Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/cc-pVTZ
| | hartrees |
| Energy at 0K | -3112.505353 |
| Energy at 298.15K | |
| HF Energy | -3112.223525 |
| Nuclear repulsion energy | 288.699059 |
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/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' |
3137 |
2997 |
8.07 |
23.98 |
0.05 |
0.09 |
| 2 |
A' |
3125 |
2986 |
1.96 |
143.92 |
0.05 |
0.09 |
| 3 |
A' |
1507 |
1440 |
3.93 |
4.54 |
0.75 |
0.86 |
| 4 |
A' |
1501 |
1434 |
3.25 |
5.87 |
0.75 |
0.85 |
| 5 |
A' |
1325 |
1266 |
1.38 |
14.89 |
0.55 |
0.71 |
| 6 |
A' |
1238 |
1183 |
41.34 |
2.62 |
0.38 |
0.55 |
| 7 |
A' |
1078 |
1030 |
1.03 |
6.62 |
0.75 |
0.85 |
| 8 |
A' |
745 |
711 |
25.04 |
48.79 |
0.28 |
0.43 |
| 9 |
A' |
649 |
620 |
56.66 |
12.71 |
0.24 |
0.38 |
| 10 |
A' |
249 |
238 |
0.84 |
4.74 |
0.30 |
0.46 |
| 11 |
A' |
194 |
186 |
6.72 |
0.19 |
0.32 |
0.49 |
| 12 |
A" |
3204 |
3061 |
0.92 |
5.73 |
0.75 |
0.86 |
| 13 |
A" |
3178 |
3036 |
0.37 |
78.71 |
0.75 |
0.86 |
| 14 |
A" |
1305 |
1247 |
0.01 |
2.99 |
0.75 |
0.86 |
| 15 |
A" |
1136 |
1085 |
2.08 |
0.06 |
0.75 |
0.86 |
| 16 |
A" |
983 |
940 |
0.25 |
3.42 |
0.75 |
0.86 |
| 17 |
A" |
774 |
740 |
3.07 |
0.02 |
0.75 |
0.86 |
| 18 |
A" |
113 |
108 |
5.52 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12721.4 cm
-1
Scaled (by 0.9554) Zero Point Vibrational Energy (zpe) 12154.1 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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.643 |
0.000 |
| C2 |
1.232 |
-0.223 |
0.000 |
| Br3 |
-1.588 |
-0.501 |
0.000 |
| Cl4 |
2.691 |
0.834 |
0.000 |
| H5 |
-0.062 |
1.259 |
0.888 |
| H6 |
-0.062 |
1.259 |
-0.888 |
| H7 |
1.286 |
-0.844 |
0.886 |
| H8 |
1.286 |
-0.844 |
-0.886 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5059 | 1.9571 | 2.6980 | 1.0822 | 1.0822 | 2.1561 | 2.1561 |
C2 | 1.5059 | | 2.8336 | 1.8022 | 2.1583 | 2.1583 | 1.0829 | 1.0829 | Br3 | 1.9571 | 2.8336 | | 4.4827 | 2.4930 | 2.4930 | 3.0269 | 3.0269 | Cl4 | 2.6980 | 1.8022 | 4.4827 | | 2.9235 | 2.9235 | 2.3611 | 2.3611 | H5 | 1.0822 | 2.1583 | 2.4930 | 2.9235 | | 1.7750 | 2.4976 | 3.0631 | H6 | 1.0822 | 2.1583 | 2.4930 | 2.9235 | 1.7750 | | 3.0631 | 2.4976 | H7 | 2.1561 | 1.0829 | 3.0269 | 2.3611 | 2.4976 | 3.0631 | | 1.7716 | H8 | 2.1561 | 1.0829 | 3.0269 | 2.3611 | 3.0631 | 2.4976 | 1.7716 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.960 |
|
