Jump to
S1C2
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -499.217152 |
| Energy at 298.15K | |
| HF Energy | -499.217152 |
| Nuclear repulsion energy | 45.113806 |
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 PBEPBE/6-311G**
| 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' |
3109 |
3081 |
7.23 |
|
|
|
| 2 |
A' |
1368 |
1356 |
7.96 |
|
|
|
| 3 |
A' |
828 |
820 |
35.52 |
|
|
|
| 4 |
A' |
180 |
178 |
93.40 |
|
|
|
| 5 |
A" |
3263 |
3233 |
0.24 |
|
|
|
| 6 |
A" |
978 |
969 |
1.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4862.5 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 4818.2 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 PBEPBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.000 |
1.124 |
0.000 |
| Cl2 |
-0.000 |
-0.588 |
0.000 |
| H3 |
0.001 |
1.625 |
0.963 |
| H4 |
0.001 |
1.625 |
-0.963 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7116 | 1.0857 | 1.0857 |
Cl2 | 1.7116 | | 2.4132 | 2.4132 | H3 | 1.0857 | 2.4132 | | 1.9264 | H4 | 1.0857 | 2.4132 | 1.9264 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.484 |
|
Br2 |
C1 |
H4 |
117.484 |
| H3 |
C1 |
H4 |
125.031 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.351 |
|
|
|
| 2 |
Cl |
-0.008 |
|
|
|
| 3 |
H |
0.179 |
|
|
|
| 4 |
H |
0.179 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.003 |
1.080 |
0.000 |
1.080 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.769 |
0.005 |
0.000 |
| y |
0.005 |
-17.604 |
0.000 |
| z |
0.000 |
0.000 |
-18.668 |
|
| Traceless |
| | x | y | z |
| x |
-2.632 |
0.005 |
0.000 |
| y |
0.005 |
2.114 |
0.000 |
| z |
0.000 |
0.000 |
0.518 |
|
| Polar |
| 3z2-r2 | 1.037 |
| x2-y2 | -3.164 |
| xy | 0.005 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.755 |
0.001 |
0.000 |
| y |
0.001 |
4.759 |
0.000 |
| z |
0.000 |
0.000 |
2.360 |
<r2> (average value of r
2) Å
2
| <r2> |
32.463 |
| (<r2>)1/2 |
5.698 |
Jump to
S1C1
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -499.217152 |
| Energy at 298.15K | -499.217963 |
| HF Energy | -499.217152 |
| Nuclear repulsion energy | 45.109595 |
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 PBEPBE/6-311G**
| 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 |
3109 |
3081 |
7.21 |
|
|
|
| 2 |
A1 |
1368 |
1356 |
7.97 |
|
|
|
| 3 |
A1 |
827 |
820 |
35.55 |
|
|
|
| 4 |
B1 |
179 |
178 |
93.42 |
|
|
|
| 5 |
B2 |
3262 |
3233 |
0.23 |
|
|
|
| 6 |
B2 |
978 |
969 |
1.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4861.8 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 4817.5 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 PBEPBE/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.124 |
| Cl2 |
0.000 |
0.000 |
0.588 |
| H3 |
0.000 |
0.963 |
-1.625 |
| H4 |
0.000 |
-0.963 |
-1.625 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7119 | 1.0857 | 1.0857 |
Cl2 | 1.7119 | | 2.4133 | 2.4133 | H3 | 1.0857 | 2.4133 | | 1.9267 | H4 | 1.0857 | 2.4133 | 1.9267 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.467 |
|
Br2 |
C1 |
H4 |
117.467 |
| H3 |
C1 |
H4 |
125.066 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.351 |
|
|
|
| 2 |
Cl |
-0.008 |
|
|
|
| 3 |
H |
0.179 |
|
|
|
| 4 |
H |
0.179 |
|
|
|
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 |
-1.081 |
1.081 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.769 |
0.000 |
0.000 |
| y |
0.000 |
-18.667 |
0.000 |
| z |
0.000 |
0.000 |
-17.605 |
|
| Traceless |
| | x | y | z |
| x |
-2.633 |
0.000 |
0.000 |
| y |
0.000 |
0.520 |
0.000 |
| z |
0.000 |
0.000 |
2.114 |
|
| Polar |
| 3z2-r2 | 4.227 |
| x2-y2 | -2.102 |
| 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 |
1.755 |
0.000 |
0.000 |
| y |
0.000 |
2.360 |
0.000 |
| z |
0.000 |
0.000 |
4.760 |
<r2> (average value of r
2) Å
2
| <r2> |
32.467 |
| (<r2>)1/2 |
5.698 |