Jump to
S1C2
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -5218.214872 |
| Energy at 298.15K | -5218.225240 |
| HF Energy | -5218.214872 |
| Nuclear repulsion energy | 421.176844 |
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 HF/6-31G(2df,p)
| 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 |
3263 |
2954 |
0.00 |
|
|
|
| 2 |
Ag |
1611 |
1458 |
0.00 |
|
|
|
| 3 |
Ag |
1422 |
1288 |
0.00 |
|
|
|
| 4 |
Ag |
1124 |
1018 |
0.00 |
|
|
|
| 5 |
Ag |
744 |
673 |
0.00 |
|
|
|
| 6 |
Ag |
209 |
189 |
0.00 |
|
|
|
| 7 |
Au |
3345 |
3029 |
1.02 |
|
|
|
| 8 |
Au |
1208 |
1094 |
2.23 |
|
|
|
| 9 |
Au |
810 |
733 |
2.72 |
|
|
|
| 10 |
Au |
112 |
101 |
5.28 |
|
|
|
| 11 |
Bg |
3322 |
3008 |
0.00 |
|
|
|
| 12 |
Bg |
1398 |
1266 |
0.00 |
|
|
|
| 13 |
Bg |
1038 |
940 |
0.00 |
|
|
|
| 14 |
Bu |
3269 |
2960 |
13.52 |
|
|
|
| 15 |
Bu |
1604 |
1453 |
7.45 |
|
|
|
| 16 |
Bu |
1329 |
1204 |
72.28 |
|
|
|
| 17 |
Bu |
660 |
597 |
84.78 |
|
|
|
| 18 |
Bu |
201 |
182 |
6.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13333.1 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 12073.1 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 HF/6-31G(2df,p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.488 |
0.578 |
0.000 |
| C2 |
-0.488 |
-0.578 |
0.000 |
| Br3 |
-0.488 |
2.244 |
0.000 |
| Br4 |
0.488 |
-2.244 |
0.000 |
| H5 |
1.109 |
0.573 |
0.881 |
| H6 |
1.109 |
0.573 |
-0.881 |
| H7 |
-1.109 |
-0.573 |
0.881 |
| H8 |
-1.109 |
-0.573 |
-0.881 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5123 | 1.9306 | 2.8219 | 1.0780 | 1.0780 | 2.1566 | 2.1566 |
C2 | 1.5123 | | 2.8219 | 1.9306 | 2.1566 | 2.1566 | 1.0780 | 1.0780 | Br3 | 1.9306 | 2.8219 | | 4.5928 | 2.4731 | 2.4731 | 3.0166 | 3.0166 | Br4 | 2.8219 | 1.9306 | 4.5928 | | 3.0166 | 3.0166 | 2.4731 | 2.4731 | H5 | 1.0780 | 2.1566 | 2.4731 | 3.0166 | | 1.7616 | 2.4972 | 3.0560 | H6 | 1.0780 | 2.1566 | 2.4731 | 3.0166 | 1.7616 | | 3.0560 | 2.4972 | H7 | 2.1566 | 1.0780 | 3.0166 | 2.4731 | 2.4972 | 3.0560 | | 1.7616 | H8 | 2.1566 | 1.0780 | 3.0166 | 2.4731 | 3.0560 | 2.4972 | 1.7616 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.493 |
|
C1 |
C2 |
H7 |
111.634 |
| C1 |
C2 |
H8 |
111.634 |
|
C2 |
C1 |
Br3 |
109.493 |
| C2 |
C1 |
H5 |
111.634 |
|
C2 |
C1 |
H6 |
111.634 |
| Br3 |
C1 |
H5 |
107.145 |
|
Br3 |
C1 |
H6 |
107.145 |
| Br4 |
C2 |
H7 |
107.145 |
|
Br4 |
C2 |
H8 |
107.145 |
| H5 |
C1 |
H6 |
109.590 |
|
H7 |
C2 |
H8 |
109.590 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.353 |
|
|
|
| 2 |
C |
-0.353 |
|
|
|
| 3 |
Br |
-0.050 |
|
|
|
| 4 |
Br |
-0.050 |
|
|
|
| 5 |
H |
0.202 |
|
|
|
| 6 |
H |
0.202 |
|
|
|
| 7 |
H |
0.202 |
|
|
|
| 8 |
H |
0.202 |
|
|
|
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 |
-48.650 |
1.623 |
0.000 |
| y |
1.623 |
-56.504 |
0.000 |
| z |
0.000 |
0.000 |
-49.242 |
|
| Traceless |
| | x | y | z |
| x |
4.223 |
1.623 |
0.000 |
| y |
1.623 |
-7.558 |
0.000 |
| z |
0.000 |
0.000 |
3.334 |
|
| Polar |
| 3z2-r2 | 6.669 |
| x2-y2 | 7.854 |
| xy | 1.623 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.736 |
-1.640 |
0.000 |
| y |
-1.640 |
12.238 |
0.000 |
| z |
0.000 |
0.000 |
6.928 |
<r2> (average value of r
2) Å
2
| <r2> |
417.485 |
| (<r2>)1/2 |
20.432 |
Jump to
S1C1
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -5218.211652 |
| Energy at 298.15K | |
| HF Energy | -5218.211652 |