C1 |
C2 |
H7 |
111.744 |
| C1 |
C2 |
H8 |
111.744 |
|
C2 |
C1 |
Br3 |
109.122 |
| C2 |
C1 |
Cl4 |
39.177 |
|
C2 |
C1 |
H6 |
111.970 |
| Br3 |
C1 |
H5 |
106.647 |
|
Br3 |
C1 |
H6 |
106.647 |
| Cl4 |
C2 |
H7 |
107.206 |
|
Cl4 |
C2 |
H8 |
107.206 |
| H5 |
C1 |
H6 |
110.196 |
|
H7 |
C2 |
H8 |
109.769 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.174 |
|
|
|
| 2 |
C |
-0.131 |
|
|
|
| 3 |
Br |
-0.124 |
|
|
|
| 4 |
Cl |
-0.165 |
|
|
|
| 5 |
H |
0.148 |
|
|
|
| 6 |
H |
0.148 |
|
|
|
| 7 |
H |
0.149 |
|
|
|
| 8 |
H |
0.149 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.048 |
-0.018 |
0.000 |
0.052 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.368 |
-2.250 |
-0.011 |
| y |
-2.250 |
-43.706 |
-0.004 |
| z |
-0.011 |
-0.004 |
-43.767 |
|
| Traceless |
| | x | y | z |
| x |
-6.631 |
-2.250 |
-0.011 |
| y |
-2.250 |
3.361 |
-0.004 |
| z |
-0.011 |
-0.004 |
3.270 |
|
| Polar |
| 3z2-r2 | 6.540 |
| x2-y2 | -6.662 |
| xy | -2.250 |
| xz | -0.011 |
| yz | -0.004 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
11.254 |
2.009 |
-0.000 |
| y |
2.009 |
7.315 |
-0.000 |
| z |
-0.000 |
-0.000 |
5.907 |
<r2> (average value of r
2) Å
2
| <r2> |
283.644 |
| (<r2>)1/2 |
16.842 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/cc-pVTZ
| | hartrees |
| Energy at 0K | -3112.502407 |
| Energy at 298.15K | |
| HF Energy | -3112.220272 |
| Nuclear repulsion energy | 304.748234 |
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/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 |
3180 |
3038 |
1.65 |
34.12 |
0.75 |
0.86 |
| 2 |
A |
3159 |
3018 |
1.14 |
79.41 |
0.75 |
0.86 |
| 3 |
A |
3115 |
2976 |
13.11 |
170.86 |
0.03 |
0.06 |
| 4 |
A |
3098 |
2960 |
8.55 |
104.07 |
0.20 |
0.33 |
| 5 |
A |
1488 |
1422 |
4.58 |
6.31 |
0.75 |
0.86 |
| 6 |
A |
1479 |
1413 |
7.41 |
7.51 |
0.73 |
0.85 |
| 7 |
A |
1342 |
1283 |
19.53 |
1.48 |
0.74 |
0.85 |
| 8 |
A |
1305 |
1247 |
48.38 |
2.77 |
0.48 |
0.65 |
| 9 |
A |
1220 |
1166 |
2.28 |
7.91 |
0.72 |
0.83 |
| 10 |
A |
1155 |
1104 |
1.20 |
3.21 |
0.72 |
0.84 |
| 11 |
A |
1052 |
1005 |
1.87 |
1.64 |
0.75 |
0.86 |
| 12 |
A |
944 |
902 |
8.32 |
4.54 |
0.38 |
0.55 |
| 13 |
A |
880 |
840 |
18.59 |
1.48 |
0.74 |
0.85 |
| 14 |
A |
681 |
651 |
19.74 |
9.10 |
0.37 |
0.54 |
| 15 |
A |
583 |
557 |
10.84 |
16.02 |
0.16 |
0.27 |
| 16 |
A |
387 |
370 |
6.97 |
2.16 |
0.71 |
0.83 |
| 17 |
A |
244 |
233 |
1.17 |
1.36 |
0.45 |
