Jump to
S1C2
Energy calculated at wB97X-D/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -499.461489 |
| Energy at 298.15K | |
| HF Energy | -499.461489 |
| Nuclear repulsion energy | 45.478966 |
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/daug-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' |
3188 |
3188 |
6.58 |
116.47 |
0.07 |
0.13 |
| 2 |
A' |
1417 |
1417 |
8.90 |
1.09 |
0.68 |
0.81 |
| 3 |
A' |
849 |
849 |
33.50 |
7.42 |
0.08 |
0.14 |
| 4 |
A' |
199 |
199 |
69.82 |
0.59 |
0.75 |
0.86 |
| 5 |
A" |
3339 |
3339 |
0.16 |
44.66 |
0.75 |
0.86 |
| 6 |
A" |
999 |
999 |
0.04 |
0.98 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4995.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4995.8 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/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
1.115 |
0.000 |
| Cl2 |
0.000 |
-0.583 |
0.000 |
| H3 |
-0.000 |
1.615 |
0.952 |
| H4 |
-0.000 |
1.615 |
-0.952 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.6980 | 1.0757 | 1.0757 |
Cl2 | 1.6980 | | 2.3958 | 2.3958 | H3 | 1.0757 | 2.3958 | | 1.9044 | H4 | 1.0757 | 2.3958 | 1.9044 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.727 |
|
Br2 |
C1 |
H4 |
117.727 |
| H3 |
C1 |
H4 |
124.545 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-1.099 |
|
|
|
| 2 |
Cl |
-0.281 |
|
|
|
| 3 |
H |
0.690 |
|
|
|
| 4 |
H |
0.690 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.000 |
1.127 |
0.000 |
1.127 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.473 |
-0.000 |
0.000 |
| y |
-0.000 |
-17.299 |
0.000 |
| z |
0.000 |
0.000 |
-18.427 |
|
| Traceless |
| | x | y | z |
| x |
-2.610 |
-0.000 |
0.000 |
| y |
-0.000 |
2.151 |
0.000 |
| z |
0.000 |
0.000 |
0.459 |
|
| Polar |
| 3z2-r2 | 0.918 |
| x2-y2 | -3.174 |
| 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 |
3.629 |
0.000 |
0.000 |
| y |
0.000 |
5.396 |
0.000 |
| z |
0.000 |
0.000 |
3.770 |
<r2> (average value of r
2) Å
2
| <r2> |
31.971 |
| (<r2>)1/2 |
5.654 |
Jump to
S1C1
Energy calculated at wB97X-D/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -499.461489 |
| Energy at 298.15K | |
| HF Energy | -499.461489 |
| Nuclear repulsion energy | 45.485818 |
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/daug-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 |
3188 |
3188 |
6.61 |
116.59 |
0.07 |
0.13 |
| 2 |
A1 |
1418 |
1418 |
8.92 |
|
|
|
| 3 |
A1 |
850 |
850 |
33.43 |
|
|
|
| 4 |
B1 |
204 |
204 |
69.77 |
|
|
|
| 5 |
B2 |
3337 |
3337 |
0.15 |
|
|
|
| 6 |
B2 |
999 |
999 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4998.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4998.2 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 wB97X-D/daug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.114 |
| Cl2 |
0.000 |
0.000 |
0.583 |
| H3 |
0.000 |
0.952 |
-1.616 |
| H4 |
0.000 |
-0.952 |
-1.616 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.6976 | 1.0758 | 1.0758 |
Cl2 | 1.6976 | | 2.3961 | 2.3961 | H3 | 1.0758 | 2.3961 | | 1.9036 | H4 | 1.0758 | 2.3961 | 1.9036 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.778 |
|
Br2 |
C1 |
H4 |
117.778 |
| H3 |
C1 |
H4 |
124.445 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-1.099 |
|
|
|
| 2 |
Cl |
-0.281 |
|
|
|
| 3 |
H |
0.690 |
|
|
|
| 4 |
H |
0.690 |
|
|
|
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 |
-1.126 |
1.126 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.472 |
0.000 |
0.000 |
| y |
0.000 |
-18.430 |
0.000 |
| z |
0.000 |
0.000 |
-17.297 |
|
| Traceless |
| | x | y | z |
| x |
-2.609 |
0.000 |
0.000 |
| y |
0.000 |
0.455 |
0.000 |
| z |
0.000 |
0.000 |
2.154 |
|
| Polar |
| 3z2-r2 | 4.308 |
| x2-y2 | -2.043 |
| 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 |
3.629 |
0.000 |
0.000 |
| y |
0.000 |
3.770 |
0.000 |
| z |
0.000 |
0.000 |
5.395 |
<r2> (average value of r
2) Å
2
| <r2> |
31.966 |
| (<r2>)1/2 |
5.654 |