Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -3112.318993 |
| Energy at 298.15K | |
| HF Energy | -3112.117442 |
| Nuclear repulsion energy | 286.922829 |
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/aug-cc-pVDZ
| 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' |
3136 |
3018 |
7.35 |
23.35 |
0.04 |
0.07 |
| 2 |
A' |
3126 |
3009 |
1.68 |
146.12 |
0.03 |
0.06 |
| 3 |
A' |
1477 |
1422 |
0.78 |
5.80 |
0.72 |
0.84 |
| 4 |
A' |
1470 |
1414 |
6.17 |
0.76 |
0.72 |
0.84 |
| 5 |
A' |
1305 |
1255 |
1.13 |
22.80 |
0.34 |
0.51 |
| 6 |
A' |
1216 |
1170 |
41.49 |
2.82 |
0.27 |
0.42 |
| 7 |
A' |
1082 |
1042 |
1.08 |
5.70 |
0.71 |
0.83 |
| 8 |
A' |
732 |
705 |
27.47 |
59.53 |
0.25 |
0.39 |
| 9 |
A' |
639 |
614 |
62.17 |
14.41 |
0.22 |
0.37 |
| 10 |
A' |
248 |
239 |
0.80 |
5.72 |
0.22 |
0.37 |
| 11 |
A' |
195 |
188 |
6.97 |
0.26 |
0.21 |
0.34 |
| 12 |
A" |
3218 |
3096 |
0.36 |
4.64 |
0.75 |
0.86 |
| 13 |
A" |
3195 |
3074 |
0.21 |
72.45 |
0.75 |
0.86 |
| 14 |
A" |
1284 |
1236 |
0.02 |
2.35 |
0.75 |
0.86 |
| 15 |
A" |
1118 |
1076 |
1.62 |
0.03 |
0.75 |
0.86 |
| 16 |
A" |
973 |
937 |
0.16 |
1.11 |
0.75 |
0.86 |
| 17 |
A" |
765 |
736 |
2.45 |
0.00 |
0.75 |
0.86 |
| 18 |
A" |
110 |
106 |
5.65 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12644.5 cm
-1
Scaled (by 0.9623) Zero Point Vibrational Energy (zpe) 12167.8 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/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.649 |
0.000 |
| C2 |
1.235 |
-0.225 |
0.000 |
| Br3 |
-1.596 |
-0.506 |
0.000 |
| Cl4 |
2.706 |
0.842 |
0.000 |
| H5 |
-0.064 |
1.268 |
0.898 |
| H6 |
-0.064 |
1.268 |
-0.898 |
| H7 |
1.293 |
-0.848 |
0.897 |
| H8 |
1.293 |
-0.848 |
-0.897 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5135 | 1.9702 | 2.7124 | 1.0926 | 1.0926 | 2.1721 | 2.1721 |
C2 | 1.5135 | | 2.8451 | 1.8171 | 2.1737 | 2.1737 | 1.0932 | 1.0932 | Br3 | 1.9702 | 2.8451 | | 4.5079 | 2.5102 | 2.5102 | 3.0447 | 3.0447 | Cl4 | 2.7124 | 1.8171 | 4.5079 | | 2.9425 | 2.9425 | 2.3779 | 2.3779 | H5 | 1.0926 | 2.1737 | 2.5102 | 2.9425 | | 1.7965 | 2.5137 | 3.0889 | H6 | 1.0926 | 2.1737 | 2.5102 | 2.9425 | 1.7965 | | 3.0889 | 2.5137 | H7 | 2.1721 | 1.0932 | 3.0447 | 2.3779 | 2.5137 | 3.0889 | | 1.7939 | H8 | 2.1721 | 1.0932 | 3.0447 | 2.3779 | 3.0889 | 2.5137 | 1.7939 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
108.716 |
|
C1 |
C2 |
H7 |
111.863 |
| C1 |
C2 |
H8 |
