Jump to
S1C2
Energy calculated at B1B95/6-31G**
| | hartrees |
| Energy at 0K | -999.057187 |
| Energy at 298.15K | -999.061874 |
| Nuclear repulsion energy | 194.736172 |
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 B1B95/6-31G**
| 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 |
3128 |
2986 |
0.00 |
|
|
|
| 2 |
Ag |
1499 |
1431 |
0.00 |
|
|
|
| 3 |
Ag |
1349 |
1288 |
0.00 |
|
|
|
| 4 |
Ag |
1083 |
1034 |
0.00 |
|
|
|
| 5 |
Ag |
781 |
746 |
0.00 |
|
|
|
| 6 |
Ag |
302 |
288 |
0.00 |
|
|
|
| 7 |
Au |
3212 |
3067 |
3.92 |
|
|
|
| 8 |
Au |
1153 |
1101 |
1.87 |
|
|
|
| 9 |
Au |
780 |
745 |
3.56 |
|
|
|
| 10 |
Au |
124 |
118 |
7.34 |
|
|
|
| 11 |
Bg |
3191 |
3047 |
0.00 |
|
|
|
| 12 |
Bg |
1300 |
1241 |
0.00 |
|
|
|
| 13 |
Bg |
1018 |
972 |
0.00 |
|
|
|
| 14 |
Bu |
3136 |
2994 |
15.21 |
|
|
|
| 15 |
Bu |
1497 |
1429 |
7.49 |
|
|
|
| 16 |
Bu |
1263 |
1206 |
35.05 |
|
|
|
| 17 |
Bu |
742 |
709 |
101.61 |
|
|
|
| 18 |
Bu |
213 |
203 |
10.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12885.0 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 12302.6 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 B1B95/6-31G**
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.474 |
0.588 |
0.000 |
| C2 |
-0.474 |
-0.588 |
0.000 |
| Cl3 |
-0.474 |
2.109 |
0.000 |
| Cl4 |
0.474 |
-2.109 |
0.000 |
| H5 |
1.103 |
0.591 |
0.889 |
| H6 |
1.103 |
0.591 |
-0.889 |
| H7 |
-1.103 |
-0.591 |
0.889 |
| H8 |
-1.103 |
-0.591 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5110 | 1.7919 | 2.6978 | 1.0889 | 1.0889 | 2.1603 | 2.1603 |
C2 | 1.5110 | | 2.6978 | 1.7919 | 2.1603 | 2.1603 | 1.0889 | 1.0889 | Cl3 | 1.7919 | 2.6978 | | 4.3237 | 2.3624 | 2.3624 | 2.9116 | 2.9116 | Cl4 | 2.6978 | 1.7919 | 4.3237 | | 2.9116 | 2.9116 | 2.3624 | 2.3624 | H5 | 1.0889 | 2.1603 | 2.3624 | 2.9116 | | 1.7774 | 2.5025 | 3.0695 | H6 | 1.0889 | 2.1603 | 2.3624 | 2.9116 | 1.7774 | | 3.0695 | 2.5025 | H7 | 2.1603 | 1.0889 | 2.9116 | 2.3624 | 2.5025 | 3.0695 | | 1.7774 | H8 | 2.1603 | 1.0889 | 2.9116 | 2.3624 | 3.0695 | 2.5025 | 1.7774 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.240 |
|
C1 |
C2 |
H7 |
111.353 |
| C1 |
C2 |
H8 |
111.353 |
|
C2 |
C1 |
Cl3 |
109.240 |
| C2 |
C1 |
H5 |
111.353 |
|
C2 |
C1 |
H6 |
111.353 |
| Cl3 |
C1 |
H5 |
107.672 |
|
Cl3 |
C1 |
H6 |
107.672 |
| Cl4 |
C2 |
H7 |
107.672 |
|
Cl4 |
C2 |
H8 |
107.672 |
| H5 |
C1 |
H6 |
109.409 |
|
H7 |
C2 |
H8 |
109.409 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.332 |
|
|
|
| 2 |
C |
-0.332 |
|
|
|
| 3 |
Cl |
-0.060 |
|
|
|
| 4 |
Cl |
-0.060 |
|
|
|
| 5 |
H |
0.196 |
|
|
|
| 6 |
H |
0.196 |
|
|
|
| 7 |
H |
0.196 |
|
|
|
| 8 |
H |
0.196 |
|
|
|
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 |
-36.874 |
2.112 |
0.000 |
| y |
2.112 |
-44.864 |
0.000 |
| z |
0.000 |
0.000 |
-37.215 |
|
| Traceless |
| | x | y | z |
| x |
4.166 |
2.112 |
0.000 |
| y |
2.112 |
-7.819 |
0.000 |
| z |
0.000 |
0.000 |
3.654 |
|
| Polar |
| 3z2-r2 | 7.307 |
| x2-y2 | 7.990 |
| xy | 2.112 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.272 |
-1.447 |
0.000 |
| y |
-1.447 |
8.609 |
0.000 |
| z |
0.000 |
0.000 |
4.389 |
<r2> (average value of r
2) Å
2
| <r2> |
199.941 |
| (<r2>)1/2 |
14.140 |
Jump to
S1C1
Energy calculated at B1B95/6-31G**
