Jump to
S1C2
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -994.283879 |
| Energy at 298.15K | -994.288550 |
| Nuclear repulsion energy | 192.959020 |
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 B3PW91/3-21G*
| 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 |
3125 |
2998 |
0.00 |
|
|
|
| 2 |
Ag |
1532 |
1470 |
0.00 |
|
|
|
| 3 |
Ag |
1360 |
1305 |
0.00 |
|
|
|
| 4 |
Ag |
1042 |
1000 |
0.00 |
|
|
|
| 5 |
Ag |
747 |
717 |
0.00 |
|
|
|
| 6 |
Ag |
302 |
290 |
0.00 |
|
|
|
| 7 |
Au |
3209 |
3079 |
1.19 |
|
|
|
| 8 |
Au |
1189 |
1141 |
1.70 |
|
|
|
| 9 |
Au |
800 |
768 |
6.99 |
|
|
|
| 10 |
Au |
118 |
113 |
7.64 |
|
|
|
| 11 |
Bg |
3184 |
3055 |
0.00 |
|
|
|
| 12 |
Bg |
1340 |
1286 |
0.00 |
|
|
|
| 13 |
Bg |
1020 |
979 |
0.00 |
|
|
|
| 14 |
Bu |
3134 |
3007 |
8.21 |
|
|
|
| 15 |
Bu |
1536 |
1473 |
17.11 |
|
|
|
| 16 |
Bu |
1298 |
1246 |
21.09 |
|
|
|
| 17 |
Bu |
704 |
676 |
96.62 |
|
|
|
| 18 |
Bu |
219 |
210 |
10.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12930.0 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 12405.0 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 B3PW91/3-21G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.762 |
0.000 |
| C2 |
0.000 |
-0.762 |
0.000 |
| Cl3 |
-1.719 |
1.344 |
0.000 |
| Cl4 |
1.719 |
-1.344 |
0.000 |
| H5 |
0.482 |
1.157 |
0.895 |
| H6 |
0.482 |
1.157 |
-0.895 |
| H7 |
-0.482 |
-1.157 |
0.895 |
| H8 |
-0.482 |
-1.157 |
-0.895 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5237 | 1.8150 | 2.7183 | 1.0908 | 1.0908 | 2.1718 | 2.1718 |
C2 | 1.5237 | | 2.7183 | 1.8150 | 2.1718 | 2.1718 | 1.0908 | 1.0908 | Cl3 | 1.8150 | 2.7183 | | 4.3641 | 2.3835 | 2.3835 | 2.9304 | 2.9304 | Cl4 | 2.7183 | 1.8150 | 4.3641 | | 2.9304 | 2.9304 | 2.3835 | 2.3835 | H5 | 1.0908 | 2.1718 | 2.3835 | 2.9304 | | 1.7905 | 2.5071 | 3.0808 | H6 | 1.0908 | 2.1718 | 2.3835 | 2.9304 | 1.7905 | | 3.0808 | 2.5071 | H7 | 2.1718 | 1.0908 | 2.9304 | 2.3835 | 2.5071 | 3.0808 | | 1.7905 | H8 | 2.1718 | 1.0908 | 2.9304 | 2.3835 | 3.0808 | 2.5071 | 1.7905 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.696 |
|
C1 |
C2 |
H7 |
111.252 |
| C1 |
C2 |
H8 |
111.252 |
|
C2 |
C1 |
Cl3 |
108.696 |
| C2 |
C1 |
H5 |
111.252 |
|
C2 |
C1 |
H6 |
111.252 |
| Cl3 |
C1 |
H5 |
107.589 |
|
Cl3 |
C1 |
H6 |
107.589 |
| Cl4 |
C2 |
H7 |
107.589 |
|
Cl4 |
C2 |
H8 |
107.589 |
| H5 |
C1 |
H6 |
110.308 |
|
H7 |
C2 |
H8 |
110.308 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.533 |
|
|
|
| 2 |
C |
-0.533 |
|
|
|
| 3 |
Cl |
-0.042 |
|
|
|
| 4 |
Cl |
-0.042 |
|
|
|
| 5 |
H |
0.288 |
|
|
|
| 6 |
H |
0.288 |
|
|
|
| 7 |
H |
0.288 |
|
|
|
| 8 |
H |
0.288 |
|
|
|
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 |
-42.743 |
4.591 |
0.000 |
| y |
4.591 |
-40.140 |
0.000 |
| z |
0.000 |
0.000 |
-37.604 |
|
| Traceless |
| | x | y | z |
| x |
-3.871 |
4.591 |
0.000 |
| y |
4.591 |
0.033 |
0.000 |
| z |
0.000 |
0.000 |
3.838 |
|
| Polar |
| 3z2-r2 | 7.675 |
| x2-y2 | -2.602 |
| xy | 4.591 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
203.427 |
| (<r2>)1/2 |
14.263 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -994.281353 |
| Energy at 298.15K | -994.286168 |
