Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -999.124114 |
| Energy at 298.15K | -999.128804 |
| Nuclear repulsion energy | 194.841763 |
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 B1B95/6-311G*
| 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 |
3120 |
2991 |
0.00 |
|
|
|
| 2 |
Ag |
1498 |
1436 |
0.00 |
|
|
|
| 3 |
Ag |
1358 |
1301 |
0.00 |
|
|
|
| 4 |
Ag |
1086 |
1041 |
0.00 |
|
|
|
| 5 |
Ag |
775 |
743 |
0.00 |
|
|
|
| 6 |
Ag |
301 |
288 |
0.00 |
|
|
|
| 7 |
Au |
3201 |
3069 |
7.01 |
|
|
|
| 8 |
Au |
1170 |
1122 |
4.47 |
|
|
|
| 9 |
Au |
781 |
749 |
4.60 |
|
|
|
| 10 |
Au |
125 |
120 |
7.14 |
|
|
|
| 11 |
Bg |
3178 |
3046 |
0.00 |
|
|
|
| 12 |
Bg |
1313 |
1259 |
0.00 |
|
|
|
| 13 |
Bg |
1025 |
983 |
0.00 |
|
|
|
| 14 |
Bu |
3128 |
2999 |
20.80 |
|
|
|
| 15 |
Bu |
1498 |
1436 |
7.12 |
|
|
|
| 16 |
Bu |
1278 |
1226 |
40.07 |
|
|
|
| 17 |
Bu |
734 |
704 |
107.75 |
|
|
|
| 18 |
Bu |
211 |
202 |
10.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12889.3 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12355.7 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 B1B95/6-311G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.473 |
0.586 |
0.000 |
| C2 |
-0.473 |
-0.586 |
0.000 |
| Cl3 |
-0.473 |
2.109 |
0.000 |
| Cl4 |
0.473 |
-2.109 |
0.000 |
| H5 |
1.100 |
0.593 |
0.888 |
| H6 |
1.100 |
0.593 |
-0.888 |
| H7 |
-1.100 |
-0.593 |
0.888 |
| H8 |
-1.100 |
-0.593 |
-0.888 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5070 | 1.7930 | 2.6949 | 1.0868 | 1.0868 | 2.1575 | 2.1575 |
C2 | 1.5070 | | 2.6949 | 1.7930 | 2.1575 | 2.1575 | 1.0868 | 1.0868 | Cl3 | 1.7930 | 2.6949 | | 4.3224 | 2.3585 | 2.3585 | 2.9119 | 2.9119 | Cl4 | 2.6949 | 1.7930 | 4.3224 | | 2.9119 | 2.9119 | 2.3585 | 2.3585 | H5 | 1.0868 | 2.1575 | 2.3585 | 2.9119 | | 1.7755 | 2.4996 | 3.0660 | H6 | 1.0868 | 2.1575 | 2.3585 | 2.9119 | 1.7755 | | 3.0660 | 2.4996 | H7 | 2.1575 | 1.0868 | 2.9119 | 2.3585 | 2.4996 | 3.0660 | | 1.7755 | H8 | 2.1575 | 1.0868 | 2.9119 | 2.3585 | 3.0660 | 2.4996 | 1.7755 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.194 |
|
C1 |
C2 |
H7 |
111.542 |
| C1 |
C2 |
H8 |
111.542 |
|
C2 |
C1 |
Cl3 |
109.194 |
| C2 |
C1 |
H5 |
111.542 |
|
C2 |
C1 |
H6 |
111.542 |
| Cl3 |
C1 |
H5 |
107.423 |
|
Cl3 |
C1 |
H6 |
107.423 |
| Cl4 |
C2 |
H7 |
107.423 |
|
Cl4 |
C2 |
H8 |
107.423 |
| H5 |
C1 |
H6 |
109.543 |
|
H7 |
C2 |
H8 |
109.543 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.508 |
|
|
|
| 2 |
C |
-0.508 |
|
|
|
| 3 |
Cl |
-0.072 |
|
|
|
| 4 |
Cl |
-0.072 |
|
|
|
| 5 |
H |
0.290 |
|
|
|
| 6 |
H |
0.290 |
|
|
|
| 7 |
H |
0.290 |
|
|
|
| 8 |
H |
0.290 |
|
|
|
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 |
-37.702 |
2.060 |
0.000 |
| y |
2.060 |
-45.913 |
0.000 |
| z |
0.000 |
0.000 |
-37.999 |
|
| Traceless |
| | x | y | z |
| x |
4.254 |
2.060 |
0.000 |
| y |
2.060 |
-8.063 |
0.000 |
| z |
0.000 |
0.000 |
3.809 |
|
| Polar |
| 3z2-r2 | 7.617 |
| x2-y2 | 8.211 |
| xy | 2.060 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.519 |
-1.628 |
0.000 |
| y |
-1.628 |
9.291 |
0.000 |
| z |
0.000 |
0.000 |
4.318 |
<r2> (average value of r
2) Å
2
| <r2> |
200.401 |
| (<r2>)1/2 |
14.156 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -999.121987 |
