Jump to
S1C2
Energy calculated at B2PLYP/6-31G
| | hartrees |
| Energy at 0K | -499.147804 |
| Energy at 298.15K | |
| HF Energy | -499.108151 |
| Nuclear repulsion energy | 43.639525 |
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/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' |
3245 |
3245 |
3.19 |
102.89 |
0.13 |
0.23 |
| 2 |
A' |
1440 |
1440 |
19.82 |
2.08 |
0.67 |
0.80 |
| 3 |
A' |
757 |
757 |
38.47 |
12.34 |
0.34 |
0.51 |
| 4 |
A' |
54 |
54 |
115.91 |
0.61 |
0.53 |
0.69 |
| 5 |
A" |
3421 |
3421 |
0.18 |
46.93 |
0.75 |
0.86 |
| 6 |
A" |
1001 |
1001 |
0.37 |
9.04 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4958.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4958.2 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/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.003 |
1.178 |
0.000 |
| Cl2 |
-0.003 |
-0.611 |
0.000 |
| H3 |
0.039 |
1.662 |
0.961 |
| H4 |
0.039 |
1.662 |
-0.961 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7887 | 1.0767 | 1.0767 |
Cl2 | 1.7887 | | 2.4680 | 2.4680 | H3 | 1.0767 | 2.4680 | | 1.9216 | H4 | 1.0767 | 2.4680 | 1.9216 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
116.723 |
|
Br2 |
C1 |
H4 |
116.723 |
| H3 |
C1 |
H4 |
126.333 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.413 |
|
|
|
| 2 |
Cl |
0.021 |
|
|
|
| 3 |
H |
0.196 |
|
|
|
| 4 |
H |
0.196 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.096 |
1.650 |
0.000 |
1.653 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.575 |
0.148 |
-0.000 |
| y |
0.148 |
-17.431 |
-0.012 |
| z |
-0.000 |
-0.012 |
-18.516 |
|
| Traceless |
| | x | y | z |
| x |
-2.601 |
0.148 |
-0.000 |
| y |
0.148 |
2.114 |
-0.012 |
| z |
-0.000 |
-0.012 |
0.487 |
|
| Polar |
| 3z2-r2 | 0.974 |
| x2-y2 | -3.144 |
| xy | 0.148 |
| xz | -0.000 |
| yz | -0.012 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.102 |
0.022 |
0.000 |
| y |
0.022 |
4.350 |
0.002 |
| z |
0.000 |
0.002 |
1.982 |
<r2> (average value of r
2) Å
2
| <r2> |
33.809 |
| (<r2>)1/2 |
5.815 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31G
| | hartrees |
| Energy at 0K | -499.147803 |
| Energy at 298.15K | |
| HF Energy | -499.108150 |
| Nuclear repulsion energy | 43.643523 |
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/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 |
3245 |
3245 |
3.09 |
102.70 |
0.13 |
0.23 |
| 2 |
A1 |
1439 |
1439 |
19.94 |
|
|
|
| 3 |
A1 |
757 |
757 |
38.28 |
|
|
|
| 4 |
B1 |
104i |
104i |
117.98 |
|
|
|
| 5 |
B2 |
3423 |
3423 |
0.15 |
|
|
|
| 6 |
B2 |
1000 |
1000 |
0.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4880.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4880.2 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/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.177 |
| Cl2 |
0.000 |
0.000 |
0.611 |
| H3 |
0.000 |
0.961 |
-1.662 |
| H4 |
0.000 |
-0.961 |
-1.662 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7884 | 1.0766 | 1.0766 |
Cl2 | 1.7884 | | 2.4683 | 2.4683 | H3 | 1.0766 | 2.4683 | | 1.9223 | H4 | 1.0766 | 2.4683 | 1.9223 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
116.780 |
|
Br2 |
C1 |
H4 |
116.780 |
| H3 |
C1 |
H4 |
126.439 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.414 |
|
|
|
| 2 |
Cl |
0.021 |
|
|
|
| 3 |
H |
0.196 |
|
|
|
| 4 |
H |
0.196 |
|
|
|
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 |
-1.650 |
1.650 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.578 |
0.000 |
0.000 |
| y |
0.000 |
-18.515 |
0.000 |
| z |
0.000 |
0.000 |
-17.438 |
|
| Traceless |
| | x | y | z |
| x |
-2.602 |
0.000 |
0.000 |
| y |
0.000 |
0.493 |
0.000 |
| z |
0.000 |
0.000 |
2.108 |
|
| Polar |
| 3z2-r2 | 4.216 |
| x2-y2 | -2.063 |
| 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 |
1.101 |
0.000 |
0.000 |
| y |
0.000 |
1.983 |
0.000 |
| z |
0.000 |
0.000 |
4.353 |
<r2> (average value of r
2) Å
2
| <r2> |
33.806 |
| (<r2>)1/2 |
5.814 |