| HF Energy | -994.281353 |
| Nuclear repulsion energy | 201.105258 |
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 B3PW91/3-21G*
| 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 |
3168 |
3040 |
0.12 |
|
|
|
| 2 |
A |
3110 |
2984 |
12.56 |
|
|
|
| 3 |
A |
1514 |
1452 |
1.60 |
|
|
|
| 4 |
A |
1369 |
1313 |
14.14 |
|
|
|
| 5 |
A |
1263 |
1211 |
0.86 |
|
|
|
| 6 |
A |
1040 |
997 |
0.66 |
|
|
|
| 7 |
A |
962 |
923 |
17.18 |
|
|
|
| 8 |
A |
651 |
624 |
19.45 |
|
|
|
| 9 |
A |
267 |
256 |
1.09 |
|
|
|
| 10 |
A |
113 |
109 |
0.98 |
|
|
|
| 11 |
B |
3184 |
3054 |
1.58 |
|
|
|
| 12 |
B |
3102 |
2976 |
2.22 |
|
|
|
| 13 |
B |
1520 |
1458 |
22.17 |
|
|
|
| 14 |
B |
1358 |
1303 |
23.12 |
|
|
|
| 15 |
B |
1210 |
1161 |
1.36 |
|
|
|
| 16 |
B |
911 |
874 |
23.96 |
|
|
|
| 17 |
B |
672 |
645 |
25.16 |
|
|
|
| 18 |
B |
422 |
405 |
8.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12915.9 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 12391.5 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 B3PW91/3-21G*
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.300 |
0.698 |
0.911 |
| C2 |
-0.300 |
-0.698 |
0.911 |
| Cl3 |
-0.300 |
1.687 |
-0.478 |
| Cl4 |
0.300 |
-1.687 |
-0.478 |
| H5 |
0.006 |
1.222 |
1.825 |
| H6 |
1.388 |
0.659 |
0.838 |
| H7 |
-0.006 |
-1.222 |
1.825 |
| H8 |
-1.388 |
-0.659 |
0.838 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5205 | 1.8074 | 2.7602 | 1.0940 | 1.0914 | 2.1492 | 2.1678 |
C2 | 1.5205 | | 2.7602 | 1.8074 | 2.1492 | 2.1678 | 1.0940 | 1.0914 | Cl3 | 1.8074 | 2.7602 | | 3.4268 | 2.3694 | 2.3749 | 3.7221 | 2.9012 | Cl4 | 2.7602 | 1.8074 | 3.4268 | | 3.7221 | 2.9012 | 2.3694 | 2.3749 | H5 | 1.0940 | 2.1492 | 2.3694 | 3.7221 | | 1.7897 | 2.4447 | 2.5414 | H6 | 1.0914 | 2.1678 | 2.3749 | 2.9012 | 1.7897 | | 2.5414 | 3.0737 | H7 | 2.1492 | 1.0940 | 3.7221 | 2.3694 | 2.4447 | 2.5414 | | 1.7897 | H8 | 2.1678 | 1.0914 | 2.9012 | 2.3749 | 2.5414 | 3.0737 | 1.7897 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
111.787 |
|
C1 |
C2 |
H7 |
109.499 |
| C1 |
C2 |
H8 |
111.126 |
|
C2 |
C1 |
Cl3 |
111.787 |
| C2 |
C1 |
H5 |
109.499 |
|
C2 |
C1 |
H6 |
111.126 |
| Cl3 |
C1 |
H5 |
106.918 |
|
Cl3 |
C1 |
H6 |
107.441 |
| Cl4 |
C2 |
H7 |
106.918 |
|
Cl4 |
C2 |
H8 |
107.441 |
| H5 |
C1 |
H6 |
109.963 |
|
H7 |
C2 |
H8 |
109.963 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.536 |
|
|
|
| 2 |
C |
-0.536 |
|
|
|
| 3 |
Cl |
-0.030 |
|
|
|
| 4 |
Cl |
-0.030 |
|
|
|
| 5 |
H |
0.278 |
|
|
|
| 6 |
H |
0.288 |
|
|
|
| 7 |
H |
0.278 |
|
|
|
| 8 |
H |
0.288 |
|
|
|
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 |
3.023 |
3.023 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.432 |
1.288 |
0.000 |
| y |
1.288 |
-42.452 |
0.000 |
| z |
0.000 |
0.000 |
-35.208 |
|
| Traceless |
| | x | y | z |
| x |
1.398 |
1.288 |
0.000 |
| y |
1.288 |
-6.132 |
0.000 |
| z |
0.000 |
0.000 |
4.734 |
|
| Polar |
| 3z2-r2 | 9.468 |
| x2-y2 | 5.020 |
| xy | 1.288 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.408 |
-0.624 |
0.000 |
| y |
-0.624 |
6.353 |
0.000 |
| z |
0.000 |
0.000 |
6.099 |
<r2> (average value of r
2) Å
2
| <r2> |
164.213 |
| (<r2>)1/2 |
12.815 |