Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -958.833285 |
| Energy at 298.15K | |
| HF Energy | -958.631461 |
| Nuclear repulsion energy | 126.037211 |
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 B2PLYP=FULLultrafine/aug-cc-pVTZ
| 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 |
3297 |
3162 |
0.88 |
|
|
|
| 2 |
A1 |
756 |
725 |
6.12 |
|
|
|
| 3 |
A1 |
310 |
298 |
0.33 |
|
|
|
| 4 |
B1 |
365i |
350i |
35.19 |
|
|
|
| 5 |
B2 |
1240 |
1190 |
50.23 |
|
|
|
| 6 |
B2 |
921 |
884 |
141.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3079.8 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 2953.9 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
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 |
1.742 |
| Cl3 |
0.000 |
1.472 |
-0.170 |
| Cl4 |
0.000 |
-1.472 |
-0.170 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0709 | 1.6954 | 1.6954 |
H2 | 1.0709 | | 2.4129 | 2.4129 | Cl3 | 1.6954 | 2.4129 | | 2.9443 | Cl4 | 1.6954 | 2.4129 | 2.9443 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.735 |
|
Cl3 |
C1 |
Cl4 |
120.530 |
| Cl4 |
C1 |
H2 |
119.735 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.334 |
|
|
|
| 2 |
H |
0.376 |
|
|
|
| 3 |
Cl |
-0.021 |
|
|
|
| 4 |
Cl |
-0.021 |
|
|
|
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 |
0.909 |
0.909 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.163 |
0.000 |
0.000 |
| y |
0.000 |
-31.292 |
0.000 |
| z |
0.000 |
0.000 |
-29.286 |
|
| Traceless |
| | x | y | z |
| x |
-1.874 |
0.000 |
0.000 |
| y |
0.000 |
-0.568 |
0.000 |
| z |
0.000 |
0.000 |
2.442 |
|
| Polar |
| 3z2-r2 | 4.883 |
| x2-y2 | -0.871 |
| 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 |
4.756 |
0.000 |
0.000 |
| y |
0.000 |
8.333 |
0.000 |
| z |
0.000 |
0.000 |
5.571 |
<r2> (average value of r
2) Å
2
| <r2> |
99.711 |
| (<r2>)1/2 |
9.986 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -958.834014 |
| Energy at 298.15K | |
| HF Energy | -958.632316 |
| Nuclear repulsion energy | 125.850366 |
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 B2PLYP=FULLultrafine/aug-cc-pVTZ
| 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' |
3258 |
3125 |
0.52 |
|
|
|
| 2 |
A' |
763 |
732 |
10.72 |
|
|
|
| 3 |
A' |
478 |
458 |
21.49 |
|
|
|
| 4 |
A' |
304 |
292 |
0.52 |
|
|
|
| 5 |
A" |
1246 |
1195 |
40.99 |
|
|
|
| 6 |
A" |
891 |
855 |
164.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3470.2 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 3328.2 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.694 |
0.000 |
| H2 |
-0.466 |
1.656 |
0.000 |
| Cl3 |
0.012 |
-0.171 |
1.469 |
| Cl4 |
0.012 |
-0.171 |
-1.469 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0741 | 1.7048 | 1.7048 |
H2 | 1.0741 | | 2.3926 | 2.3926 | Cl3 | 1.7048 | 2.3926 | | 2.9381 | Cl4 | 1.7048 | 2.3926 | 2.9381 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
117.034 |
|
Cl3 |
C1 |
Cl4 |
119.023 |
| Cl4 |
C1 |
H2 |
117.034 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.321 |
|
|
|
| 2 |
H |
0.355 |
|
|
|
| 3 |
Cl |
-0.017 |
|
|
|
| 4 |
Cl |
-0.017 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.418 |
0.831 |
0.000 |
0.931 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.911 |
-0.857 |
0.001 |
| y |
-0.857 |
-29.675 |
0.004 |
| z |
0.001 |
0.004 |
-31.375 |
|
| Traceless |
| | x | y | z |
| x |
-1.386 |
-0.857 |
0.001 |
| y |
-0.857 |
1.968 |
0.004 |
| z |
0.001 |
0.004 |
-0.582 |
|
| Polar |
| 3z2-r2 | -1.164 |
| x2-y2 | -2.236 |
| xy | -0.857 |
| xz | 0.001 |
| yz | 0.004 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.792 |
-0.051 |
-0.000 |
| y |
-0.051 |
5.606 |
0.001 |
| z |
-0.000 |
0.001 |
8.410 |
<r2> (average value of r
2) Å
2
| <r2> |
99.580 |
| (<r2>)1/2 |
9.979 |