Jump to
S1C2
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -3112.998536 |
| Energy at 298.15K | |
| HF Energy | -3112.998536 |
| Nuclear repulsion energy | 288.454797 |
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 wB97X-D/6-311G*
| 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' |
3130 |
3130 |
13.85 |
14.74 |
0.08 |
0.14 |
| 2 |
A' |
3122 |
3122 |
2.02 |
143.87 |
0.08 |
0.14 |
| 3 |
A' |
1509 |
1509 |
0.21 |
15.28 |
0.72 |
0.84 |
| 4 |
A' |
1506 |
1506 |
8.67 |
0.39 |
0.70 |
0.82 |
| 5 |
A' |
1360 |
1360 |
2.50 |
13.62 |
0.64 |
0.78 |
| 6 |
A' |
1268 |
1268 |
47.97 |
2.46 |
0.52 |
0.69 |
| 7 |
A' |
1079 |
1079 |
1.15 |
8.60 |
0.74 |
0.85 |
| 8 |
A' |
766 |
766 |
27.65 |
47.60 |
0.29 |
0.45 |
| 9 |
A' |
669 |
669 |
59.14 |
11.67 |
0.24 |
0.39 |
| 10 |
A' |
254 |
254 |
0.85 |
4.33 |
0.39 |
0.56 |
| 11 |
A' |
200 |
200 |
7.40 |
0.15 |
0.30 |
0.47 |
| 12 |
A" |
3206 |
3206 |
4.26 |
2.72 |
0.75 |
0.86 |
| 13 |
A" |
3183 |
3183 |
0.49 |
97.84 |
0.75 |
0.86 |
| 14 |
A" |
1321 |
1321 |
0.22 |
6.52 |
0.75 |
0.86 |
| 15 |
A" |
1166 |
1166 |
4.55 |
0.06 |
0.75 |
0.86 |
| 16 |
A" |
1000 |
1000 |
0.17 |
6.22 |
0.75 |
0.86 |
| 17 |
A" |
778 |
778 |
5.30 |
0.03 |
0.75 |
0.86 |
| 18 |
A" |
115 |
115 |
5.94 |
0.02 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12814.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12814.8 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 wB97X-D/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.639 |
0.000 |
| C2 |
1.234 |
-0.235 |
0.000 |
| Br3 |
-1.594 |
-0.486 |
0.000 |
| Cl4 |
2.702 |
0.810 |
0.000 |
| H5 |
-0.052 |
1.262 |
0.889 |
| H6 |
-0.052 |
1.262 |
-0.889 |
| H7 |
1.285 |
-0.859 |
0.889 |
| H8 |
1.285 |
-0.859 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5120 | 1.9510 | 2.7073 | 1.0876 | 1.0876 | 2.1647 | 2.1647 |
C2 | 1.5120 | | 2.8399 | 1.8014 | 2.1648 | 2.1648 | 1.0879 | 1.0879 | Br3 | 1.9510 | 2.8399 | | 4.4875 | 2.4953 | 2.4953 | 3.0366 | 3.0366 | Cl4 | 2.7073 | 1.8014 | 4.4875 | | 2.9291 | 2.9291 | 2.3634 | 2.3634 | H5 | 1.0876 | 2.1648 | 2.4953 | 2.9291 | | 1.7788 | 2.5079 | 3.0746 | H6 | 1.0876 | 2.1648 | 2.4953 | 2.9291 | 1.7788 | | 3.0746 | 2.5079 | H7 | 2.1647 | 1.0879 | 3.0366 | 2.3634 | 2.5079 | 3.0746 | | 1.7784 | H8 | 2.1647 | 1.0879 | 3.0366 | 2.3634 | 3.0746 | 2.5079 | 1.7784 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
109.277 |
|
C1 |
C2 |
H7 |
111.697 |
| C1 |
C2 |
H8 |
111.697 |
|
C2 |
C1 |
Br3 |
109.528 |
| C2 |
C1 |
Cl4 |
38.909 |
|
C2 |
C1 |
H6 |
111.730 |
| Br3 |
C1 |
H5 |
106.948 |
|
Br3 |
C1 |
H6 |
106.948 |
| Cl4 |
C2 |
H7 |
107.167 |
|
Cl4 |
C2 |
H8 |
107.167 |
| H5 |
C1 |
H6 |
109.729 |
|
H7 |
C2 |
H8 |
109.632 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.521 |
|
|
|
| 2 |
C |
-0.497 |
|
|
|
| 3 |
Br |
-0.037 |
|
|
|
| 4 |
Cl |
-0.080 |
|
|
|
| 5 |
H |
0.284 |
|
|
|
| 6 |
H |
0.284 |
|
|
|
| 7 |
H |
0.283 |
|
|
|
| 8 |
H |
0.283 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.242 |
-0.091 |
0.000 |
0.258 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.033 |
-2.306 |
0.000 |
| y |
-2.306 |
-43.622 |
0.000 |
| z |
0.000 |
0.000 |
-43.787 |
|
| Traceless |
| | x | y | z |
| x |
-7.328 |
-2.306 |
0.000 |
| y |
-2.306 |
3.788 |
0.000 |
| z |
0.000 |
0.000 |
3.540 |
|
| Polar |
| 3z2-r2 | 7.081 |
| x2-y2 | -7.411 |
| xy | -2.306 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.360 |
2.180 |
0.000 |
| y |
2.180 |
6.388 |
0.000 |
| z |
0.000 |
0.000 |
4.861 |
<r2> (average value of r
2) Å
2
| <r2> |
284.373 |
| (<r2>)1/2 |
