023 |
H2 | 1.0820 | | 2.3978 | 2.3978 | Cl3 | 1.7023 | 2.3978 | | 2.9383 | Cl4 | 1.7023 | 2.3978 | 2.9383 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.151 |
|
Cl3 |
C1 |
Cl4 |
119.319 |
| Cl4 |
C1 |
H2 |
117.151 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.130 |
|
|
|
| 2 |
H |
0.204 |
|
|
|
| 3 |
Cl |
-0.037 |
|
|
|
| 4 |
Cl |
-0.037 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.422 |
0.885 |
0.000 |
0.981 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.176 |
-0.802 |
0.000 |
| y |
-0.802 |
-28.823 |
0.000 |
| z |
0.000 |
0.000 |
-30.630 |
|
| Traceless |
| | x | y | z |
| x |
-1.449 |
-0.802 |
0.000 |
| y |
-0.802 |
2.080 |
0.000 |
| z |
0.000 |
0.000 |
-0.631 |
|
| Polar |
| 3z2-r2 | -1.262 |
| x2-y2 | -2.352 |
| xy | -0.802 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.251 |
-0.159 |
0.000 |
| y |
-0.159 |
4.315 |
0.000 |
| z |
0.000 |
0.000 |
7.192 |
<r2> (average value of r
2) Å
2
| <r2> |
99.081 |
| (<r2>)1/2 |
9.954 |