111.863 |
|
C2 |
C1 |
Br3 |
108.799 |
| C2 |
C1 |
Cl4 |
39.381 |
|
C2 |
C1 |
H6 |
112.026 |
| Br3 |
C1 |
H5 |
106.539 |
|
Br3 |
C1 |
H6 |
106.539 |
| Cl4 |
C2 |
H7 |
106.939 |
|
Cl4 |
C2 |
H8 |
106.939 |
| H5 |
C1 |
H6 |
110.590 |
|
H7 |
C2 |
H8 |
110.262 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.176 |
|
|
|
| 2 |
C |
0.262 |
|
|
|
| 3 |
Br |
0.202 |
|
|
|
| 4 |
Cl |
-0.083 |
|
|
|
| 5 |
H |
-0.156 |
|
|
|
| 6 |
H |
-0.156 |
|
|
|
| 7 |
H |
-0.122 |
|
|
|
| 8 |
H |
-0.122 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.086 |
-0.032 |
0.000 |
0.092 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.073 |
-2.389 |
-0.014 |
| y |
-2.389 |
-44.182 |
-0.004 |
| z |
-0.014 |
-0.004 |
-44.259 |
|
| Traceless |
| | x | y | z |
| x |
-6.853 |
-2.389 |
-0.014 |
| y |
-2.389 |
3.484 |
-0.004 |
| z |
-0.014 |
-0.004 |
3.369 |
|
| Polar |
| 3z2-r2 | 6.738 |
| x2-y2 | -6.891 |
| xy | -2.389 |
| xz | -0.014 |
| yz | -0.004 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
12.417 |
1.854 |
-0.001 |
| y |
1.854 |
8.518 |
-0.000 |
| z |
-0.001 |
-0.000 |
7.340 |
<r2> (average value of r
2) Å
2
| <r2> |
286.878 |
| (<r2>)1/2 |
16.937 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -3112.315840 |
| Energy at 298.15K | |
| HF Energy | -3112.114057 |
| Nuclear repulsion energy | 302.844100 |
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/aug-cc-pVDZ
| 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 |
3192 |
3071 |
0.89 |
35.60 |
0.75 |
0.86 |
| 2 |
A |
3174 |
3054 |
0.75 |
74.88 |
0.75 |
0.86 |
| 3 |
A |
3113 |
2996 |
13.01 |
183.19 |
0.03 |
0.06 |
| 4 |
A |
3099 |
2982 |
8.56 |
100.71 |
0.17 |
0.29 |
| 5 |
A |
1457 |
1402 |
2.78 |
4.01 |
0.75 |
0.86 |
| 6 |
A |
1446 |
1392 |
9.81 |
7.26 |
0.73 |
0.85 |
| 7 |
A |
1321 |
1271 |
18.67 |
1.59 |
0.30 |
0.46 |
| 8 |
A |
1283 |
1234 |
50.65 |
4.10 |
0.40 |
0.57 |
| 9 |
A |
1207 |
1161 |
1.61 |
5.27 |
0.68 |
0.81 |
| 10 |
A |
1136 |
1093 |
0.99 |
1.31 |
0.68 |
0.81 |
| 11 |
A |
1053 |
1014 |
2.08 |
1.20 |
0.75 |
0.86 |
| 12 |
A |
932 |
897 |
7.56 |
3.94 |
0.19 |
0.32 |
| 13 |
A |
869 |
836 |
18.57 |
1.30 |
0.72 |
0.84 |
| 14 |
A |
671 |
645 |
21.57 |
10.80 |
0.27 |
0.43 |
| 15 |
A |
574 |
552 |
11.68 |
19.18 |
0.13 |
0.23 |
| 16 |
A |
387 |
372 |
7.59 |
1.87 |
0.69 |
0.82 |
| 17 |
A |
243 |
234 |
1.24 |
1.29 |
0.23 |
0.37 |
| 18 |
A |
95 |
91 |
0.57 |
1.04 |
0.65 |
0.79 |
