Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -107.442197 |
| Energy at 298.15K | -107.446940 |
| Nuclear repulsion energy | 88.551977 |
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/LANL2DZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3344 |
3009 |
0.00 |
|
|
|
| 2 |
Ag |
1648 |
1483 |
0.00 |
|
|
|
| 3 |
Ag |
1475 |
1328 |
0.00 |
|
|
|
| 4 |
Ag |
1163 |
1047 |
0.00 |
|
|
|
| 5 |
Ag |
753 |
678 |
0.00 |
|
|
|
| 6 |
Ag |
303 |
272 |
0.00 |
|
|
|
| 7 |
Au |
3444 |
3100 |
12.08 |
|
|
|
| 8 |
Au |
1243 |
1118 |
0.12 |
|
|
|
| 9 |
Au |
868 |
782 |
3.70 |
|
|
|
| 10 |
Au |
119 |
107 |
14.40 |
|
|
|
| 11 |
Bg |
3426 |
3083 |
0.00 |
|
|
|
| 12 |
Bg |
1415 |
1273 |
0.00 |
|
|
|
| 13 |
Bg |
1104 |
993 |
0.00 |
|
|
|
| 14 |
Bu |
3348 |
3013 |
23.79 |
|
|
|
| 15 |
Bu |
1641 |
1477 |
12.49 |
|
|
|
| 16 |
Bu |
1402 |
1261 |
52.03 |
|
|
|
| 17 |
Bu |
686 |
618 |
153.81 |
|
|
|
| 18 |
Bu |
225 |
203 |
17.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13804.2 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 12422.4 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/LANL2DZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.757 |
0.000 |
| C2 |
0.000 |
-0.757 |
0.000 |
| Cl3 |
-1.779 |
1.337 |
0.000 |
| Cl4 |
1.779 |
-1.337 |
0.000 |
| H5 |
0.444 |
1.171 |
0.885 |
| H6 |
0.444 |
1.171 |
-0.885 |
| H7 |
-0.444 |
-1.171 |
0.885 |
| H8 |
-0.444 |
-1.171 |
-0.885 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5150 | 1.8706 | 2.7478 | 1.0735 | 1.0735 | 2.1683 | 2.1683 |
C2 | 1.5150 | | 2.7478 | 1.8706 | 2.1683 | 2.1683 | 1.0735 | 1.0735 | Cl3 | 1.8706 | 2.7478 | | 4.4501 | 2.3984 | 2.3984 | 2.9758 | 2.9758 | Cl4 | 2.7478 | 1.8706 | 4.4501 | | 2.9758 | 2.9758 | 2.3984 | 2.3984 | H5 | 1.0735 | 2.1683 | 2.3984 | 2.9758 | | 1.7703 | 2.5058 | 3.0680 | H6 | 1.0735 | 2.1683 | 2.3984 | 2.9758 | 1.7703 | | 3.0680 | 2.5058 | H7 | 2.1683 | 1.0735 | 2.9758 | 2.3984 | 2.5058 | 3.0680 | | 1.7703 | H8 | 2.1683 | 1.0735 | 2.9758 | 2.3984 | 3.0680 | 2.5058 | 1.7703 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.047 |
|
C1 |
C2 |
H7 |
112.682 |
| C1 |
C2 |
H8 |
112.682 |
|
C2 |
C1 |
Cl3 |
108.047 |
| C2 |
C1 |
H5 |
112.682 |
|
C2 |
C1 |
H6 |
112.682 |
| Cl3 |
C1 |
H5 |
105.912 |
|
Cl3 |
C1 |
H6 |
105.912 |
| Cl4 |
C2 |
H7 |
105.912 |
|
Cl4 |
C2 |
H8 |
105.912 |
| H5 |
C1 |
H6 |
111.089 |
|
H7 |
C2 |
H8 |
111.089 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.364 |
|
|
|
| 2 |
C |
-0.364 |
|
|
|
| 3 |
Cl |
-0.136 |
|
|
|
| 4 |
Cl |
-0.136 |
|
|
|
| 5 |
H |
0.250 |
|
|
|
| 6 |
H |
0.250 |
|
|
|
| 7 |
H |
0.250 |
|
|
|
| 8 |
H |
0.250 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-45.458 |
7.183 |
0.000 |
| y |
7.183 |
-39.991 |
0.000 |
| z |
0.000 |
0.000 |
-36.099 |
|
| Traceless |
| | x | y | z |
| x |
-7.413 |
7.183 |
0.000 |
| y |
7.183 |
0.788 |
0.000 |
| z |
0.000 |
0.000 |
6.625 |
|
| Polar |
| 3z2-r2 | 13.251 |
| x2-y2 | -5.468 |
| xy | 7.183 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.151 |
-2.191 |
0.000 |
| y |
-2.191 |
4.254 |
0.000 |
| z |
0.000 |
0.000 |
2.980 |
<r2> (average value of r
2) Å
2
| <r2> |
110.916 |
| (<r2>)1/2 |
10.532 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -107.438426 |