| Nuclear repulsion energy | 455.634661 |
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 HF/6-31G(2df,p)
| 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 |
3307 |
2994 |
0.21 |
83.76 |
0.75 |
0.86 |
| 2 |
A |
3248 |
2941 |
24.04 |
166.48 |
0.04 |
0.07 |
| 3 |
A |
1597 |
1446 |
0.06 |
5.06 |
0.75 |
0.85 |
| 4 |
A |
1432 |
1297 |
26.15 |
2.22 |
0.19 |
0.32 |
| 5 |
A |
1303 |
1180 |
1.02 |
7.37 |
0.72 |
0.84 |
| 6 |
A |
1104 |
1000 |
0.59 |
2.60 |
0.67 |
0.80 |
| 7 |
A |
992 |
899 |
8.03 |
3.89 |
0.36 |
0.53 |
| 8 |
A |
610 |
553 |
12.52 |
24.19 |
0.07 |
0.13 |
| 9 |
A |
245 |
222 |
1.23 |
1.00 |
0.23 |
0.38 |
| 10 |
A |
87 |
79 |
0.33 |
0.86 |
0.64 |
0.78 |
| 11 |
B |
3320 |
3007 |
2.79 |
21.94 |
0.75 |
0.86 |
| 12 |
B |
3236 |
2930 |
2.93 |
37.51 |
0.75 |
0.86 |
| 13 |
B |
1590 |
1440 |
9.67 |
12.18 |
0.75 |
0.86 |
| 14 |
B |
1401 |
1269 |
72.28 |
2.09 |
0.75 |
0.86 |
| 15 |
B |
1223 |
1107 |
1.37 |
2.41 |
0.75 |
0.86 |
| 16 |
B |
928 |
841 |
14.60 |
0.91 |
0.75 |
0.86 |
| 17 |
B |
649 |
588 |
18.97 |
11.42 |
0.75 |
0.86 |
| 18 |
B |
388 |
351 |
7.38 |
2.14 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13330.3 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 12070.6 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 HF/6-31G(2df,p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.309 |
0.691 |
1.166 |
| C2 |
-0.309 |
-0.691 |
1.166 |
| Br3 |
-0.309 |
1.785 |
-0.290 |
| Br4 |
0.309 |
-1.785 |
-0.290 |
| H5 |
0.031 |
1.206 |
2.075 |
| H6 |
1.384 |
0.644 |
1.096 |
| H7 |
-0.031 |
-1.206 |
2.075 |
| H8 |
-1.384 |
-0.644 |
1.096 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5136 | 1.9237 | 2.8725 | 1.0811 | 1.0784 | 2.1309 | 2.1572 |
C2 | 1.5136 | | 2.8725 | 1.9237 | 2.1309 | 2.1572 | 1.0811 | 1.0784 | Br3 | 1.9237 | 2.8725 | | 3.6233 | 2.4584 | 2.4679 | 3.8235 | 2.9961 | Br4 | 2.8725 | 1.9237 | 3.6233 | | 3.8235 | 2.9961 | 2.4584 | 2.4679 | H5 | 1.0811 | 2.1309 | 2.4584 | 3.8235 | | 1.7623 | 2.4137 | 2.5269 | H6 | 1.0784 | 2.1572 | 2.4679 | 2.9961 | 1.7623 | | 2.5269 | 3.0532 | H7 | 2.1309 | 1.0811 | 3.8235 | 2.4584 | 2.4137 | 2.5269 | | 1.7623 | H8 | 2.1572 | 1.0784 | 2.9961 | 2.4679 | 2.5269 | 3.0532 | 1.7623 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
112.829 |
|
C1 |
C2 |
H7 |
109.289 |
| C1 |
C2 |
H8 |
111.558 |
|
C2 |
C1 |
Br3 |
112.829 |
| C2 |
C1 |
H5 |
109.289 |
|
C2 |
C1 |
H6 |
111.558 |
| Br3 |
C1 |
H5 |
106.402 |
|
Br3 |
C1 |
H6 |
107.201 |
| Br4 |
C2 |
H7 |
106.402 |
|
Br4 |
C2 |
H8 |
107.201 |
| H5 |
C1 |
H6 |
109.386 |
|
H7 |
C2 |
H8 |
109.386 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.349 |
|
|
|
| 2 |
C |
-0.349 |
|
|
|
| 3 |
Br |
-0.046 |
|
|
|
| 4 |
Br |
-0.046 |
|
|
|
| 5 |
H |
0.194 |
|
|
|
| 6 |
H |
0.201 |
|
|
|
| 7 |
H |
0.194 |
|
|
|
| 8 |
H |
0.201 |
|
|
|
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 |
2.786 |
2.786 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.015 |
1.083 |
0.000 |
| y |
1.083 |
-54.148 |
0.000 |
| z |
0.000 |
0.000 |
-44.881 |
|
| Traceless |
| | x | y | z |
| x |
0.500 |
1.083 |
0.000 |
| y |
1.083 |
-7.200 |
0.000 |
| z |
0.000 |
0.000 |
6.700 |
|
| Polar |
| 3z2-r2 | 13.400 |
| x2-y2 | 5.133 |
| xy | 1.083 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.177 |
-0.708 |
0.000 |
| y |
-0.708 |
9.922 |
0.000 |
| z |
0.000 |
0.000 |
8.749 |
<r2> (average value of r
2) Å
2
| <r2> |
308.236 |
| (<r2>)1/2 |
17.557 |