Unscaled Zero Point Vibrational Energy (zpe) 12624.5 cm
-1
Scaled (by 0.9623) Zero Point Vibrational Energy (zpe) 12148.5 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 B2PLYP=FULLultrafine/aug-cc-pVDZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.014 |
1.105 |
-0.390 |
| C2 |
1.283 |
0.906 |
0.410 |
| Br3 |
-1.364 |
-0.226 |
0.036 |
| Cl4 |
2.186 |
-0.578 |
-0.087 |
| H5 |
-0.426 |
2.078 |
-0.147 |
| H6 |
0.195 |
1.030 |
-1.466 |
| H7 |
1.958 |
1.751 |
0.231 |
| H8 |
1.079 |
0.814 |
1.480 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Cl4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5128 | 1.9628 | 2.7638 | 1.0956 | 1.0934 | 2.1406 | 2.1718 |
C2 | 1.5128 | | 2.9029 | 1.8065 | 2.1454 | 2.1716 | 1.0967 | 1.0940 | Br3 | 1.9628 | 2.9029 | | 3.5692 | 2.4946 | 2.5034 | 3.8711 | 3.0224 | Cl4 | 2.7638 | 1.8065 | 3.5692 | | 3.7253 | 2.9070 | 2.3617 | 2.3707 | H5 | 1.0956 | 2.1454 | 2.4946 | 3.7253 | | 1.7954 | 2.4356 | 2.5510 | H6 | 1.0934 | 2.1716 | 2.5034 | 2.9070 | 1.7954 | | 2.5506 | 3.0835 | H7 | 2.1406 | 1.0967 | 3.8711 | 2.3617 | 2.4356 | 2.5506 | | 1.7927 | H8 | 2.1718 | 1.0940 | 3.0224 | 2.3707 | 2.5510 | 3.0835 | 1.7927 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Cl4 |
112.441 |
|
C1 |
C2 |
H7 |
109.196 |
| C1 |
C2 |
H8 |
111.838 |
|
C2 |
C1 |
Br3 |
112.635 |
| C2 |
C1 |
Cl4 |
37.167 |
|
C2 |
C1 |
H6 |
111.862 |
| Br3 |
C1 |
H5 |
105.790 |
|
Br3 |
C1 |
H6 |
106.496 |
| Cl4 |
C2 |
H7 |
106.291 |
|
Cl4 |
C2 |
H8 |
107.063 |
| H5 |
C1 |
H6 |
110.216 |
|
H7 |
C2 |
H8 |
109.838 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.125 |
|
|
|
| 2 |
C |
0.199 |
|
|
|
| 3 |
Br |
0.226 |
|
|
|
| 4 |
Cl |
-0.058 |
|
|
|
| 5 |
H |
-0.152 |
|
|
|
| 6 |
H |
-0.145 |
|
|
|
| 7 |
H |
-0.103 |
|
|
|
| 8 |
H |
-0.092 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.358 |
2.701 |
0.107 |
2.727 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.686 |
2.756 |
0.489 |
| y |
2.756 |
-41.180 |
-0.091 |
| z |
0.489 |
-0.091 |
-43.887 |
|
| Traceless |
| | x | y | z |
| x |
-6.152 |
2.756 |
0.489 |
| y |
2.756 |
5.106 |
-0.091 |
| z |
0.489 |
-0.091 |
1.046 |
|
| Polar |
| 3z2-r2 | 2.092 |
| x2-y2 | -7.506 |
| xy | 2.756 |
| xz | 0.489 |
| yz | -0.091 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.600 |
0.191 |
-0.189 |
| y |
0.191 |
9.085 |
0.032 |
| z |
-0.189 |
0.032 |
7.549 |
<r2> (average value of r
2) Å
2
| <r2> |
224.602 |
| (<r2>)1/2 |
14.987 |