Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -5226.238804 |
| Energy at 298.15K | |
| HF Energy | -5225.927687 |
| Nuclear repulsion energy | 417.973061 |
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-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 |
Ag |
3130 |
3002 |
0.00 |
157.89 |
0.03 |
0.05 |
| 2 |
Ag |
1503 |
1441 |
0.00 |
6.12 |
0.71 |
0.83 |
| 3 |
Ag |
1293 |
1240 |
0.00 |
49.58 |
0.28 |
0.44 |
| 4 |
Ag |
1080 |
1035 |
0.00 |
8.39 |
0.73 |
0.84 |
| 5 |
Ag |
679 |
651 |
0.00 |
98.78 |
0.24 |
0.39 |
| 6 |
Ag |
191 |
184 |
0.00 |
4.89 |
0.20 |
0.34 |
| 7 |
Au |
3208 |
3077 |
0.00 |
0.00 |
0.54 |
0.70 |
| 8 |
Au |
1113 |
1067 |
2.39 |
0.00 |
0.46 |
0.63 |
| 9 |
Au |
763 |
732 |
3.22 |
0.00 |
0.55 |
0.71 |
| 10 |
Au |
102 |
98 |
4.32 |
0.00 |
0.51 |
0.68 |
| 11 |
Bg |
3186 |
3055 |
0.00 |
67.68 |
0.75 |
0.86 |
| 12 |
Bg |
1301 |
1248 |
0.00 |
1.78 |
0.75 |
0.86 |
| 13 |
Bg |
956 |
917 |
0.00 |
0.83 |
0.75 |
0.86 |
| 14 |
Bu |
3139 |
3010 |
5.25 |
0.00 |
0.16 |
0.27 |
| 15 |
Bu |
1498 |
1436 |
7.23 |
0.00 |
0.65 |
0.79 |
| 16 |
Bu |
1221 |
1171 |
52.94 |
0.00 |
0.73 |
0.85 |
| 17 |
Bu |
607 |
582 |
67.73 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
180 |
172 |
6.28 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12573.7 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 12059.5 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-pVTZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.492 |
0.567 |
0.000 |
| C2 |
-0.492 |
-0.567 |
0.000 |
| Br3 |
-0.492 |
2.261 |
0.000 |
| Br4 |
0.492 |
-2.261 |
0.000 |
| H5 |
1.111 |
0.573 |
0.888 |
| H6 |
1.111 |
0.573 |
-0.888 |
| H7 |
-1.111 |
-0.573 |
0.888 |
| H8 |
-1.111 |
-0.573 |
-0.888 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5021 | 1.9585 | 2.8283 | 1.0824 | 1.0824 | 2.1583 | 2.1583 |
C2 | 1.5021 | | 2.8283 | 1.9585 | 2.1583 | 2.1583 | 1.0824 | 1.0824 | Br3 | 1.9585 | 2.8283 | | 4.6275 | 2.4914 | 2.4914 | 3.0335 | 3.0335 | Br4 | 2.8283 | 1.9585 | 4.6275 | | 3.0335 | 3.0335 | 2.4914 | 2.4914 | H5 | 1.0824 | 2.1583 | 2.4914 | 3.0335 | | 1.7758 | 2.5000 | 3.0665 | H6 | 1.0824 | 2.1583 | 2.4914 | 3.0335 | 1.7758 | | 3.0665 | 2.5000 | H7 | 2.1583 | 1.0824 | 3.0335 | 2.4914 | 2.5000 | 3.0665 | | 1.7758 | H8 | 2.1583 | 1.0824 | 3.0335 | 2.4914 | 3.0665 | 2.5000 | 1.7758 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.917 |
|
C1 |
C2 |
H7 |
112.237 |
| C1 |
C2 |
H8 |
112.237 |
|
C2 |
C1 |
Br3 |
108.917 |
| C2 |
C1 |
H5 |
112.237 |
|
C2 |
C1 |
H6 |
112.237 |
| Br3 |
C1 |
H5 |
106.436 |
|
Br3 |
C1 |
H6 |
106.436 |
| Br4 |
C2 |
H7 |
106.436 |
|
Br4 |
C2 |
H8 |
106.436 |
| H5 |
C1 |
H6 |
110.232 |
|
H7 |
C2 |
H8 |
110.232 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.415 |
|
|
|
| 2 |
C |
-0.415 |
|
|
|
| 3 |
Br |
-0.091 |
|
|
|
| 4 |
Br |
-0.091 |
|
|
|
| 5 |
H |
0.253 |
|
|
|
| 6 |
H |
0.253 |
|
|
|
| 7 |
H |
0.253 |
|
|
|
| 8 |
H |
0.253 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.453 |
1.382 |
0.000 |
| y |
1.382 |
-56.407 |
0.000 |
| z |
0.000 |
0.000 |
-49.989 |
|
| Traceless |
| | x | y | z |
| x |
3.745 |
1.382 |
0.000 |
| y |
1.382 |
-6.686 |
0.000 |
| z |
0.000 |
0.000 |
2.941 |
|
| Polar |
| 3z2-r2 | 5.881 |
| x2-y2 | 6.954 |
| xy | 1.382 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.301 |
-1.635 |
0.000 |
| y |
-1.635 |
14.720 |
0.000 |
| z |
0.000 |
0.000 |
8.425 |
<r2> (average value of r
2) Å
2
| <r2> |
423.362 |
| (<r2>)1/2 |
