Jump to
S1C2
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -999.097449 |
| Energy at 298.15K | -999.102118 |
| Nuclear repulsion energy | 194.494963 |
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/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 |
Ag |
3117 |
2996 |
0.00 |
|
|
|
| 2 |
Ag |
1466 |
1409 |
0.00 |
|
|
|
| 3 |
Ag |
1309 |
1259 |
0.00 |
|
|
|
| 4 |
Ag |
1089 |
1046 |
0.00 |
|
|
|
| 5 |
Ag |
775 |
745 |
0.00 |
|
|
|
| 6 |
Ag |
301 |
289 |
0.00 |
|
|
|
| 7 |
Au |
3203 |
3079 |
3.24 |
|
|
|
| 8 |
Au |
1118 |
1075 |
1.72 |
|
|
|
| 9 |
Au |
775 |
745 |
3.31 |
|
|
|
| 10 |
Au |
120 |
116 |
6.53 |
|
|
|
| 11 |
Bg |
3181 |
3057 |
0.00 |
|
|
|
| 12 |
Bg |
1275 |
1225 |
0.00 |
|
|
|
| 13 |
Bg |
991 |
952 |
0.00 |
|
|
|
| 14 |
Bu |
3123 |
3002 |
14.50 |
|
|
|
| 15 |
Bu |
1461 |
1404 |
5.84 |
|
|
|
| 16 |
Bu |
1222 |
1175 |
32.03 |
|
|
|
| 17 |
Bu |
739 |
710 |
98.61 |
|
|
|
| 18 |
Bu |
211 |
203 |
9.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12737.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 12243.1 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/cc-pVDZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.473 |
0.588 |
0.000 |
| C2 |
-0.473 |
-0.588 |
0.000 |
| Cl3 |
-0.473 |
2.111 |
0.000 |
| Cl4 |
0.473 |
-2.111 |
0.000 |
| H5 |
1.106 |
0.593 |
0.894 |
| H6 |
1.106 |
0.593 |
-0.894 |
| H7 |
-1.106 |
-0.593 |
0.894 |
| H8 |
-1.106 |
-0.593 |
-0.894 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5090 | 1.7939 | 2.6987 | 1.0956 | 1.0956 | 2.1654 | 2.1654 |
C2 | 1.5090 | | 2.6987 | 1.7939 | 2.1654 | 2.1654 | 1.0956 | 1.0956 | Cl3 | 1.7939 | 2.6987 | | 4.3273 | 2.3665 | 2.3665 | 2.9177 | 2.9177 | Cl4 | 2.6987 | 1.7939 | 4.3273 | | 2.9177 | 2.9177 | 2.3665 | 2.3665 | H5 | 1.0956 | 2.1654 | 2.3665 | 2.9177 | | 1.7885 | 2.5106 | 3.0825 | H6 | 1.0956 | 2.1654 | 2.3665 | 2.9177 | 1.7885 | | 3.0825 | 2.5106 | H7 | 2.1654 | 1.0956 | 2.9177 | 2.3665 | 2.5106 | 3.0825 | | 1.7885 | H8 | 2.1654 | 1.0956 | 2.9177 | 2.3665 | 3.0825 | 2.5106 | 1.7885 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.280 |
|
C1 |
C2 |
H7 |
111.494 |
| C1 |
C2 |
H8 |
111.494 |
|
C2 |
C1 |
Cl3 |
109.280 |
| C2 |
C1 |
H5 |
111.494 |
|
C2 |
C1 |
H6 |
111.494 |
| Cl3 |
C1 |
H5 |
107.496 |
|
Cl3 |
C1 |
H6 |
107.496 |
| Cl4 |
C2 |
H7 |
107.496 |
|
Cl4 |
C2 |
H8 |
107.496 |
| H5 |
C1 |
H6 |
109.417 |
|
H7 |
C2 |
H8 |
109.417 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.067 |
|
|
|
| 2 |
C |
-0.067 |
|
|
|
| 3 |
Cl |
-0.123 |
|
|
|
| 4 |
Cl |
-0.123 |
|
|
|
| 5 |
H |
0.095 |
|
|
|
| 6 |
H |
0.095 |
|
|
|
| 7 |
H |
0.095 |
|
|
|
| 8 |
H |
0.095 |
|
|
|
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 |
-36.827 |
1.866 |
0.000 |
| y |
1.866 |
-44.215 |
0.000 |
| z |
0.000 |
0.000 |
-37.141 |
|
| Traceless |
| | x | y | z |
| x |
3.850 |
1.866 |
0.000 |
| y |
1.866 |
-7.231 |
0.000 |
| z |
0.000 |
0.000 |
3.380 |
|
| Polar |
| 3z2-r2 | 6.761 |
| x2-y2 | 7.388 |
| xy | 1.866 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.414 |
-1.431 |
0.000 |
| y |
-1.431 |
8.746 |
0.000 |
| z |
0.000 |
0.000 |
4.364 |
<r2> (average value of r
2) Å
2
| <r2> |
200.105 |
| (<r2>)1/2 |
