Jump to
S1C2
Energy calculated at B97D3/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -999.103242 |
| Energy at 298.15K | |
| HF Energy | -999.103242 |
| Nuclear repulsion energy | 193.123503 |
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 B97D3/daug-cc-pVTZ
| 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 |
3046 |
3046 |
0.00 |
192.98 |
0.03 |
0.06 |
| 2 |
Ag |
1461 |
1461 |
0.00 |
7.01 |
0.75 |
0.86 |
| 3 |
Ag |
1295 |
1295 |
0.00 |
13.47 |
0.35 |
0.52 |
| 4 |
Ag |
1039 |
1039 |
0.00 |
3.86 |
0.58 |
0.74 |
| 5 |
Ag |
710 |
710 |
0.00 |
64.30 |
0.23 |
0.38 |
| 6 |
Ag |
289 |
289 |
0.00 |
6.06 |
0.21 |
0.34 |
| 7 |
Au |
3125 |
3125 |
3.86 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1113 |
1113 |
1.10 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
766 |
766 |
2.17 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
114 |
114 |
6.52 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3101 |
3101 |
0.00 |
88.09 |
0.75 |
0.86 |
| 12 |
Bg |
1268 |
1268 |
0.00 |
2.76 |
0.75 |
0.86 |
| 13 |
Bg |
986 |
986 |
0.00 |
1.07 |
0.75 |
0.86 |
| 14 |
Bu |
3055 |
3055 |
16.08 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1464 |
1464 |
5.82 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1225 |
1225 |
30.66 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
668 |
668 |
111.01 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
210 |
210 |
9.62 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12467.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12467.5 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 B97D3/daug-cc-pVTZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.479 |
0.586 |
0.000 |
| C2 |
-0.479 |
-0.586 |
0.000 |
| Cl3 |
-0.479 |
2.128 |
0.000 |
| Cl4 |
0.479 |
-2.128 |
0.000 |
| H5 |
1.104 |
0.597 |
0.893 |
| H6 |
1.104 |
0.597 |
-0.893 |
| H7 |
-1.104 |
-0.597 |
0.893 |
| H8 |
-1.104 |
-0.597 |
-0.893 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5136 | 1.8163 | 2.7138 | 1.0895 | 1.0895 | 2.1684 | 2.1684 |
C2 | 1.5136 | | 2.7138 | 1.8163 | 2.1684 | 2.1684 | 1.0895 | 1.0895 | Cl3 | 1.8163 | 2.7138 | | 4.3631 | 2.3767 | 2.3767 | 2.9349 | 2.9349 | Cl4 | 2.7138 | 1.8163 | 4.3631 | | 2.9349 | 2.9349 | 2.3767 | 2.3767 | H5 | 1.0895 | 2.1684 | 2.3767 | 2.9349 | | 1.7854 | 2.5099 | 3.0801 | H6 | 1.0895 | 2.1684 | 2.3767 | 2.9349 | 1.7854 | | 3.0801 | 2.5099 | H7 | 2.1684 | 1.0895 | 2.9349 | 2.3767 | 2.5099 | 3.0801 | | 1.7854 | H8 | 2.1684 | 1.0895 | 2.9349 | 2.3767 | 3.0801 | 2.5099 | 1.7854 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.835 |
|
C1 |
C2 |
H7 |
111.786 |
| C1 |
C2 |
H8 |
111.786 |
|
C2 |
C1 |
Cl3 |
108.835 |
| C2 |
C1 |
H5 |
111.786 |
|
C2 |
C1 |
H6 |
111.786 |
| Cl3 |
C1 |
H5 |
107.081 |
|
Cl3 |
C1 |
H6 |
107.081 |
| Cl4 |
C2 |
H7 |
107.081 |
|
Cl4 |
C2 |
H8 |
107.081 |
| H5 |
C1 |
H6 |
110.039 |
|
H7 |
C2 |
H8 |
110.039 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.429 |
|
|
|
| 2 |
C |
0.429 |
|
|
|
| 3 |
Cl |
-0.896 |
|
|
|
| 4 |
Cl |
-0.896 |
|
|
|
| 5 |
H |
0.233 |
|
|
|
| 6 |
H |
0.233 |
|
|
|
| 7 |
H |
0.233 |
|
|
|
| 8 |
H |
0.233 |
|
|
|
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
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.828 |
-1.192 |
0.000 |
| y |
-1.192 |
11.546 |
0.000 |
| z |
0.000 |
0.000 |
6.999 |
<r2> (average value of r
2) Å
