Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-31G**
| | hartrees |
| Energy at 0K | -3109.805846 |
| Energy at 298.15K | |
| HF Energy | -3109.617198 |
| Nuclear repulsion energy | 287.850169 |
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 B2PLYP=FULLultrafine/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' |
3165 |
3165 |
8.17 |
28.90 |
0.08 |
0.14 |
| 2 |
A' |
3153 |
3153 |
2.87 |
116.53 |
0.08 |
0.15 |
| 3 |
A' |
1527 |
1527 |
1.51 |
13.48 |
0.75 |
0.86 |
| 4 |
A' |
1522 |
1522 |
4.62 |
3.98 |
0.74 |
0.85 |
| 5 |
A' |
1353 |
1353 |
3.20 |
13.67 |
0.55 |
0.71 |
| 6 |
A' |
1253 |
1253 |
48.13 |
2.55 |
0.43 |
0.60 |
| 7 |
A' |
1085 |
1085 |
1.28 |
8.29 |
0.75 |
0.86 |
| 8 |
A' |
756 |
756 |
29.69 |
47.62 |
0.30 |
0.46 |
| 9 |
A' |
649 |
649 |
56.11 |
11.53 |
0.25 |
0.41 |
| 10 |
A' |
251 |
251 |
0.92 |
5.19 |
0.33 |
0.50 |
| 11 |
A' |
195 |
195 |
7.51 |
0.20 |
0.29 |
0.45 |
| 12 |
A" |
3245 |
3245 |
1.89 |
10.84 |
0.75 |
0.86 |
| 13 |
A" |
3219 |
3219 |
0.78 |
83.13 |
0.75 |
0.86 |
| 14 |
A" |
1318 |
1318 |
0.06 |
9.11 |
0.75 |
0.86 |
| 15 |
A" |
1150 |
1150 |
2.18 |
0.37 |
0.75 |
0.86 |
| 16 |
A" |
992 |
992 |
0.13 |
8.15 |
0.75 |
0.86 |
| 17 |
A" |
777 |
777 |
3.22 |
0.03 |
0.75 |
0.86 |
| 18 |
A" |
114 |
114 |
5.90 |
0.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12862.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12862.3 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 B2PLYP=FULLultrafine/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.656 |
0.000 |
| C2 |
1.231 |
-0.222 |
0.000 |
| Br3 |
-1.594 |
-0.495 |
0.000 |
| Cl4 |
2.706 |
0.815 |
0.000 |
| H5 |
-0.063 |
1.273 |
0.891 |
| H6 |
-0.063 |
1.273 |
-0.891 |
| H7 |
1.270 |
-0.848 |
0.888 |
| H8 |
1.270 |
-0.848 |
-0.888 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5119 | 1.9662 | 2.7106 | 1.0858 | 1.0858 | 2.1595 | 2.1595 |
C2 | 1.5119 | | 2.8383 | 1.8033 | 2.1684 | 2.1684 | 1.0868 | 1.0868 | Br3 | 1.9662 | 2.8383 | | 4.4954 | 2.5030 | 2.5030 | 3.0196 | 3.0196 | Cl4 | 2.7106 | 1.8033 | 4.4954 | | 2.9442 | 2.9442 | 2.3698 | 2.3698 | H5 | 1.0858 | 2.1684 | 2.5030 | 2.9442 | | 1.7826 | 2.5049 | 3.0723 | H6 | 1.0858 | 2.1684 | 2.5030 | 2.9442 | 1.7826 | | 3.0723 | 2.5049 | H7 | 2.1595 | 1.0868 | 3.0196 | 2.3698 | 2.5049 | 3.0723 | | 1.7750 | H8 | 2.1595 | 1.0868 | 3.0196 | 2.3698 | 3.0723 | 2.5049 | 1.7750 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.382 |
|
C1 |
C2 |
H7 |
111.345 |
| C1 |
C2 |
H8 |
111.345 |
|
C2 |
C1 |
Br3 |
108.679 |
| C2 |
C1 |
Cl4 |
38.871 |
|
C2 |
C1 |
H6 |
112.139 |
| Br3 |
C1 |
H5 |
106.607 |
|
Br3 |
C1 |
H6 |
106.607 |
| Cl4 |
C2 |
H7 |
107.564 |
|
Cl4 |
C2 |
H8 |
107.564 |
| H5 |
C1 |
H6 |
110.349 |
|
H7 |
C2 |
H8 |
109.494 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.203 |
|
|
|
| 2 |
C |
-0.287 |
|
|
|
| 3 |
Br |
-0.137 |
|
|
|
| 4 |
Cl |
-0.073 |
|
|
|
| 5 |
H |
0.173 |
|
|
|
| 6 |
H |
0.173 |
|
|
|
| 7 |
H |
0.177 |
|
|
|
| 8 |
H |
0.177 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.153 |
-0.035 |
0.000 |
0.157 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.376 |
-2.292 |
-0.007 |
| y |
-2.292 |
-43.215 |
-0.002 |
| z |
-0.007 |
-0.002 |
-43.446 |
|
| Traceless |
| | x | y | z |
| x |
-7.046 |
-2.292 |
-0.007 |
| y |
-2.292 |
3.697 |
-0.002 |
| z |
-0.007 |
-0.002 |
3.349 |
|
| Polar |
| 3z2-r2 | 6.699 |
| x2-y2 | -7.162 |
| xy | -2.292 |
| xz | -0.007 |
| yz | -0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.875 |
1.971 |
-0.000 |
| y |
1.971 |
6.279 |
-0.000 |
| z |
-0.000 |
-0.000 |
5.102 |
<r2> (average value of r
2) Å
2
| <r2> |
284.881 |
| (<r2>)1/2 |
