Jump to
S1C2
Energy calculated at wB97X-D/LANL2DZ
| hartrees |
Energy at 0K | -54.165380 |
Energy at 298.15K | |
HF Energy | -54.165380 |
Nuclear repulsion energy | 21.693971 |
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 wB97X-D/LANL2DZ
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' |
3226 |
3226 |
8.49 |
116.16 |
0.13 |
0.23 |
2 |
A' |
1415 |
1415 |
8.33 |
1.13 |
0.65 |
0.79 |
3 |
A' |
786 |
786 |
44.85 |
14.44 |
0.34 |
0.51 |
4 |
A' |
214 |
214 |
162.82 |
0.00 |
0.74 |
0.85 |
5 |
A" |
3412 |
3412 |
2.61 |
32.67 |
0.75 |
0.86 |
6 |
A" |
1004 |
1004 |
0.46 |
6.15 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5028.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5028.5 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 wB97X-D/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.000 |
1.168 |
0.000 |
Cl2 |
-0.000 |
-0.607 |
0.000 |
H3 |
0.000 |
1.653 |
0.965 |
H4 |
0.000 |
1.653 |
-0.965 |
Atom - Atom Distances (Å)
|
C1 |
Cl2 |
H3 |
H4 |
C1 | | 1.7748 | 1.0797 | 1.0797 |
Cl2 | 1.7748 | | 2.4569 | 2.4569 | H3 | 1.0797 | 2.4569 | | 1.9295 | H4 | 1.0797 | 2.4569 | 1.9295 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
H3 |
116.683 |
|
Br2 |
C1 |
H4 |
116.683 |
H3 |
C1 |
H4 |
126.634 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.493 |
|
|
|
2 |
Cl |
-0.028 |
|
|
|
3 |
H |
0.261 |
|
|
|
4 |
H |
0.261 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.001 |
1.718 |
0.000 |
1.718 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.894 |
0.001 |
0.000 |
y |
0.001 |
-16.366 |
0.000 |
z |
0.000 |
0.000 |
-17.443 |
|
Traceless |
| x | y | z |
x |
-2.990 |
0.001 |
0.000 |
y |
0.001 |
2.303 |
0.000 |
z |
0.000 |
0.000 |
0.687 |
|
Polar |
3z2-r2 | 1.375 |
x2-y2 | -3.529 |
xy | 0.001 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.915 |
0.000 |
0.000 |
y |
0.000 |
4.101 |
0.000 |
z |
0.000 |
0.000 |
1.586 |
<r2> (average value of r
2) Å
2
<r2> |
29.269 |
(<r2>)1/2 |
5.410 |
Jump to
S1C1
Energy calculated at wB97X-D/LANL2DZ
| hartrees |
Energy at 0K | -54.165380 |
Energy at 298.15K | |
HF Energy | -54.165380 |
Nuclear repulsion energy | 21.691629 |
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 wB97X-D/LANL2DZ
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 |
3226 |
3226 |
8.48 |
116.19 |
0.13 |
0.23 |
2 |
A1 |
1415 |
1415 |
8.35 |
|
|
|
3 |
A1 |
786 |
786 |
44.81 |
|
|
|
4 |
B1 |
215 |
215 |
162.76 |
|
|
|
5 |
B2 |
3411 |
3411 |
2.62 |
|
|
|
6 |
B2 |
1004 |
1004 |
0.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5028.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5028.3 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 wB97X-D/LANL2DZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
-1.168 |
Cl2 |
0.000 |
0.000 |
0.607 |
H3 |
0.000 |
0.965 |
-1.653 |
H4 |
0.000 |
-0.965 |
-1.653 |
Atom - Atom Distances (Å)
|
C1 |
Cl2 |
H3 |
H4 |
C1 | | 1.7750 | 1.0798 | 1.0798 |
Cl2 | 1.7750 | | 2.4574 | 2.4574 | H3 | 1.0798 | 2.4574 | | 1.9292 | H4 | 1.0798 | 2.4574 | 1.9292 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
H3 |
116.701 |
|
Br2 |
C1 |
H4 |
116.701 |
H3 |
C1 |
H4 |
126.599 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.493 |
|
|
|
2 |
Cl |
-0.028 |
|
|
|
3 |
H |
0.261 |
|
|
|
4 |
H |
0.261 |
|
|
|
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 |
-1.718 |
1.718 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.895 |
0.000 |
0.000 |
y |
0.000 |
-17.444 |
0.000 |
z |
0.000 |
0.000 |
-16.363 |
|
Traceless |
| x | y | z |
x |
-2.992 |
0.000 |
0.000 |
y |
0.000 |
0.685 |
0.000 |
z |
0.000 |
0.000 |
2.307 |
|
Polar |
3z2-r2 | 4.613 |
x2-y2 | -2.451 |
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 |
0.915 |
0.000 |
0.000 |
y |
0.000 |
1.586 |
0.000 |
z |
0.000 |
0.000 |
4.102 |
<r2> (average value of r
2) Å
2
<r2> |
29.274 |
(<r2>)1/2 |
5.411 |