Jump to
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -998.998999 |
| Energy at 298.15K | -999.003600 |
| Nuclear repulsion energy | 190.185635 |
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 |
3161 |
3014 |
0.00 |
|
|
|
| 2 |
Ag |
1530 |
1459 |
0.00 |
|
|
|
| 3 |
Ag |
1351 |
1289 |
0.00 |
|
|
|
| 4 |
Ag |
1110 |
1059 |
0.00 |
|
|
|
| 5 |
Ag |
717 |
684 |
0.00 |
|
|
|
| 6 |
Ag |
287 |
274 |
0.00 |
|
|
|
| 7 |
Au |
3257 |
3106 |
2.51 |
|
|
|
| 8 |
Au |
1151 |
1097 |
1.30 |
|
|
|
| 9 |
Au |
803 |
765 |
5.37 |
|
|
|
| 10 |
Au |
114 |
108 |
9.85 |
|
|
|
| 11 |
Bg |
3233 |
3084 |
0.00 |
|
|
|
| 12 |
Bg |
1319 |
1257 |
0.00 |
|
|
|
| 13 |
Bg |
1015 |
968 |
0.00 |
|
|
|
| 14 |
Bu |
3169 |
3022 |
7.59 |
|
|
|
| 15 |
Bu |
1528 |
1458 |
14.42 |
|
|
|
| 16 |
Bu |
1284 |
1224 |
28.15 |
|
|
|
| 17 |
Bu |
680 |
649 |
107.58 |
|
|
|
| 18 |
Bu |
203 |
193 |
14.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12954.7 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 12354.9 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 |
0.488 |
0.572 |
0.000 |
| C2 |
-0.488 |
-0.572 |
0.000 |
| Cl3 |
-0.488 |
2.167 |
0.000 |
| Cl4 |
0.488 |
-2.167 |
0.000 |
| H5 |
1.106 |
0.594 |
0.894 |
| H6 |
1.106 |
0.594 |
-0.894 |
| H7 |
-1.106 |
-0.594 |
0.894 |
| H8 |
-1.106 |
-0.594 |
-0.894 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5038 | 1.8704 | 2.7382 | 1.0870 | 1.0870 | 2.1680 | 2.1680 |
C2 | 1.5038 | | 2.7382 | 1.8704 | 2.1680 | 2.1680 | 1.0870 | 1.0870 | Cl3 | 1.8704 | 2.7382 | | 4.4420 | 2.4119 | 2.4119 | 2.9664 | 2.9664 | Cl4 | 2.7382 | 1.8704 | 4.4420 | | 2.9664 | 2.9664 | 2.4119 | 2.4119 | H5 | 1.0870 | 2.1680 | 2.4119 | 2.9664 | | 1.7880 | 2.5111 | 3.0827 | H6 | 1.0870 | 2.1680 | 2.4119 | 2.9664 | 1.7880 | | 3.0827 | 2.5111 | H7 | 2.1680 | 1.0870 | 2.9664 | 2.4119 | 2.5111 | 3.0827 | | 1.7880 | H8 | 2.1680 | 1.0870 | 2.9664 | 2.4119 | 3.0827 | 2.5111 | 1.7880 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.001 |
|
C1 |
C2 |
H7 |
112.622 |
| C1 |
C2 |
H8 |
112.622 |
|
C2 |
C1 |
Cl3 |
108.001 |
| C2 |
C1 |
H5 |
112.622 |
|
C2 |
C1 |
H6 |
112.622 |
| Cl3 |
C1 |
H5 |
106.243 |
|
Cl3 |
C1 |
H6 |
106.243 |
| Cl4 |
C2 |
H7 |
106.243 |
|
Cl4 |
C2 |
H8 |
106.243 |
| H5 |
C1 |
H6 |
110.660 |
|
H7 |
C2 |
H8 |
110.660 |
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 |
-0.460 |
|
|
|
| 2 |
C |
-0.460 |
|
|
|
| 3 |
Cl |
-0.025 |
|
|
|
| 4 |
Cl |
-0.025 |
|
|
|
| 5 |
H |
0.242 |
|
|
|
| 6 |
H |
0.242 |
|
|
|
| 7 |
H |
0.242 |
|
|
|
| 8 |
H |
0.242 |
|
|
|
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 |
-37.188 |
3.014 |
0.000 |
| y |
3.014 |
-47.544 |
0.000 |
| z |
0.000 |
0.000 |
-37.391 |
|
| Traceless |
| | x | y | z |
| x |
5.279 |
3.014 |
0.000 |
| y |
3.014 |
-10.254 |
0.000 |
| z |
0.000 |
0.000 |
4.975 |
|
| Polar |
| 3z2-r2 | 9.949 |
| x2-y2 | 10.355 |
| xy | 3.014 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.865 |
-1.949 |
0.000 |
| y |
-1.949 |
9.037 |
0.000 |
| z |
0.000 |
0.000 |
3.743 |
<r2> (average value of r
2) Å
2
| <r2> |
209.428 |
| (<r2>)1/2 |
14.472 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -998.996106 |
