Jump to
S1C2
Energy calculated at ROHF/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -957.402923 |
| Energy at 298.15K | |
| HF Energy | -957.402923 |
| Nuclear repulsion energy | 125.291176 |
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/aug-cc-pVDZ
| 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 |
3441 |
3441 |
1.05 |
|
|
|
| 2 |
A1 |
786 |
786 |
10.76 |
|
|
|
| 3 |
A1 |
323 |
323 |
0.82 |
|
|
|
| 4 |
B1 |
657i |
657i |
30.64 |
|
|
|
| 5 |
B2 |
1312 |
1312 |
73.03 |
|
|
|
| 6 |
B2 |
986 |
986 |
119.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3095.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3095.2 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 ROHF/aug-cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.683 |
| H2 |
0.000 |
0.000 |
1.756 |
| Cl3 |
0.000 |
1.478 |
-0.172 |
| Cl4 |
0.000 |
-1.478 |
-0.172 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0725 | 1.7081 | 1.7081 |
H2 | 1.0725 | | 2.4296 | 2.4296 | Cl3 | 1.7081 | 2.4296 | | 2.9567 | Cl4 | 1.7081 | 2.4296 | 2.9567 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
120.060 |
|
Cl3 |
C1 |
Cl4 |
119.881 |
| Cl4 |
C1 |
H2 |
120.060 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.006 |
|
|
|
| 2 |
H |
-0.001 |
|
|
|
| 3 |
Cl |
-0.002 |
|
|
|
| 4 |
Cl |
-0.002 |
|
|
|
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 |
1.221 |
1.221 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.451 |
0.000 |
0.000 |
| y |
0.000 |
-31.933 |
-0.000 |
| z |
0.000 |
-0.000 |
-29.048 |
|
| Traceless |
| | x | y | z |
| x |
-1.961 |
0.000 |
0.000 |
| y |
0.000 |
-1.183 |
-0.000 |
| z |
0.000 |
-0.000 |
3.144 |
|
| Polar |
| 3z2-r2 | 6.288 |
| x2-y2 | -0.518 |
| 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 |
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> |
100.652 |
| (<r2>)1/2 |
10.033 |
Jump to
S1C1
Energy calculated at ROHF/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -957.406750 |
| Energy at 298.15K | -957.407734 |
| HF Energy | -957.406750 |
| Nuclear repulsion energy | 125.013703 |
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/aug-cc-pVDZ
| 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' |
3372 |
3372 |
1.89 |
|
|
|
| 2 |
A' |
819 |
819 |
20.28 |
|
|
|
| 3 |
A' |
708 |
708 |
6.85 |
|
|
|
| 4 |
A' |
318 |
318 |
0.49 |
|
|
|
| 5 |
A" |
1320 |
1320 |
51.38 |
|
|
|
| 6 |
A" |
932 |
932 |
166.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3734.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3734.7 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 ROHF/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.015 |
0.723 |
0.000 |
| H2 |
-0.608 |
1.604 |
0.000 |
| Cl3 |
0.015 |
-0.175 |
1.472 |
| Cl4 |
0.015 |
-0.175 |
-1.472 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0783 | 1.7245 | 1.7245 |
H2 | 1.0783 | | 2.3912 | 2.3912 | Cl3 | 1.7245 | 2.3912 | | 2.9441 | Cl4 | 1.7245 | 2.3912 | 2.9441 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
115.166 |
|
Cl3 |
C1 |
Cl4 |
117.211 |
| Cl4 |
C1 |
H2 |
115.166 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.076 |
|
|
|
| 2 |
H |
0.086 |
|
|
|
| 3 |
Cl |
-0.005 |
|
|
|
| 4 |
Cl |
-0.005 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.512 |
1.140 |
0.000 |
1.249 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.994 |
-1.032 |
0.000 |
| y |
-1.032 |
-29.646 |
-0.000 |
| z |
0.000 |
-0.000 |
-32.192 |
|
| Traceless |
| | x | y | z |
| x |
-1.075 |
-1.032 |
0.000 |
| y |
-1.032 |
2.447 |
-0.000 |
| z |
0.000 |
-0.000 |
-1.372 |
|
| Polar |
| 3z2-r2 | -2.744 |
| x2-y2 | -2.349 |
| xy | -1.032 |
| 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> |
100.340 |
| (<r2>)1/2 |
10.017 |