16.878 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-31G**
| | hartrees |
| Energy at 0K | -3109.803022 |
| Energy at 298.15K | |
| HF Energy | -3109.614144 |
| Nuclear repulsion energy | 304.505921 |
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 B2PLYP=FULLultrafine/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 |
3222 |
3222 |
1.84 |
42.92 |
0.75 |
0.86 |
| 2 |
A |
3200 |
3200 |
1.90 |
79.96 |
0.75 |
0.86 |
| 3 |
A |
3145 |
3145 |
11.21 |
133.23 |
0.05 |
0.10 |
| 4 |
A |
3126 |
3126 |
10.08 |
103.03 |
0.21 |
0.34 |
| 5 |
A |
1508 |
1508 |
1.58 |
7.77 |
0.71 |
0.83 |
| 6 |
A |
1499 |
1499 |
8.22 |
15.83 |
0.75 |
0.86 |
| 7 |
A |
1369 |
1369 |
28.00 |
3.56 |
0.75 |
0.86 |
| 8 |
A |
1321 |
1321 |
51.66 |
1.53 |
0.52 |
0.69 |
| 9 |
A |
1235 |
1235 |
3.89 |
16.47 |
0.75 |
0.85 |
| 10 |
A |
1168 |
1168 |
1.53 |
5.93 |
0.73 |
0.84 |
| 11 |
A |
1059 |
1059 |
1.57 |
3.79 |
0.75 |
0.86 |
| 12 |
A |
954 |
954 |
8.29 |
6.30 |
0.45 |
0.62 |
| 13 |
A |
885 |
885 |
18.65 |
1.54 |
0.71 |
0.83 |
| 14 |
A |
690 |
690 |
19.94 |
10.32 |
0.41 |
0.58 |
| 15 |
A |
580 |
580 |
12.28 |
15.68 |
0.21 |
0.34 |
| 16 |
A |
391 |
391 |
8.02 |
2.59 |
0.71 |
0.83 |
| 17 |
A |
244 |
244 |
1.22 |
1.08 |
0.32 |
0.49 |
| 18 |
A |
103 |
103 |
0.56 |
1.31 |
0.73 |
0.84 |
Unscaled Zero Point Vibrational Energy (zpe) 12847.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12847.7 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 B2PLYP=FULLultrafine/6-31G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
1.118 |
-0.383 |
| C2 |
1.286 |
0.906 |
0.402 |
| Br3 |
-1.351 |
-0.227 |
0.036 |
| Cl4 |
2.159 |
-0.583 |
-0.087 |
| H5 |
-0.426 |
2.080 |
-0.122 |
| H6 |
0.180 |
1.063 |
-1.455 |
| H7 |
1.961 |
1.742 |
0.223 |
| H8 |
1.081 |
0.828 |
1.467 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5115 | 1.9598 | 2.7557 | 1.0883 | 1.0863 | 2.1350 | 2.1568 |
C2 | 1.5115 | | 2.8928 | 1.7942 | 2.1410 | 2.1671 | 1.0903 | 1.0874 | Br3 | 1.9598 | 2.8928 | | 3.5305 | 2.4901 | 2.4959 | 3.8580 | 3.0131 | Cl4 | 2.7557 | 1.7942 | 3.5305 | | 3.7117 | 2.9156 | 2.3543 | 2.3603 | H5 | 1.0883 | 2.1410 | 2.4901 | 3.7117 | | 1.7820 | 2.4358 | 2.5230 | H6 | 1.0863 | 2.1671 | 2.4959 | 2.9156 | 1.7820 | | 2.5398 | 3.0671 | H7 | 2.1350 | 1.0903 | 3.8580 | 2.3543 | 2.4358 | 2.5398 | | 1.7771 | H8 | 2.1568 | 1.0874 | 3.0131 | 2.3603 | 2.5230 | 3.0671 | 1.7771 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.670 |
|
C1 |
C2 |
H7 |
109.219 |
| C1 |
C2 |
H8 |
111.127 |
|
C2 |
C1 |
Br3 |
112.246 |
| C2 |
C1 |
Cl4 |
36.925 |
|
C2 |
C1 |
H6 |
112.030 |
| Br3 |
C1 |
H5 |
105.992 |
|
Br3 |
C1 |
H6 |
106.488 |
| Cl4 |
C2 |
H7 |
106.869 |
|
Cl4 |
C2 |
H8 |
107.441 |
| H5 |
C1 |
H6 |
110.062 |
|
H7 |
C2 |
H8 |
109.383 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.209 |
|
|
|
| 2 |
C |
-0.283 |
|
|
|
| 3 |
Br |
-0.124 |
|
|
|
| 4 |
Cl |
-0.060 |
|
|
|
| 5 |
H |
0.162 |
|
|
|
| 6 |
H |
0.173 |
|
|
|
| 7 |
H |
0.164 |
|
|
|
| 8 |
H |
0.176 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.334 |
2.758 |
0.118 |
2.781 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.536 |
2.860 |
0.451 |
| y |
2.860 |
-40.388 |
-0.118 |
| z |
0.451 |
-0.118 |
-43.046 |
|
| Traceless |
| | x | y | z |
| x |
-5.819 |
2.860 |
0.451 |
| y |
2.860 |
4.902 |
-0.118 |
| z |
0.451 |
-0.118 |
0.917 |
|
| Polar |
| 3z2-r2 | 1.833 |
| x2-y2 | -7.147 |
| xy | 2.860 |
| xz | 0.451 |
| yz | -0.118 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.983 |
0.211 |
-0.314 |
| y |
0.211 |
7.156 |
0.082 |
| z |
-0.314 |
0.082 |
5.284 |
<r2> (average value of r
2) Å
2
| <r2> |
221.100 |
| (<r2>)1/2 |
14.869 |