14.146 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -999.096309 |
| Energy at 298.15K | -999.101121 |
| HF Energy | -999.096309 |
| Nuclear repulsion energy | 202.536178 |
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/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 |
3175 |
3052 |
0.60 |
|
|
|
| 2 |
A |
3112 |
2992 |
20.69 |
|
|
|
| 3 |
A |
1445 |
1389 |
1.32 |
|
|
|
| 4 |
A |
1329 |
1277 |
20.25 |
|
|
|
| 5 |
A |
1222 |
1175 |
0.96 |
|
|
|
| 6 |
A |
1062 |
1021 |
2.16 |
|
|
|
| 7 |
A |
954 |
917 |
11.53 |
|
|
|
| 8 |
A |
682 |
656 |
19.64 |
|
|
|
| 9 |
A |
258 |
248 |
0.84 |
|
|
|
| 10 |
A |
113 |
108 |
0.78 |
|
|
|
| 11 |
B |
3187 |
3064 |
3.68 |
|
|
|
| 12 |
B |
3104 |
2983 |
3.43 |
|
|
|
| 13 |
B |
1439 |
1383 |
10.77 |
|
|
|
| 14 |
B |
1295 |
1245 |
37.80 |
|
|
|
| 15 |
B |
1150 |
1105 |
0.72 |
|
|
|
| 16 |
B |
889 |
854 |
20.42 |
|
|
|
| 17 |
B |
701 |
674 |
25.22 |
|
|
|
| 18 |
B |
410 |
394 |
8.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12763.8 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 12268.6 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/cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.290 |
0.694 |
0.898 |
| C2 |
-0.290 |
-0.694 |
0.898 |
| Cl3 |
-0.290 |
1.681 |
-0.473 |
| Cl4 |
0.290 |
-1.681 |
-0.473 |
| H5 |
-0.011 |
1.214 |
1.816 |
| H6 |
1.384 |
0.669 |
0.840 |
| H7 |
0.011 |
-1.214 |
1.816 |
| H8 |
-1.384 |
-0.669 |
0.840 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5055 | 1.7858 | 2.7424 | 1.0970 | 1.0951 | 2.1362 | 2.1600 |
C2 | 1.5055 | | 2.7424 | 1.7858 | 2.1362 | 2.1600 | 1.0970 | 1.0951 | Cl3 | 1.7858 | 2.7424 | | 3.4116 | 2.3525 | 2.3557 | 3.7025 | 2.9052 | Cl4 | 2.7424 | 1.7858 | 3.4116 | | 3.7025 | 2.9052 | 2.3525 | 2.3557 | H5 | 1.0970 | 2.1362 | 2.3525 | 3.7025 | | 1.7872 | 2.4280 | 2.5267 | H6 | 1.0951 | 2.1600 | 2.3557 | 2.9052 | 1.7872 | | 2.5267 | 3.0740 | H7 | 2.1362 | 1.0970 | 3.7025 | 2.3525 | 2.4280 | 2.5267 | | 1.7872 | H8 | 2.1600 | 1.0951 | 2.9052 | 2.3557 | 2.5267 | 3.0740 | 1.7872 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.586 |
|
C1 |
C2 |
H7 |
109.328 |
| C1 |
C2 |
H8 |
111.337 |
|
C2 |
C1 |
Cl3 |
112.586 |
| C2 |
C1 |
H5 |
109.328 |
|
C2 |
C1 |
H6 |
111.337 |
| Cl3 |
C1 |
H5 |
106.942 |
|
Cl3 |
C1 |
H6 |
107.272 |
| Cl4 |
C2 |
H7 |
106.942 |
|
Cl4 |
C2 |
H8 |
107.272 |
| H5 |
C1 |
H6 |
109.230 |
|
H7 |
C2 |
H8 |
109.230 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.070 |
|
|
|
| 2 |
C |
-0.070 |
|
|
|
| 3 |
Cl |
-0.115 |
|
|
|
| 4 |
Cl |
-0.115 |
|
|
|
| 5 |
H |
0.088 |
|
|
|
| 6 |
H |
0.096 |
|
|
|
| 7 |
H |
0.088 |
|
|
|
| 8 |
H |
0.096 |
|
|
|
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 |
2.738 |
2.738 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.016 |
1.085 |
0.000 |
| y |
1.085 |
-41.579 |
0.000 |
| z |
0.000 |
0.000 |
-34.904 |
|
| Traceless |
| | x | y | z |
| x |
1.225 |
1.085 |
0.000 |
| y |
1.085 |
-5.619 |
0.000 |
| z |
0.000 |
0.000 |
4.394 |
|
| Polar |
| 3z2-r2 | 8.788 |
| x2-y2 | 4.562 |
| xy | 1.085 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.760 |
-0.523 |
0.000 |
| y |
-0.523 |
6.739 |
0.000 |
| z |
0.000 |
0.000 |
6.448 |
<r2> (average value of r
2) Å
2
| <r2> |
162.309 |
| (<r2>)1/2 |
12.740 |