Jump to
S1C2
Energy calculated at ROHF/Def2TZVPP
| | hartrees |
| Energy at 0K | -498.504205 |
| Energy at 298.15K | |
| HF Energy | -498.504205 |
| Nuclear repulsion energy | 45.261284 |
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 ROHF/Def2TZVPP
| 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' |
3300 |
3300 |
14.52 |
|
|
|
| 2 |
A' |
1531 |
1531 |
17.01 |
|
|
|
| 3 |
A' |
861 |
861 |
44.37 |
|
|
|
| 4 |
A' |
635 |
635 |
37.79 |
|
|
|
| 5 |
A" |
3443 |
3443 |
0.89 |
|
|
|
| 6 |
A" |
1084 |
1084 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5427.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5427.5 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 ROHF/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.019 |
1.128 |
0.000 |
| Cl2 |
-0.019 |
-0.586 |
0.000 |
| H3 |
0.219 |
1.595 |
0.932 |
| H4 |
0.219 |
1.595 |
-0.932 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7142 | 1.0689 | 1.0689 |
Cl2 | 1.7142 | | 2.3836 | 2.3836 | H3 | 1.0689 | 2.3836 | | 1.8632 | H4 | 1.0689 | 2.3836 | 1.8632 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
115.897 |
|
Br2 |
C1 |
H4 |
115.897 |
| H3 |
C1 |
H4 |
121.284 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.075 |
|
|
|
| 2 |
Cl |
-0.100 |
|
|
|
| 3 |
H |
0.088 |
|
|
|
| 4 |
H |
0.088 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.383 |
1.468 |
0.000 |
1.517 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.365 |
0.674 |
-0.000 |
| y |
0.674 |
-17.313 |
0.000 |
| z |
-0.000 |
0.000 |
-18.639 |
|
| Traceless |
| | x | y | z |
| x |
-2.389 |
0.674 |
-0.000 |
| y |
0.674 |
2.189 |
0.000 |
| z |
-0.000 |
0.000 |
0.200 |
|
| Polar |
| 3z2-r2 | 0.400 |
| x2-y2 | -3.052 |
| xy | 0.674 |
| xz | -0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
32.128 |
| (<r2>)1/2 |
5.668 |
Jump to
S1C1
Energy calculated at ROHF/Def2TZVPP
| | hartrees |
| Energy at 0K | -498.503489 |
| Energy at 298.15K | |
| HF Energy | -498.503489 |
| Nuclear repulsion energy | 45.391999 |
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 ROHF/Def2TZVPP
| 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 |
3332 |
3332 |
9.68 |
|
|
|
| 2 |
A1 |
1529 |
1529 |
18.74 |
|
|
|
| 3 |
A1 |
869 |
869 |
38.44 |
|
|
|
| 4 |
B1 |
498i |
498i |
67.30 |
|
|
|
| 5 |
B2 |
3487 |
3487 |
0.02 |
|
|
|
| 6 |
B2 |
1064 |
1064 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4891.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4891.3 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 ROHF/Def2TZVPP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.120 |
| Cl2 |
0.000 |
0.000 |
0.586 |
| H3 |
0.000 |
0.942 |
-1.618 |
| H4 |
0.000 |
-0.942 |
-1.618 |
Atom - Atom Distances (Å)
| |
C1 |
Cl2 |
H3 |
H4 |
| C1 | | 1.7057 | 1.0657 | 1.0657 |
Cl2 | 1.7057 | | 2.3963 | 2.3963 | H3 | 1.0657 | 2.3963 | | 1.8850 | H4 | 1.0657 | 2.3963 | 1.8850 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
117.825 |
|
Br2 |
C1 |
H4 |
117.825 |
| H3 |
C1 |
H4 |
124.351 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.083 |
|
|
|
| 2 |
Cl |
-0.088 |
|
|
|
| 3 |
H |
0.086 |
|
|
|
| 4 |
H |
0.086 |
|
|
|
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 |
-1.465 |
1.465 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.511 |
0.000 |
0.000 |
| y |
0.000 |
-18.528 |
-0.001 |
| z |
0.000 |
-0.001 |
-17.159 |
|
| Traceless |
| | x | y | z |
| x |
-2.667 |
0.000 |
0.000 |
| y |
0.000 |
0.307 |
-0.001 |
| z |
0.000 |
-0.001 |
2.361 |
|
| Polar |
| 3z2-r2 | 4.721 |
| x2-y2 | -1.983 |
| xy | 0.000 |
| xz | 0.000 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
32.067 |
| (<r2>)1/2 |
5.663 |