16.863 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -3112.995860 |
| Energy at 298.15K | |
| HF Energy | -3112.995860 |
| Nuclear repulsion energy | 303.875091 |
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 wB97X-D/6-311G*
| 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 |
3183 |
3183 |
4.02 |
36.98 |
0.75 |
0.86 |
| 2 |
A |
3167 |
3167 |
2.16 |
94.26 |
0.75 |
0.86 |
| 3 |
A |
3114 |
3114 |
18.05 |
165.08 |
0.04 |
0.07 |
| 4 |
A |
3100 |
3100 |
10.22 |
84.54 |
0.26 |
0.41 |
| 5 |
A |
1493 |
1493 |
2.87 |
6.41 |
0.69 |
0.82 |
| 6 |
A |
1486 |
1486 |
12.36 |
12.74 |
0.73 |
0.84 |
| 7 |
A |
1369 |
1369 |
26.28 |
3.56 |
0.75 |
0.86 |
| 8 |
A |
1329 |
1329 |
48.85 |
1.60 |
0.55 |
0.71 |
| 9 |
A |
1248 |
1248 |
4.16 |
13.65 |
0.74 |
0.85 |
| 10 |
A |
1177 |
1177 |
3.29 |
5.67 |
0.74 |
0.85 |
| 11 |
A |
1061 |
1061 |
1.38 |
2.40 |
0.73 |
0.84 |
| 12 |
A |
953 |
953 |
10.94 |
6.76 |
0.42 |
0.59 |
| 13 |
A |
890 |
890 |
25.86 |
2.05 |
0.74 |
0.85 |
| 14 |
A |
693 |
693 |
22.53 |
9.67 |
0.45 |
0.62 |
| 15 |
A |
596 |
596 |
11.82 |
15.62 |
0.20 |
0.33 |
| 16 |
A |
394 |
394 |
7.00 |
2.55 |
0.71 |
0.83 |
| 17 |
A |
248 |
248 |
1.17 |
1.46 |
0.53 |
0.69 |
| 18 |
A |
101 |
101 |
0.62 |
1.91 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12799.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12799.9 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 wB97X-D/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.007 |
1.093 |
-0.383 |
| C2 |
1.283 |
0.898 |
0.402 |
| Br3 |
-1.363 |
-0.225 |
0.036 |
| Cl4 |
2.186 |
-0.573 |
-0.086 |
| H5 |
-0.421 |
2.065 |
-0.139 |
| H6 |
0.183 |
1.036 |
-1.455 |
| H7 |
1.946 |
1.745 |
0.219 |
| H8 |
1.090 |
0.819 |
1.470 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5106 | 1.9469 | 2.7592 | 1.0898 | 1.0881 | 2.1320 | 2.1638 |
C2 | 1.5106 | | 2.8979 | 1.7937 | 2.1350 | 2.1626 | 1.0910 | 1.0885 | Br3 | 1.9469 | 2.8979 | | 3.5685 | 2.4828 | 2.4905 | 3.8554 | 3.0277 | Cl4 | 2.7592 | 1.7937 | 3.5685 | | 3.7095 | 2.9113 | 2.3503 | 2.3580 | H5 | 1.0898 | 2.1350 | 2.4828 | 3.7095 | | 1.7769 | 2.4149 | 2.5349 | H6 | 1.0881 | 2.1626 | 2.4905 | 2.9113 | 1.7769 | | 2.5322 | 3.0703 | H7 | 2.1320 | 1.0910 | 3.8554 | 2.3503 | 2.4149 | 2.5322 | | 1.7764 | H8 | 2.1638 | 1.0885 | 3.0277 | 2.3580 | 2.5349 | 3.0703 | 1.7764 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.960 |
|
C1 |
C2 |
H7 |
109.008 |
| C1 |
C2 |
H8 |
111.690 |
|
C2 |
C1 |
Br3 |
113.288 |
| C2 |
C1 |
Cl4 |
36.769 |
|
C2 |
C1 |
H6 |
111.618 |
| Br3 |
C1 |
H5 |
106.229 |
|
Br3 |
C1 |
H6 |
106.851 |
| Cl4 |
C2 |
H7 |
106.568 |
|
Cl4 |
C2 |
H8 |
107.249 |
| H5 |
C1 |
H6 |
109.343 |
|
H7 |
C2 |
H8 |
109.186 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.523 |
|
|
|
| 2 |
C |
-0.493 |
|
|
|
| 3 |
Br |
-0.026 |
|
|
|
| 4 |
Cl |
-0.068 |
|
|
|
| 5 |
H |
0.271 |
|
|
|
| 6 |
H |
0.284 |
|
|
|
| 7 |
H |
0.272 |
|
|
|
| 8 |
H |
0.283 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.231 |
2.833 |
0.122 |
2.845 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.298 |
2.983 |
0.400 |
| y |
2.983 |
-40.703 |
-0.102 |
| z |
0.400 |
-0.102 |
-43.420 |
|
| Traceless |
| | x | y | z |
| x |
-6.236 |
2.983 |
0.400 |
| y |
2.983 |
5.156 |
-0.102 |
| z |
0.400 |
-0.102 |
1.080 |
|
| Polar |
| 3z2-r2 | 2.160 |
| x2-y2 | -7.595 |
| xy | 2.983 |
| xz | 0.400 |
| yz | -0.102 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.244 |
0.247 |
-0.329 |
| y |
0.247 |
7.303 |
0.076 |
| z |
-0.329 |
0.076 |
5.199 |
<r2> (average value of r
2) Å
2
| <r2> |
223.707 |
| (<r2>)1/2 |
14.957 |