Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/3-21G
| | hartrees |
| Energy at 0K | -3097.208426 |
| Energy at 298.15K | |
| HF Energy | -3097.115504 |
| Nuclear repulsion energy | 281.584877 |
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/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' |
3182 |
3182 |
4.30 |
7.80 |
0.11 |
0.20 |
| 2 |
A' |
3172 |
3172 |
0.33 |
136.77 |
0.09 |
0.16 |
| 3 |
A' |
1557 |
1557 |
7.83 |
8.37 |
0.75 |
0.86 |
| 4 |
A' |
1554 |
1554 |
6.71 |
14.63 |
0.75 |
0.86 |
| 5 |
A' |
1340 |
1340 |
0.10 |
37.36 |
0.48 |
0.65 |
| 6 |
A' |
1274 |
1274 |
41.86 |
0.12 |
0.28 |
0.44 |
| 7 |
A' |
1059 |
1059 |
1.26 |
24.80 |
0.66 |
0.80 |
| 8 |
A' |
682 |
682 |
5.92 |
86.61 |
0.32 |
0.48 |
| 9 |
A' |
626 |
626 |
80.54 |
0.53 |
0.46 |
0.63 |
| 10 |
A' |
238 |
238 |
1.02 |
8.74 |
0.39 |
0.56 |
| 11 |
A' |
191 |
191 |
8.84 |
0.09 |
0.51 |
0.67 |
| 12 |
A" |
3263 |
3263 |
0.99 |
3.75 |
0.75 |
0.86 |
| 13 |
A" |
3237 |
3237 |
0.04 |
90.63 |
0.75 |
0.86 |
| 14 |
A" |
1350 |
1350 |
0.02 |
11.54 |
0.75 |
0.86 |
| 15 |
A" |
1156 |
1156 |
1.22 |
0.04 |
0.75 |
0.86 |
| 16 |
A" |
967 |
967 |
0.11 |
16.67 |
0.75 |
0.86 |
| 17 |
A" |
791 |
791 |
6.63 |
0.08 |
0.75 |
0.86 |
| 18 |
A" |
109 |
109 |
6.89 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12872.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12872.8 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 B2PLYP=FULLultrafine/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.644 |
0.000 |
| C2 |
1.228 |
-0.236 |
0.000 |
| Br3 |
-1.621 |
-0.540 |
0.000 |
| Cl4 |
2.755 |
0.919 |
0.000 |
| H5 |
-0.061 |
1.257 |
0.894 |
| H6 |
-0.061 |
1.257 |
-0.894 |
| H7 |
1.322 |
-0.837 |
0.899 |
| H8 |
1.322 |
-0.837 |
-0.899 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5110 | 2.0075 | 2.7689 | 1.0856 | 1.0856 | 2.1787 | 2.1787 |
C2 | 1.5110 | | 2.8655 | 1.9140 | 2.1652 | 2.1652 | 1.0850 | 1.0850 | Br3 | 2.0075 | 2.8655 | | 4.6129 | 2.5424 | 2.5424 | 3.0909 | 3.0909 | Cl4 | 2.7689 | 1.9140 | 4.6129 | | 2.9736 | 2.9736 | 2.4379 | 2.4379 | H5 | 1.0856 | 2.1652 | 2.5424 | 2.9736 | | 1.7883 | 2.5086 | 3.0833 | H6 | 1.0856 | 2.1652 | 2.5424 | 2.9736 | 1.7883 | | 3.0833 | 2.5086 | H7 | 2.1787 | 1.0850 | 3.0909 | 2.4379 | 2.5086 | 3.0833 | | 1.7970 | H8 | 2.1787 | 1.0850 | 3.0909 | 2.4379 | 3.0833 | 2.5086 | 1.7970 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
107.300 |
|
C1 |
C2 |
H7 |
113.104 |
| C1 |
C2 |
H8 |
113.104 |
|
C2 |
C1 |
Br3 |
108.233 |
| C2 |
C1 |
Cl4 |
41.300 |
|
C2 |
C1 |
H6 |
111.958 |
| Br3 |
C1 |
H5 |
106.736 |
|
Br3 |
C1 |
H6 |
106.736 |
| Cl4 |
C2 |
H7 |
105.397 |
|
Cl4 |
C2 |
H8 |
105.397 |
| H5 |
C1 |
H6 |
110.904 |
|
H7 |
C2 |
H8 |
111.812 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.583 |
|
|
|
| 2 |
C |
-0.495 |
|
|
|
| 3 |
Br |
0.056 |
|
|
|
| 4 |
Cl |
-0.061 |
|
|
|
| 5 |
H |
0.272 |
|
|
|
| 6 |
H |
0.272 |
|
|
|
| 7 |
H |
0.269 |
|
|
|
| 8 |
H |
0.269 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.760 |
-0.447 |
0.000 |
0.882 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.743 |
-3.532 |
-0.012 |
| y |
-3.532 |
-44.037 |
-0.004 |
| z |
-0.012 |
-0.004 |
-43.700 |
|
| Traceless |
| | x | y | z |
| x |
-8.875 |
-3.532 |
-0.012 |
| y |
-3.532 |
4.185 |
-0.004 |
| z |
-0.012 |
-0.004 |
4.690 |
|
| Polar |
| 3z2-r2 | 9.380 |
| x2-y2 | -8.707 |
| xy | -3.532 |
| xz | -0.012 |
| yz | -0.004 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.523 |
2.930 |
0.000 |
| y |
2.930 |
5.360 |
0.000 |
| z |
0.000 |
0.000 |
3.509 |
<r2> (average value of r
2) Å
2
| <r2> |
297.966 |
