Jump to
S1C2
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -959.030898 |
| Energy at 298.15K | |
| HF Energy | -959.030898 |
| Nuclear repulsion energy | 125.268207 |
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 wB97X-D/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 |
3288 |
3132 |
0.77 |
|
|
|
| 2 |
A1 |
764 |
728 |
11.42 |
|
|
|
| 3 |
A1 |
311 |
296 |
0.43 |
|
|
|
| 4 |
B1 |
397i |
378i |
51.51 |
|
|
|
| 5 |
B2 |
1213 |
1155 |
54.19 |
|
|
|
| 6 |
B2 |
936 |
892 |
152.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3057.2 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 2912.2 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 wB97X-D/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.676 |
| H2 |
0.000 |
0.000 |
1.764 |
| Cl3 |
0.000 |
1.480 |
-0.171 |
| Cl4 |
0.000 |
-1.480 |
-0.171 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0878 | 1.7055 | 1.7055 |
H2 | 1.0878 | | 2.4364 | 2.4364 | Cl3 | 1.7055 | 2.4364 | | 2.9599 | Cl4 | 1.7055 | 2.4364 | 2.9599 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
119.803 |
|
Cl3 |
C1 |
Cl4 |
120.394 |
| Cl4 |
C1 |
H2 |
119.803 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.139 |
|
|
|
| 2 |
H |
0.126 |
|
|
|
| 3 |
Cl |
0.007 |
|
|
|
| 4 |
Cl |
0.007 |
|
|
|
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 |
0.943 |
0.943 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.618 |
0.000 |
0.000 |
| y |
0.000 |
-30.661 |
0.000 |
| z |
0.000 |
0.000 |
-28.594 |
|
| Traceless |
| | x | y | z |
| x |
-1.990 |
0.000 |
0.000 |
| y |
0.000 |
-0.555 |
0.000 |
| z |
0.000 |
0.000 |
2.545 |
|
| Polar |
| 3z2-r2 | 5.090 |
| x2-y2 | -0.957 |
| 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 |
2.221 |
0.000 |
0.000 |
| y |
0.000 |
6.532 |
0.000 |
| z |
0.000 |
0.000 |
3.616 |
<r2> (average value of r
2) Å
2
| <r2> |
100.241 |
| (<r2>)1/2 |
10.012 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -959.031844 |
| Energy at 298.15K | -959.032661 |
| HF Energy | -959.031844 |
| Nuclear repulsion energy | 125.121565 |
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 wB97X-D/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' |
3243 |
3089 |
1.46 |
|
|
|
| 2 |
A' |
768 |
732 |
17.30 |
|
|
|
| 3 |
A' |
506 |
482 |
25.28 |
|
|
|
| 4 |
A' |
305 |
291 |
0.58 |
|
|
|
| 5 |
A" |
1221 |
1163 |
43.39 |
|
|
|
| 6 |
A" |
904 |
861 |
179.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3473.6 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 3309.0 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 wB97X-D/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
0.701 |
0.000 |
| H2 |
-0.500 |
1.665 |
0.000 |
| Cl3 |
0.013 |
-0.173 |
1.476 |
| Cl4 |
0.013 |
-0.173 |
-1.476 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
Cl3 |
Cl4 |
| C1 | | 1.0911 | 1.7152 | 1.7152 |
H2 | 1.0911 | | 2.4117 | 2.4117 | Cl3 | 1.7152 | 2.4117 | | 2.9515 | Cl4 | 1.7152 | 2.4117 | 2.9515 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Cl3 |
C1 |
H2 |
116.736 |
|
Cl3 |
C1 |
Cl4 |
118.718 |
| Cl4 |
C1 |
H2 |
116.736 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.126 |
|
|
|
| 2 |
H |
0.128 |
|
|
|
| 3 |
Cl |
-0.001 |
|
|
|
| 4 |
Cl |
-0.001 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.516 |
0.852 |
0.000 |
0.996 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.318 |
-0.916 |
0.000 |
| y |
-0.916 |
-29.049 |
0.000 |
| z |
0.000 |
0.000 |
-30.827 |
|
| Traceless |
| | x | y | z |
| x |
-1.381 |
-0.916 |
0.000 |
| y |
-0.916 |
2.024 |
0.000 |
| z |
0.000 |
0.000 |
-0.643 |
|
| Polar |
| 3z2-r2 | -1.286 |
| x2-y2 | -2.270 |
| xy | -0.916 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.327 |
-0.192 |
0.000 |
| y |
-0.192 |
3.634 |
0.000 |
| z |
0.000 |
0.000 |
6.600 |
<r2> (average value of r
2) Å
2
| <r2> |
100.027 |
| (<r2>)1/2 |
10.001 |