| Energy at 298.15K | -999.126819 |
| HF Energy | -999.121987 |
| Nuclear repulsion energy | 202.752006 |
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 B1B95/6-311G*
| 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 |
3174 |
3042 |
1.48 |
|
|
|
| 2 |
A |
3117 |
2988 |
27.61 |
|
|
|
| 3 |
A |
1483 |
1422 |
1.11 |
|
|
|
| 4 |
A |
1369 |
1313 |
22.04 |
|
|
|
| 5 |
A |
1256 |
1204 |
2.02 |
|
|
|
| 6 |
A |
1071 |
1026 |
0.47 |
|
|
|
| 7 |
A |
971 |
931 |
14.31 |
|
|
|
| 8 |
A |
679 |
651 |
21.53 |
|
|
|
| 9 |
A |
260 |
249 |
0.90 |
|
|
|
| 10 |
A |
115 |
110 |
0.82 |
|
|
|
| 11 |
B |
3187 |
3055 |
7.76 |
|
|
|
| 12 |
B |
3109 |
2980 |
4.61 |
|
|
|
| 13 |
B |
1478 |
1417 |
12.28 |
|
|
|
| 14 |
B |
1344 |
1288 |
38.92 |
|
|
|
| 15 |
B |
1190 |
1141 |
3.09 |
|
|
|
| 16 |
B |
909 |
871 |
26.02 |
|
|
|
| 17 |
B |
701 |
672 |
28.83 |
|
|
|
| 18 |
B |
411 |
394 |
8.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12912.0 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 12377.5 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 B1B95/6-311G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.293 |
0.693 |
0.893 |
| C2 |
-0.293 |
-0.693 |
0.893 |
| Cl3 |
-0.293 |
1.683 |
-0.470 |
| Cl4 |
0.293 |
-1.683 |
-0.470 |
| H5 |
0.001 |
1.207 |
1.807 |
| H6 |
1.377 |
0.663 |
0.828 |
| H7 |
-0.001 |
-1.207 |
1.807 |
| H8 |
-1.377 |
-0.663 |
0.828 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5043 | 1.7847 | 2.7396 | 1.0886 | 1.0865 | 2.1288 | 2.1526 |
C2 | 1.5043 | | 2.7396 | 1.7847 | 2.1288 | 2.1526 | 1.0886 | 1.0865 | Cl3 | 1.7847 | 2.7396 | | 3.4173 | 2.3454 | 2.3487 | 3.6917 | 2.8928 | Cl4 | 2.7396 | 1.7847 | 3.4173 | | 3.6917 | 2.8928 | 2.3454 | 2.3487 | H5 | 1.0886 | 2.1288 | 2.3454 | 3.6917 | | 1.7742 | 2.4147 | 2.5219 | H6 | 1.0865 | 2.1526 | 2.3487 | 2.8928 | 1.7742 | | 2.5219 | 3.0575 | H7 | 2.1288 | 1.0886 | 3.6917 | 2.3454 | 2.4147 | 2.5219 | | 1.7742 | H8 | 2.1526 | 1.0865 | 2.8928 | 2.3487 | 2.5219 | 3.0575 | 1.7742 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.525 |
|
C1 |
C2 |
H7 |
109.327 |
| C1 |
C2 |
H8 |
111.359 |
|
C2 |
C1 |
Cl3 |
112.525 |
| C2 |
C1 |
H5 |
109.327 |
|
C2 |
C1 |
H6 |
111.359 |
| Cl3 |
C1 |
H5 |
106.914 |
|
Cl3 |
C1 |
H6 |
107.260 |
| Cl4 |
C2 |
H7 |
106.914 |
|
Cl4 |
C2 |
H8 |
107.260 |
| H5 |
C1 |
H6 |
109.312 |
|
H7 |
C2 |
H8 |
109.312 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.507 |
|
|
|
| 2 |
C |
-0.507 |
|
|
|
| 3 |
Cl |
-0.060 |
|
|
|
| 4 |
Cl |
-0.060 |
|
|
|
| 5 |
H |
0.276 |
|
|
|
| 6 |
H |
0.291 |
|
|
|
| 7 |
H |
0.276 |
|
|
|
| 8 |
H |
0.291 |
|
|
|
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 |
2.943 |
2.943 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.871 |
1.207 |
0.000 |
| y |
1.207 |
-43.031 |
0.000 |
| z |
0.000 |
0.000 |
-35.631 |
|
| Traceless |
| | x | y | z |
| x |
1.460 |
1.207 |
0.000 |
| y |
1.207 |
-6.280 |
0.000 |
| z |
0.000 |
0.000 |
4.820 |
|
| Polar |
| 3z2-r2 | 9.640 |
| x2-y2 | 5.160 |
| xy | 1.207 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.783 |
-0.613 |
0.000 |
| y |
-0.613 |
6.988 |
0.000 |
| z |
0.000 |
0.000 |
6.644 |
<r2> (average value of r
2) Å
2
| <r2> |
162.907 |
| (<r2>)1/2 |
12.763 |