0.62 |
| 18 |
A |
99 |
95 |
0.53 |
1.47 |
0.71 |
0.83 |
Unscaled Zero Point Vibrational Energy (zpe) 12705.8 cm
-1
Scaled (by 0.9554) Zero Point Vibrational Energy (zpe) 12139.1 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/cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.013 |
1.100 |
-0.385 |
| C2 |
1.280 |
0.900 |
0.404 |
| Br3 |
-1.356 |
-0.225 |
0.036 |
| Cl4 |
2.171 |
-0.576 |
-0.086 |
| H5 |
-0.422 |
2.064 |
-0.142 |
| H6 |
0.189 |
1.032 |
-1.451 |
| H7 |
1.948 |
1.738 |
0.225 |
| H8 |
1.082 |
0.818 |
1.466 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5059 | 1.9506 | 2.7485 | 1.0850 | 1.0829 | 2.1271 | 2.1556 |
C2 | 1.5059 | | 2.8896 | 1.7923 | 2.1330 | 2.1561 | 1.0865 | 1.0836 | Br3 | 1.9506 | 2.8896 | | 3.5464 | 2.4779 | 2.4856 | 3.8478 | 3.0121 | Cl4 | 2.7485 | 1.7923 | 3.5464 | | 3.7006 | 2.8944 | 2.3452 | 2.3531 | H5 | 1.0850 | 2.1330 | 2.4779 | 3.7006 | | 1.7749 | 2.4207 | 2.5298 | H6 | 1.0829 | 2.1561 | 2.4856 | 2.8944 | 1.7749 | | 2.5299 | 3.0580 | H7 | 2.1271 | 1.0865 | 3.8478 | 2.3452 | 2.4207 | 2.5299 | | 1.7717 | H8 | 2.1556 | 1.0836 | 3.0121 | 2.3531 | 2.5298 | 3.0580 | 1.7717 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.598 |
|
C1 |
C2 |
H7 |
109.205 |
| C1 |
C2 |
H8 |
111.664 |
|
C2 |
C1 |
Br3 |
112.807 |
| C2 |
C1 |
Cl4 |
37.016 |
|
C2 |
C1 |
H6 |
111.748 |
| Br3 |
C1 |
H5 |
105.880 |
|
Br3 |
C1 |
H6 |
106.515 |
| Cl4 |
C2 |
H7 |
106.516 |
|
Cl4 |
C2 |
H8 |
107.229 |
| H5 |
C1 |
H6 |
109.917 |
|
H7 |
C2 |
H8 |
109.462 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.181 |
|
|
|
| 2 |
C |
-0.138 |
|
|
|
| 3 |
Br |
-0.108 |
|
|
|
| 4 |
Cl |
-0.148 |
|
|
|
| 5 |
H |
0.141 |
|
|
|
| 6 |
H |
0.143 |
|
|
|
| 7 |
H |
0.144 |
|
|
|
| 8 |
H |
0.146 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.374 |
2.640 |
0.102 |
2.668 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.895 |
2.648 |
0.421 |
| y |
2.648 |
-40.867 |
-0.079 |
| z |
0.421 |
-0.079 |
-43.442 |
|
| Traceless |
| | x | y | z |
| x |
-5.740 |
2.648 |
0.421 |
| y |
2.648 |
4.801 |
-0.079 |
| z |
0.421 |
-0.079 |
0.939 |
|
| Polar |
| 3z2-r2 | 1.878 |
| x2-y2 | -7.027 |
| xy | 2.648 |
| xz | 0.421 |
| yz | -0.079 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.278 |
0.289 |
-0.222 |
| y |
0.289 |
8.063 |
0.038 |
| z |
-0.222 |
0.038 |
6.212 |
<r2> (average value of r
2) Å
2
| <r2> |
221.906 |
| (<r2>)1/2 |
14.897 |