20.576 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -5226.235392 |
| Energy at 298.15K | |
| HF Energy | -5225.923774 |
| Nuclear repulsion energy | 452.009954 |
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-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 |
3167 |
3038 |
0.00 |
79.10 |
0.75 |
0.86 |
| 2 |
A |
3112 |
2985 |
14.10 |
251.17 |
0.02 |
0.04 |
| 3 |
A |
1482 |
1422 |
0.55 |
3.10 |
0.71 |
0.83 |
| 4 |
A |
1318 |
1264 |
17.79 |
5.10 |
0.10 |
0.18 |
| 5 |
A |
1205 |
1155 |
1.21 |
4.83 |
0.74 |
0.85 |
| 6 |
A |
1048 |
1005 |
1.06 |
1.04 |
0.65 |
0.79 |
| 7 |
A |
918 |
881 |
6.59 |
4.26 |
0.18 |
0.31 |
| 8 |
A |
567 |
544 |
7.14 |
23.59 |
0.05 |
0.09 |
| 9 |
A |
228 |
218 |
1.16 |
1.37 |
0.19 |
0.32 |
| 10 |
A |
78 |
75 |
0.23 |
0.75 |
0.60 |
0.75 |
| 11 |
B |
3180 |
3050 |
0.46 |
24.59 |
0.75 |
0.86 |
| 12 |
B |
3104 |
2977 |
2.21 |
37.45 |
0.75 |
0.86 |
| 13 |
B |
1479 |
1419 |
11.91 |
8.16 |
0.75 |
0.86 |
| 14 |
B |
1291 |
1238 |
64.15 |
4.06 |
0.75 |
0.86 |
| 15 |
B |
1135 |
1088 |
1.44 |
1.05 |
0.75 |
0.86 |
| 16 |
B |
859 |
823 |
16.66 |
1.03 |
0.75 |
0.86 |
| 17 |
B |
601 |
577 |
14.57 |
7.98 |
0.75 |
0.86 |
| 18 |
B |
358 |
343 |
5.74 |
1.70 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12564.7 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 12050.8 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-pVTZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.311 |
0.684 |
1.178 |
| C2 |
-0.311 |
-0.684 |
1.178 |
| Br3 |
-0.311 |
1.800 |
-0.293 |
| Br4 |
0.311 |
-1.800 |
-0.293 |
| H5 |
0.033 |
1.212 |
2.085 |
| H6 |
1.390 |
0.641 |
1.095 |
| H7 |
-0.033 |
-1.212 |
2.085 |
| H8 |
-1.390 |
-0.641 |
1.095 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5037 | 1.9483 | 2.8873 | 1.0857 | 1.0831 | 2.1301 | 2.1583 |
C2 | 1.5037 | | 2.8873 | 1.9483 | 2.1301 | 2.1583 | 1.0857 | 1.0831 | Br3 | 1.9483 | 2.8873 | | 3.6539 | 2.4736 | 2.4829 | 3.8478 | 3.0078 | Br4 | 2.8873 | 1.9483 | 3.6539 | | 3.8478 | 3.0078 | 2.4736 | 2.4829 | H5 | 1.0857 | 2.1301 | 2.4736 | 3.8478 | | 1.7749 | 2.4249 | 2.5375 | H6 | 1.0831 | 2.1583 | 2.4829 | 3.0078 | 1.7749 | | 2.5375 | 3.0617 | H7 | 2.1301 | 1.0857 | 3.8478 | 2.4736 | 2.4249 | 2.5375 | | 1.7749 | H8 | 2.1583 | 1.0831 | 3.0078 | 2.4829 | 2.5375 | 3.0617 | 1.7749 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
112.891 |
|
C1 |
C2 |
H7 |
109.641 |
| C1 |
C2 |
H8 |
112.074 |
|
C2 |
C1 |
Br3 |
112.891 |
| C2 |
C1 |
H5 |
109.641 |
|
C2 |
C1 |
H6 |
112.074 |
| Br3 |
C1 |
H5 |
105.689 |
|
Br3 |
C1 |
H6 |
106.456 |
| Br4 |
C2 |
H7 |
105.689 |
|
Br4 |
C2 |
H8 |
106.456 |
| H5 |
C1 |
H6 |
109.848 |
|
H7 |
C2 |
H8 |
109.848 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.421 |
|
|
|
| 2 |
C |
-0.421 |
|
|
|
| 3 |
Br |
-0.058 |
|
|
|
| 4 |
Br |
-0.058 |
|
|
|
| 5 |
H |
0.223 |
|
|
|
| 6 |
H |
0.256 |
|
|
|
| 7 |
H |
0.223 |
|
|
|
| 8 |
H |
0.256 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.575 |
2.575 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.808 |
0.970 |
0.000 |
| y |
0.970 |
-54.534 |
0.000 |
| z |
0.000 |
0.000 |
-45.612 |
|
| Traceless |
| | x | y | z |
| x |
0.265 |
0.970 |
0.000 |
| y |
0.970 |
-6.824 |
0.000 |
| z |
0.000 |
0.000 |
6.559 |
|
| Polar |
| 3z2-r2 | 13.118 |
| x2-y2 | 4.726 |
| xy | 0.970 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.702 |
-0.669 |
0.000 |
| y |
-0.669 |
11.940 |
0.000 |
| z |
0.000 |
0.000 |
10.205 |
<r2> (average value of r
2) Å
2
| <r2> |
313.014 |
| (<r2>)1/2 |
17.692 |