2
| <r2> |
203.206 |
| (<r2>)1/2 |
14.255 |
Jump to
S1C1
Energy calculated at B97D3/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -999.100981 |
| Energy at 298.15K | |
| HF Energy | -999.100981 |
| Nuclear repulsion energy | 200.464978 |
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 B97D3/daug-cc-pVTZ
| 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 |
3083 |
3083 |
0.54 |
93.84 |
0.74 |
0.85 |
| 2 |
A |
3028 |
3028 |
26.70 |
269.26 |
0.02 |
0.03 |
| 3 |
A |
1439 |
1439 |
0.58 |
2.63 |
0.75 |
0.86 |
| 4 |
A |
1306 |
1306 |
14.74 |
1.94 |
0.35 |
0.52 |
| 5 |
A |
1198 |
1198 |
0.49 |
6.01 |
0.60 |
0.75 |
| 6 |
A |
1020 |
1020 |
1.44 |
0.67 |
0.69 |
0.82 |
| 7 |
A |
925 |
925 |
11.66 |
3.64 |
0.20 |
0.33 |
| 8 |
A |
624 |
624 |
19.32 |
19.25 |
0.04 |
0.08 |
| 9 |
A |
258 |
258 |
1.13 |
1.34 |
0.20 |
0.33 |
| 10 |
A |
112 |
112 |
0.80 |
1.06 |
0.67 |
0.80 |
| 11 |
B |
3097 |
3097 |
5.71 |
23.55 |
0.75 |
0.86 |
| 12 |
B |
3019 |
3019 |
3.39 |
39.23 |
0.75 |
0.86 |
| 13 |
B |
1438 |
1438 |
10.90 |
8.62 |
0.75 |
0.86 |
| 14 |
B |
1283 |
1283 |
40.37 |
0.99 |
0.75 |
0.86 |
| 15 |
B |
1137 |
1137 |
0.47 |
1.39 |
0.75 |
0.86 |
| 16 |
B |
874 |
874 |
17.82 |
1.09 |
0.75 |
0.86 |
| 17 |
B |
644 |
644 |
32.43 |
6.09 |
0.75 |
0.86 |
| 18 |
B |
402 |
402 |
9.45 |
1.46 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12442.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12442.8 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 B97D3/daug-cc-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.299 |
0.694 |
0.897 |
| C2 |
-0.299 |
-0.694 |
0.897 |
| Cl3 |
-0.299 |
1.713 |
-0.471 |
| Cl4 |
0.299 |
-1.713 |
-0.471 |
| H5 |
0.011 |
1.211 |
1.816 |
| H6 |
1.386 |
0.664 |
0.818 |
| H7 |
-0.011 |
-1.211 |
1.816 |
| H8 |
-1.386 |
-0.664 |
0.818 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Cl3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5108 | 1.8078 | 2.7682 | 1.0931 | 1.0903 | 2.1370 | 2.1652 |
C2 | 1.5108 | | 2.7682 | 1.8078 | 2.1370 | 2.1652 | 1.0931 | 1.0903 | Cl3 | 1.8078 | 2.7682 | | 3.4772 | 2.3620 | 2.3672 | 3.7230 | 2.9142 | Cl4 | 2.7682 | 1.8078 | 3.4772 | | 3.7230 | 2.9142 | 2.3620 | 2.3672 | H5 | 1.0931 | 2.1370 | 2.3620 | 3.7230 | | 1.7849 | 2.4215 | 2.5414 | H6 | 1.0903 | 2.1652 | 2.3672 | 2.9142 | 1.7849 | | 2.5414 | 3.0735 | H7 | 2.1370 | 1.0931 | 3.7230 | 2.3620 | 2.4215 | 2.5414 | | 1.7849 | H8 | 2.1652 | 1.0903 | 2.9142 | 2.3672 | 2.5414 | 3.0735 | 1.7849 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.747 |
|
C1 |
C2 |
H7 |
109.261 |
| C1 |
C2 |
H8 |
111.679 |
|
C2 |
C1 |
Cl3 |
112.747 |
| C2 |
C1 |
H5 |
109.261 |
|
C2 |
C1 |
H6 |
111.679 |
| Cl3 |
C1 |
H5 |
106.403 |
|
Cl3 |
C1 |
H6 |
106.909 |
| Cl4 |
C2 |
H7 |
106.403 |
|
Cl4 |
C2 |
H8 |
106.909 |
| H5 |
C1 |
H6 |
109.671 |
|
H7 |
C2 |
H8 |
109.671 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.515 |
|
|
|
| 2 |
C |
0.515 |
|
|
|
| 3 |
Cl |
-0.910 |
|
|
|
| 4 |
Cl |
-0.910 |
|
|
|
| 5 |
H |
0.235 |
|
|
|
| 6 |
H |
0.160 |
|
|
|
| 7 |
H |
0.235 |
|
|
|
| 8 |
H |
0.160 |
|
|
|
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 |
2.727 |
2.727 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.300 |
-0.451 |
0.000 |
| y |
-0.451 |
9.691 |
0.000 |
| z |
0.000 |
0.000 |
8.536 |
<r2> (average value of r
2) Å
2
| <r2> |
166.491 |
| (<r2>)1/2 |
12.903 |