Jump to
S1C2
Energy calculated at BLYP/TZVP
| | hartrees |
| Energy at 0K | -959.049127 |
| Energy at 298.15K | |
| HF Energy | -959.049127 |
| Nuclear repulsion energy | 123.452431 |
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 BLYP/TZVP
| 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 |
3186 |
3178 |
0.00 |
|
|
|
| 2 |
A1 |
703 |
701 |
8.42 |
|
|
|
| 3 |
A1 |
296 |
295 |
0.13 |
|
|
|
| 4 |
B1 |
373i |
372i |
62.39 |
|
|
|
| 5 |
B2 |
1197 |
1194 |
42.58 |
|
|
|
| 6 |
B2 |
835 |
833 |
181.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2922.1 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 2914.8 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 BLYP/TZVP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.679 |
| H2 |
0.000 |
0.000 |
1.762 |
| Cl3 |
0.000 |
1.506 |
-0.172 |
| Cl4 |
0.000 |
-1.506 |
-0.172 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0821 | 1.7299 | 1.7299 |
H2 | 1.0821 | | 2.4506 | 2.4506 | Cl3 | 1.7299 | 2.4506 | | 3.0121 | Cl4 | 1.7299 | 2.4506 | 3.0121 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.472 |
|
Cl3 |
C1 |
Cl4 |
121.056 |
| Cl4 |
C1 |
H2 |
119.472 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.233 |
|
|
|
| 2 |
H |
0.205 |
|
|
|
| 3 |
Cl |
0.014 |
|
|
|
| 4 |
Cl |
0.014 |
|
|
|
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 |
0.835 |
0.835 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.231 |
0.000 |
0.000 |
| y |
0.000 |
-31.041 |
0.000 |
| z |
0.000 |
0.000 |
-29.254 |
|
| Traceless |
| | x | y | z |
| x |
-2.083 |
0.000 |
0.000 |
| y |
0.000 |
-0.298 |
0.000 |
| z |
0.000 |
0.000 |
2.381 |
|
| Polar |
| 3z2-r2 | 4.763 |
| x2-y2 | -1.190 |
| 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 |
2.925 |
0.000 |
0.000 |
| y |
0.000 |
7.462 |
0.000 |
| z |
0.000 |
0.000 |
4.106 |
<r2> (average value of r
2) Å
2
| <r2> |
103.256 |
| (<r2>)1/2 |
10.161 |
Jump to
S1C1
Energy calculated at BLYP/TZVP
| | hartrees |
| Energy at 0K | -959.050140 |
| Energy at 298.15K | -959.050863 |
| HF Energy | -959.050140 |
| Nuclear repulsion energy | 123.164361 |
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 BLYP/TZVP
| 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' |
3139 |
3131 |
1.97 |
|
|
|
| 2 |
A' |
715 |
713 |
16.31 |
|
|
|
| 3 |
A' |
480 |
478 |
26.30 |
|
|
|
| 4 |
A' |
289 |
289 |
0.33 |
|
|
|
| 5 |
A" |
1201 |
1198 |
34.40 |
|
|
|
| 6 |
A" |
794 |
792 |
208.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3308.5 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 3300.2 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 BLYP/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.708 |
0.000 |
| H2 |
-0.524 |
1.653 |
0.000 |
| Cl3 |
0.013 |
-0.174 |
1.503 |
| Cl4 |
0.013 |
-0.174 |
-1.503 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0860 | 1.7427 | 1.7427 |
H2 | 1.0860 | | 2.4253 | 2.4253 | Cl3 | 1.7427 | 2.4253 | | 3.0059 | Cl4 | 1.7427 | 2.4253 | 3.0059 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.107 |
|
Cl3 |
C1 |
Cl4 |
119.183 |
| Cl4 |
C1 |
H2 |
116.107 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.193 |
|
|
|
| 2 |
H |
0.185 |
|
|
|
| 3 |
Cl |
0.004 |
|
|
|
| 4 |
Cl |
0.004 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.573 |
0.738 |
0.000 |
0.935 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.898 |
-1.012 |
0.000 |
| y |
-1.012 |
-29.766 |
0.000 |
| z |
0.000 |
0.000 |
-31.245 |
|
| Traceless |
| | x | y | z |
| x |
-1.392 |
-1.012 |
0.000 |
| y |
-1.012 |
1.805 |
0.000 |
| z |
0.000 |
0.000 |
-0.412 |
|
| Polar |
| 3z2-r2 | -0.825 |
| x2-y2 | -2.132 |
| xy | -1.012 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.011 |
-0.119 |
0.000 |
| y |
-0.119 |
4.187 |
0.000 |
| z |
0.000 |
0.000 |
7.573 |
<r2> (average value of r
2) Å
2
| <r2> |
103.195 |
| (<r2>)1/2 |
10.158 |