| (<r2>)1/2 |
17.262 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/3-21G
| | hartrees |
| Energy at 0K | -3097.204514 |
| Energy at 298.15K | |
| HF Energy | -3097.111444 |
| Nuclear repulsion energy | 298.187560 |
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/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 |
3235 |
3235 |
0.85 |
36.82 |
0.75 |
0.86 |
| 2 |
A |
3215 |
3215 |
0.18 |
87.19 |
0.75 |
0.86 |
| 3 |
A |
3155 |
3155 |
7.45 |
158.81 |
0.05 |
0.10 |
| 4 |
A |
3142 |
3142 |
3.43 |
82.08 |
0.31 |
0.48 |
| 5 |
A |
1540 |
1540 |
11.49 |
18.32 |
0.74 |
0.85 |
| 6 |
A |
1532 |
1532 |
5.96 |
13.20 |
0.73 |
0.84 |
| 7 |
A |
1367 |
1367 |
19.20 |
5.39 |
0.64 |
0.78 |
| 8 |
A |
1342 |
1342 |
48.76 |
1.56 |
0.74 |
0.85 |
| 9 |
A |
1235 |
1235 |
1.53 |
26.90 |
0.75 |
0.86 |
| 10 |
A |
1180 |
1180 |
1.22 |
10.63 |
0.75 |
0.86 |
| 11 |
A |
1045 |
1045 |
3.13 |
4.26 |
0.72 |
0.84 |
| 12 |
A |
934 |
934 |
9.39 |
13.12 |
0.54 |
0.70 |
| 13 |
A |
871 |
871 |
24.34 |
2.84 |
0.62 |
0.77 |
| 14 |
A |
615 |
615 |
25.01 |
18.20 |
0.58 |
0.73 |
| 15 |
A |
570 |
570 |
10.06 |
17.93 |
0.17 |
0.28 |
| 16 |
A |
380 |
380 |
8.36 |
4.56 |
0.75 |
0.86 |
| 17 |
A |
244 |
244 |
1.50 |
1.92 |
0.42 |
0.60 |
| 18 |
A |
94 |
94 |
0.84 |
2.71 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 12848.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12848.4 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/3-21G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
1.130 |
-0.406 |
| C2 |
1.268 |
0.971 |
0.420 |
| Br3 |
-1.376 |
-0.235 |
0.037 |
| Cl4 |
2.216 |
-0.597 |
-0.084 |
| H5 |
-0.447 |
2.096 |
-0.195 |
| H6 |
0.217 |
1.036 |
-1.469 |
| H7 |
1.965 |
1.785 |
0.233 |
| H8 |
1.065 |
0.859 |
1.481 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5119 | 1.9967 | 2.8192 | 1.0897 | 1.0864 | 2.1575 | 2.1783 |
C2 | 1.5119 | | 2.9307 | 1.9012 | 2.1406 | 2.1629 | 1.0884 | 1.0855 | Br3 | 1.9967 | 2.9307 | | 3.6122 | 2.5202 | 2.5343 | 3.9094 | 3.0396 | Cl4 | 2.8192 | 1.9012 | 3.6122 | | 3.7891 | 2.9298 | 2.4166 | 2.4278 | H5 | 1.0897 | 2.1406 | 2.5202 | 3.7891 | | 1.7854 | 2.4694 | 2.5737 | H6 | 1.0864 | 2.1629 | 2.5343 | 2.9298 | 1.7854 | | 2.5527 | 3.0746 | H7 | 2.1575 | 1.0884 | 3.9094 | 2.4166 | 2.4694 | 2.5527 | | 1.7958 | H8 | 2.1783 | 1.0855 | 3.0396 | 2.4278 | 2.5737 | 3.0746 | 1.7958 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
110.869 |
|
C1 |
C2 |
H7 |
111.091 |
| C1 |
C2 |
H8 |
112.970 |
|
C2 |
C1 |
Br3 |
112.564 |
| C2 |
C1 |
Cl4 |
39.059 |
|
C2 |
C1 |
H6 |
111.650 |
| Br3 |
C1 |
H5 |
105.694 |
|
Br3 |
C1 |
H6 |
106.819 |
| Cl4 |
C2 |
H7 |
104.572 |
|
Cl4 |
C2 |
H8 |
105.476 |
| H5 |
C1 |
H6 |
110.254 |
|
H7 |
C2 |
H8 |
111.397 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.594 |
|
|
|
| 2 |
C |
-0.503 |
|
|
|
| 3 |
Br |
0.073 |
|
|
|
| 4 |
Cl |
-0.044 |
|
|
|
| 5 |
H |
0.262 |
|
|
|
| 6 |
H |
0.273 |
|
|
|
| 7 |
H |
0.263 |
|
|
|
| 8 |
H |
0.270 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.172 |
3.106 |
0.215 |
3.118 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.766 |
3.475 |
0.623 |
| y |
3.475 |
-40.984 |
-0.070 |
| z |
0.623 |
-0.070 |
-43.277 |
|
| Traceless |
| | x | y | z |
| x |
-6.636 |
3.475 |
0.623 |
| y |
3.475 |
5.037 |
-0.070 |
| z |
0.623 |
-0.070 |
1.599 |
|
| Polar |
| 3z2-r2 | 3.197 |
| x2-y2 | -7.782 |
| xy | 3.475 |
| xz | 0.623 |
| yz | -0.070 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.957 |
0.283 |
-0.573 |
| y |
0.283 |
6.418 |
0.060 |
| z |
-0.573 |
0.060 |
3.799 |
<r2> (average value of r
2) Å
2
| <r2> |
229.700 |
| (<r2>)1/2 |
15.156 |