| Energy at 298.15K | -999.000876 |
| HF Energy | -998.996106 |
| Nuclear repulsion energy | 198.061290 |
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 |
3224 |
3075 |
0.12 |
|
|
|
| 2 |
A |
3151 |
3006 |
11.60 |
|
|
|
| 3 |
A |
1510 |
1440 |
1.96 |
|
|
|
| 4 |
A |
1366 |
1303 |
18.40 |
|
|
|
| 5 |
A |
1248 |
1190 |
0.46 |
|
|
|
| 6 |
A |
1094 |
1043 |
2.31 |
|
|
|
| 7 |
A |
973 |
928 |
12.48 |
|
|
|
| 8 |
A |
634 |
605 |
22.28 |
|
|
|
| 9 |
A |
258 |
246 |
1.30 |
|
|
|
| 10 |
A |
111 |
106 |
1.45 |
|
|
|
| 11 |
B |
3237 |
3087 |
1.87 |
|
|
|
| 12 |
B |
3143 |
2997 |
2.01 |
|
|
|
| 13 |
B |
1510 |
1440 |
19.59 |
|
|
|
| 14 |
B |
1349 |
1287 |
35.14 |
|
|
|
| 15 |
B |
1181 |
1126 |
1.13 |
|
|
|
| 16 |
B |
909 |
867 |
22.72 |
|
|
|
| 17 |
B |
655 |
624 |
31.12 |
|
|
|
| 18 |
B |
402 |
384 |
10.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12977.9 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 12377.1 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 |
0.308 |
0.684 |
0.925 |
| C2 |
-0.308 |
-0.684 |
0.925 |
| Cl3 |
-0.308 |
1.726 |
-0.483 |
| Cl4 |
0.308 |
-1.726 |
-0.483 |
| H5 |
0.029 |
1.220 |
1.831 |
| H6 |
1.390 |
0.650 |
0.826 |
| H7 |
-0.029 |
-1.220 |
1.831 |
| H8 |
-1.390 |
-0.650 |
0.826 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4998 | 1.8572 | 2.7910 | 1.0895 | 1.0867 | 2.1355 | 2.1617 |
C2 | 1.4998 | | 2.7910 | 1.8572 | 2.1355 | 2.1617 | 1.0895 | 1.0867 | Cl3 | 1.8572 | 2.7910 | | 3.5072 | 2.3925 | 2.3990 | 3.7570 | 2.9211 | Cl4 | 2.7910 | 1.8572 | 3.5072 | | 3.7570 | 2.9211 | 2.3925 | 2.3990 | H5 | 1.0895 | 2.1355 | 2.3925 | 3.7570 | | 1.7848 | 2.4415 | 2.5541 | H6 | 1.0867 | 2.1617 | 2.3990 | 2.9211 | 1.7848 | | 2.5541 | 3.0691 | H7 | 2.1355 | 1.0895 | 3.7570 | 2.3925 | 2.4415 | 2.5541 | | 1.7848 | H8 | 2.1617 | 1.0867 | 2.9211 | 2.3990 | 2.5541 | 3.0691 | 1.7848 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.049 |
|
C1 |
C2 |
H7 |
110.119 |
| C1 |
C2 |
H8 |
112.408 |
|
C2 |
C1 |
Cl3 |
112.049 |
| C2 |
C1 |
H5 |
110.119 |
|
C2 |
C1 |
H6 |
112.408 |
| Cl3 |
C1 |
H5 |
105.598 |
|
Cl3 |
C1 |
H6 |
106.191 |
| Cl4 |
C2 |
H7 |
105.598 |
|
Cl4 |
C2 |
H8 |
106.191 |
| H5 |
C1 |
H6 |
110.200 |
|
H7 |
C2 |
H8 |
110.200 |
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 |
-0.468 |
|
|
|
| 2 |
C |
-0.468 |
|
|
|
| 3 |
Cl |
-0.010 |
|
|
|
| 4 |
Cl |
-0.010 |
|
|
|
| 5 |
H |
0.233 |
|
|
|
| 6 |
H |
0.245 |
|
|
|
| 7 |
H |
0.233 |
|
|
|
| 8 |
H |
0.245 |
|
|
|
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 |
3.512 |
3.512 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.284 |
1.708 |
0.000 |
| y |
1.708 |
-43.370 |
0.000 |
| z |
0.000 |
0.000 |
-35.221 |
|
| Traceless |
| | x | y | z |
| x |
2.012 |
1.708 |
0.000 |
| y |
1.708 |
-7.118 |
0.000 |
| z |
0.000 |
0.000 |
5.106 |
|
| Polar |
| 3z2-r2 | 10.212 |
| x2-y2 | 6.087 |
| xy | 1.708 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.169 |
-0.791 |
0.000 |
| y |
-0.791 |
6.389 |
0.000 |
| z |
0.000 |
0.000 |
6.184 |
<r2> (average value of r
2) Å
2
| <r2> |
169.382 |
| (<r2>)1/2 |
13.015 |