| Energy at 298.15K | -107.443322 |
| HF Energy | -107.438426 |
| Nuclear repulsion energy | 89.535006 |
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/LANL2DZ
| 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 |
3404 |
3063 |
1.77 |
|
|
|
| 2 |
A |
3324 |
2992 |
39.63 |
|
|
|
| 3 |
A |
1625 |
1462 |
0.90 |
|
|
|
| 4 |
A |
1478 |
1330 |
24.18 |
|
|
|
| 5 |
A |
1339 |
1205 |
0.17 |
|
|
|
| 6 |
A |
1151 |
1036 |
1.60 |
|
|
|
| 7 |
A |
1044 |
939 |
11.86 |
|
|
|
| 8 |
A |
645 |
580 |
38.10 |
|
|
|
| 9 |
A |
280 |
252 |
1.57 |
|
|
|
| 10 |
A |
113 |
101 |
2.38 |
|
|
|
| 11 |
B |
3413 |
3071 |
10.27 |
|
|
|
| 12 |
B |
3314 |
2982 |
6.41 |
|
|
|
| 13 |
B |
1623 |
1460 |
12.81 |
|
|
|
| 14 |
B |
1466 |
1319 |
51.31 |
|
|
|
| 15 |
B |
1268 |
1141 |
0.57 |
|
|
|
| 16 |
B |
992 |
892 |
18.64 |
|
|
|
| 17 |
B |
667 |
600 |
49.72 |
|
|
|
| 18 |
B |
428 |
385 |
16.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13785.6 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 12405.7 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/LANL2DZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.318 |
0.687 |
0.914 |
| C2 |
-0.318 |
-0.687 |
0.914 |
| Cl3 |
-0.318 |
1.744 |
-0.476 |
| Cl4 |
0.318 |
-1.744 |
-0.476 |
| H5 |
0.057 |
1.217 |
1.814 |
| H6 |
1.385 |
0.648 |
0.796 |
| H7 |
-0.057 |
-1.217 |
1.814 |
| H8 |
-1.385 |
-0.648 |
0.796 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5131 | 1.8587 | 2.8002 | 1.0768 | 1.0741 | 2.1384 | 2.1662 |
C2 | 1.5131 | | 2.8002 | 1.8587 | 2.1384 | 2.1662 | 1.0768 | 1.0741 | Cl3 | 1.8587 | 2.8002 | | 3.5460 | 2.3796 | 2.3911 | 3.7524 | 2.9115 | Cl4 | 2.8002 | 1.8587 | 3.5460 | | 3.7524 | 2.9115 | 2.3796 | 2.3911 | H5 | 1.0768 | 2.1384 | 2.3796 | 3.7524 | | 1.7677 | 2.4362 | 2.5672 | H6 | 1.0741 | 2.1662 | 2.3911 | 2.9115 | 1.7677 | | 2.5672 | 3.0572 | H7 | 2.1384 | 1.0768 | 3.7524 | 2.3796 | 2.4362 | 2.5672 | | 1.7677 | H8 | 2.1662 | 1.0741 | 2.9115 | 2.3911 | 2.5672 | 3.0572 | 1.7677 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
111.890 |
|
C1 |
C2 |
H7 |
110.179 |
| C1 |
C2 |
H8 |
112.604 |
|
C2 |
C1 |
Cl3 |
111.890 |
| C2 |
C1 |
H5 |
110.179 |
|
C2 |
C1 |
H6 |
112.604 |
| Cl3 |
C1 |
H5 |
105.185 |
|
Cl3 |
C1 |
H6 |
106.130 |
| Cl4 |
C2 |
H7 |
105.185 |
|
Cl4 |
C2 |
H8 |
106.130 |
| H5 |
C1 |
H6 |
110.539 |
|
H7 |
C2 |
H8 |
110.539 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.371 |
|
|
|
| 2 |
C |
-0.371 |
|
|
|
| 3 |
Cl |
-0.118 |
|
|
|
| 4 |
Cl |
-0.118 |
|
|
|
| 5 |
H |
0.235 |
|
|
|
| 6 |
H |
0.254 |
|
|
|
| 7 |
H |
0.235 |
|
|
|
| 8 |
H |
0.254 |
|
|
|
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 |
4.080 |
4.080 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.045 |
2.138 |
0.000 |
| y |
2.138 |
-43.889 |
0.000 |
| z |
0.000 |
0.000 |
-34.174 |
|
| Traceless |
| | x | y | z |
| x |
2.987 |
2.138 |
0.000 |
| y |
2.138 |
-8.780 |
0.000 |
| z |
0.000 |
0.000 |
5.793 |
|
| Polar |
| 3z2-r2 | 11.587 |
| x2-y2 | 7.845 |
| xy | 2.138 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.556 |
-0.974 |
0.000 |
| y |
-0.974 |
5.519 |
0.000 |
| z |
0.000 |
0.000 |
5.744 |
<r2> (average value of r
2) Å
2
| <r2> |
103.317 |
| (<r2>)1/2 |
10.164 |