| | hartrees |
| Energy at 0K | -999.050756 |
| Energy at 298.15K | -999.055590 |
| HF Energy | -999.050756 |
| Nuclear repulsion energy | 202.537368 |
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 B1B95/6-31G**
| 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 |
3190 |
3046 |
0.70 |
|
|
|
| 2 |
A |
3131 |
2989 |
20.90 |
|
|
|
| 3 |
A |
1499 |
1431 |
0.38 |
|
|
|
| 4 |
A |
1371 |
1309 |
23.87 |
|
|
|
| 5 |
A |
1256 |
1200 |
1.12 |
|
|
|
| 6 |
A |
1073 |
1024 |
0.88 |
|
|
|
| 7 |
A |
976 |
931 |
13.49 |
|
|
|
| 8 |
A |
685 |
654 |
20.38 |
|
|
|
| 9 |
A |
259 |
247 |
0.88 |
|
|
|
| 10 |
A |
114 |
108 |
0.93 |
|
|
|
| 11 |
B |
3203 |
3058 |
4.87 |
|
|
|
| 12 |
B |
3123 |
2982 |
3.37 |
|
|
|
| 13 |
B |
1495 |
1427 |
12.59 |
|
|
|
| 14 |
B |
1345 |
1284 |
40.50 |
|
|
|
| 15 |
B |
1188 |
1134 |
1.30 |
|
|
|
| 16 |
B |
911 |
870 |
21.90 |
|
|
|
| 17 |
B |
708 |
676 |
25.76 |
|
|
|
| 18 |
B |
413 |
394 |
8.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12968.8 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 12382.6 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 B1B95/6-31G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.291 |
0.696 |
0.893 |
| C2 |
-0.291 |
-0.696 |
0.893 |
| Cl3 |
-0.291 |
1.686 |
-0.471 |
| Cl4 |
0.291 |
-1.686 |
-0.471 |
| H5 |
-0.005 |
1.206 |
1.811 |
| H6 |
1.379 |
0.667 |
0.837 |
| H7 |
0.005 |
-1.206 |
1.811 |
| H8 |
-1.379 |
-0.667 |
0.837 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5084 | 1.7835 | 2.7446 | 1.0912 | 1.0891 | 2.1307 | 2.1557 |
C2 | 1.5084 | | 2.7446 | 1.7835 | 2.1307 | 2.1557 | 1.0912 | 1.0891 | Cl3 | 1.7835 | 2.7446 | | 3.4220 | 2.3492 | 2.3532 | 3.6956 | 2.9029 | Cl4 | 2.7446 | 1.7835 | 3.4220 | | 3.6956 | 2.9029 | 2.3492 | 2.3532 | H5 | 1.0912 | 2.1307 | 2.3492 | 3.6956 | | 1.7762 | 2.4118 | 2.5180 | H6 | 1.0891 | 2.1557 | 2.3532 | 2.9029 | 1.7762 | | 2.5180 | 3.0624 | H7 | 2.1307 | 1.0912 | 3.6956 | 2.3492 | 2.4118 | 2.5180 | | 1.7762 | H8 | 2.1557 | 1.0891 | 2.9029 | 2.3532 | 2.5180 | 3.0624 | 1.7762 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.709 |
|
C1 |
C2 |
H7 |
109.043 |
| C1 |
C2 |
H8 |
111.154 |
|
C2 |
C1 |
Cl3 |
112.709 |
| C2 |
C1 |
H5 |
109.043 |
|
C2 |
C1 |
H6 |
111.154 |
| Cl3 |
C1 |
H5 |
107.146 |
|
Cl3 |
C1 |
H6 |
107.540 |
| Cl4 |
C2 |
H7 |
107.146 |
|
Cl4 |
C2 |
H8 |
107.540 |
| H5 |
C1 |
H6 |
109.117 |
|
H7 |
C2 |
H8 |
109.117 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.411 |
|
|
|
| 2 |
C |
-0.411 |
|
|
|
| 3 |
Cl |
-0.047 |
|
|
|
| 4 |
Cl |
-0.047 |
|
|
|
| 5 |
H |
0.223 |
|
|
|
| 6 |
H |
0.235 |
|
|
|
| 7 |
H |
0.223 |
|
|
|
| 8 |
H |
0.235 |
|
|
|
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 |
2.908 |
2.908 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.089 |
1.215 |
0.000 |
| y |
1.215 |
-41.961 |
0.000 |
| z |
0.000 |
0.000 |
-34.949 |
|
| Traceless |
| | x | y | z |
| x |
1.366 |
1.215 |
0.000 |
| y |
1.215 |
-5.942 |
0.000 |
| z |
0.000 |
0.000 |
4.576 |
|
| Polar |
| 3z2-r2 | 9.152 |
| x2-y2 | 4.872 |
| xy | 1.215 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.660 |
-0.577 |
0.000 |
| y |
-0.577 |
6.612 |
0.000 |
| z |
0.000 |
0.000 |
6.268 |
<r2> (average value of r
2) Å
2
| <r2> |
162.765 |
| (<r2>)1/2 |
12.758 |