Jump to
S1C2
Energy calculated at PBEPBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -499.232472 |
| Energy at 298.15K | |
| HF Energy | -499.232472 |
| Nuclear repulsion energy | 45.305299 |
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/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' |
3103 |
3082 |
7.10 |
|
|
|
| 2 |
A' |
1362 |
1352 |
7.63 |
|
|
|
| 3 |
A' |
835 |
830 |
29.72 |
|
|
|
| 4 |
A' |
207 |
205 |
71.23 |
|
|
|
| 5 |
A" |
3251 |
3228 |
0.05 |
|
|
|
| 6 |
A" |
966 |
959 |
0.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4861.7 cm
-1
Scaled (by 0.9931) Zero Point Vibrational Energy (zpe) 4828.2 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
1.118 |
0.000 |
| Cl2 |
0.000 |
-0.585 |
0.000 |
| H3 |
-0.000 |
1.622 |
0.960 |
| H4 |
-0.000 |
1.622 |
-0.960 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7028 | 1.0844 | 1.0844 |
Cl2 | 1.7028 | | 2.4069 | 2.4069 | H3 | 1.0844 | 2.4069 | | 1.9201 | H4 | 1.0844 | 2.4069 | 1.9201 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.714 |
|
Br2 |
C1 |
H4 |
117.714 |
| H3 |
C1 |
H4 |
124.573 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.223 |
|
|
|
| 2 |
Cl |
-0.036 |
|
|
|
| 3 |
H |
0.129 |
|
|
|
| 4 |
H |
0.129 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.000 |
0.967 |
0.000 |
0.967 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.460 |
-0.001 |
0.000 |
| y |
-0.001 |
-17.377 |
0.000 |
| z |
0.000 |
0.000 |
-18.458 |
|
| Traceless |
| | x | y | z |
| x |
-2.542 |
-0.001 |
0.000 |
| y |
-0.001 |
2.081 |
0.000 |
| z |
0.000 |
0.000 |
0.461 |
|
| Polar |
| 3z2-r2 | 0.922 |
| x2-y2 | -3.082 |
| 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 |
2.484 |
-0.000 |
0.000 |
| y |
-0.000 |
5.009 |
0.000 |
| z |
0.000 |
0.000 |
2.956 |
<r2> (average value of r
2) Å
2
| <r2> |
32.140 |
| (<r2>)1/2 |
5.669 |
Jump to
S1C1
Energy calculated at PBEPBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -499.232472 |
| Energy at 298.15K | -499.233327 |
| HF Energy | -499.232472 |
| Nuclear repulsion energy | 45.308318 |
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/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 |
3103 |
3081 |
7.11 |
|
|
|
| 2 |
A1 |
1362 |
1352 |
7.61 |
|
|
|
| 3 |
A1 |
836 |
830 |
29.74 |
|
|
|
| 4 |
B1 |
207 |
205 |
71.25 |
|
|
|
| 5 |
B2 |
3250 |
3228 |
0.05 |
|
|
|
| 6 |
B2 |
966 |
960 |
0.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4861.7 cm
-1
Scaled (by 0.9931) Zero Point Vibrational Energy (zpe) 4828.2 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/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.118 |
| Cl2 |
0.000 |
0.000 |
0.585 |
| H3 |
0.000 |
0.960 |
-1.621 |
| H4 |
0.000 |
-0.960 |
-1.621 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7027 | 1.0845 | 1.0845 |
Cl2 | 1.7027 | | 2.4065 | 2.4065 | H3 | 1.0845 | 2.4065 | | 1.9206 | H4 | 1.0845 | 2.4065 | 1.9206 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.687 |
|
Br2 |
C1 |
H4 |
117.687 |
| H3 |
C1 |
H4 |
124.627 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.222 |
|
|
|
| 2 |
Cl |
-0.036 |
|
|
|
| 3 |
H |
0.129 |
|
|
|
| 4 |
H |
0.129 |
|
|
|
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 |
-0.967 |
0.967 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.460 |
0.000 |
0.000 |
| y |
0.000 |
-18.456 |
0.000 |
| z |
0.000 |
0.000 |
-17.380 |
|
| Traceless |
| | x | y | z |
| x |
-2.542 |
0.000 |
0.000 |
| y |
0.000 |
0.464 |
0.000 |
| z |
0.000 |
0.000 |
2.078 |
|
| Polar |
| 3z2-r2 | 4.155 |
| x2-y2 | -2.004 |
| 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 |
2.484 |
0.000 |
0.000 |
| y |
0.000 |
2.956 |
0.000 |
| z |
0.000 |
0.000 |
5.008 |
<r2> (average value of r
2) Å
2
| <r2> |
32.137 |
| (<r2>)1/2 |
5.669 |