Jump to
S1C2
Energy calculated at HF/cc-pVQZ
| | hartrees |
| Energy at 0K | -498.522490 |
| Energy at 298.15K | |
| HF Energy | -498.522490 |
| Nuclear repulsion energy | 45.308618 |
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 HF/cc-pVQZ
| 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' |
3298 |
2996 |
11.56 |
111.09 |
0.09 |
0.16 |
| 2 |
A' |
1524 |
1385 |
16.87 |
1.01 |
0.74 |
0.85 |
| 3 |
A' |
858 |
780 |
41.33 |
9.33 |
0.20 |
0.33 |
| 4 |
A' |
442 |
401 |
46.65 |
0.68 |
0.08 |
0.16 |
| 5 |
A" |
3445 |
3129 |
0.14 |
46.76 |
0.75 |
0.86 |
| 6 |
A" |
1071 |
973 |
0.02 |
1.41 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 5319.0 cm
-1
Scaled (by 0.9084) Zero Point Vibrational Energy (zpe) 4831.7 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 HF/cc-pVQZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.014 |
1.125 |
0.000 |
| Cl2 |
-0.014 |
-0.586 |
0.000 |
| H3 |
0.159 |
1.606 |
0.938 |
| H4 |
0.159 |
1.606 |
-0.938 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7106 | 1.0680 | 1.0680 |
Cl2 | 1.7106 | | 2.3902 | 2.3902 | H3 | 1.0680 | 2.3902 | | 1.8756 | H4 | 1.0680 | 2.3902 | 1.8756 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
116.774 |
|
Br2 |
C1 |
H4 |
116.774 |
| H3 |
C1 |
H4 |
122.824 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.161 |
|
|
|
| 2 |
Cl |
-0.086 |
|
|
|
| 3 |
H |
0.123 |
|
|
|
| 4 |
H |
0.123 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.276 |
1.469 |
0.000 |
1.495 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.440 |
0.496 |
0.000 |
| y |
0.496 |
-17.311 |
0.000 |
| z |
0.000 |
0.000 |
-18.619 |
|
| Traceless |
| | x | y | z |
| x |
-2.475 |
0.496 |
0.000 |
| y |
0.496 |
2.219 |
0.000 |
| z |
0.000 |
0.000 |
0.257 |
|
| Polar |
| 3z2-r2 | 0.513 |
| x2-y2 | -3.129 |
| xy | 0.496 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.810 |
0.040 |
0.000 |
| y |
0.040 |
4.688 |
0.000 |
| z |
0.000 |
0.000 |
3.133 |
<r2> (average value of r
2) Å
2
| <r2> |
32.133 |
| (<r2>)1/2 |
5.669 |
Jump to
S1C1
Energy calculated at HF/cc-pVQZ
| | hartrees |
| Energy at 0K | -498.522336 |
| Energy at 298.15K | |
| HF Energy | -498.522336 |
| Nuclear repulsion energy | 45.362007 |
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 HF/cc-pVQZ
| 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 |
3309 |
3006 |
9.25 |
108.52 |
0.09 |
0.16 |
| 2 |
A1 |
1522 |
1383 |
18.04 |
|
|
|
| 3 |
A1 |
862 |
783 |
38.21 |
|
|
|
| 4 |
B1 |
319i |
289i |
60.19 |
|
|
|
| 5 |
B2 |
3464 |
3147 |
0.02 |
|
|
|
| 6 |
B2 |
1060 |
963 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4949.5 cm
-1
Scaled (by 0.9084) Zero Point Vibrational Energy (zpe) 4496.1 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 HF/cc-pVQZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.121 |
| Cl2 |
0.000 |
0.000 |
0.586 |
| H3 |
0.000 |
0.944 |
-1.618 |
| H4 |
0.000 |
-0.944 |
-1.618 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7069 | 1.0666 | 1.0666 |
Cl2 | 1.7069 | | 2.3973 | 2.3973 | H3 | 1.0666 | 2.3973 | | 1.8877 | H4 | 1.0666 | 2.3973 | 1.8877 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.759 |
|
Br2 |
C1 |
H4 |
117.759 |
| H3 |
C1 |
H4 |
124.482 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.172 |
|
|
|
| 2 |
Cl |
-0.082 |
|
|
|
| 3 |
H |
0.127 |
|
|
|
| 4 |
H |
0.127 |
|
|
|
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 |
-1.473 |
1.473 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.512 |
0.000 |
0.000 |
| y |
0.000 |
-18.562 |
0.000 |
| z |
0.000 |
0.000 |
-17.230 |
|
| Traceless |
| | x | y | z |
| x |
-2.615 |
0.000 |
0.000 |
| y |
0.000 |
0.309 |
0.000 |
| z |
0.000 |
0.000 |
2.307 |
|
| Polar |
| 3z2-r2 | 4.613 |
| x2-y2 | -1.949 |
| 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 |
2.804 |
0.000 |
0.000 |
| y |
0.000 |
3.121 |
0.000 |
| z |
0.000 |
0.000 |
4.669 |
<r2> (average value of r
2) Å
2
| <r2> |
32.113 |
| (<r2>)1/2 |
5.667 |