Jump to
S1C2
Energy calculated at mPW1PW91/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -5227.257099 |
| Energy at 298.15K | |
| HF Energy | -5227.257099 |
| Nuclear repulsion energy | 418.833741 |
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 mPW1PW91/6-311+G(3df,2p)
| 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 |
3124 |
3124 |
0.00 |
147.58 |
0.02 |
0.05 |
| 2 |
Ag |
1489 |
1489 |
0.00 |
5.94 |
0.71 |
0.83 |
| 3 |
Ag |
1285 |
1285 |
0.00 |
47.79 |
0.29 |
0.45 |
| 4 |
Ag |
1084 |
1084 |
0.00 |
8.08 |
0.73 |
0.84 |
| 5 |
Ag |
683 |
683 |
0.00 |
98.66 |
0.25 |
0.40 |
| 6 |
Ag |
192 |
192 |
0.00 |
4.23 |
0.21 |
0.35 |
| 7 |
Au |
3208 |
3208 |
0.02 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1107 |
1107 |
2.43 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
757 |
757 |
3.69 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
102 |
102 |
4.42 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3184 |
3184 |
0.00 |
69.20 |
0.75 |
0.86 |
| 12 |
Bg |
1289 |
1289 |
0.00 |
1.91 |
0.75 |
0.86 |
| 13 |
Bg |
949 |
949 |
0.00 |
0.87 |
0.75 |
0.86 |
| 14 |
Bu |
3132 |
3132 |
4.18 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1484 |
1484 |
9.07 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1211 |
1211 |
46.32 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
615 |
615 |
70.37 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
178 |
178 |
6.72 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12536.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12536.1 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 mPW1PW91/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.491 |
0.568 |
0.000 |
| C2 |
-0.491 |
-0.568 |
0.000 |
| Br3 |
-0.491 |
2.256 |
0.000 |
| Br4 |
0.491 |
-2.256 |
0.000 |
| H5 |
1.112 |
0.576 |
0.889 |
| H6 |
1.112 |
0.576 |
-0.889 |
| H7 |
-1.112 |
-0.576 |
0.889 |
| H8 |
-1.112 |
-0.576 |
-0.889 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5011 | 1.9521 | 2.8239 | 1.0846 | 1.0846 | 2.1600 | 2.1600 |
C2 | 1.5011 | | 2.8239 | 1.9521 | 2.1600 | 2.1600 | 1.0846 | 1.0846 | Br3 | 1.9521 | 2.8239 | | 4.6171 | 2.4861 | 2.4861 | 3.0320 | 3.0320 | Br4 | 2.8239 | 1.9521 | 4.6171 | | 3.0320 | 3.0320 | 2.4861 | 2.4861 | H5 | 1.0846 | 2.1600 | 2.4861 | 3.0320 | | 1.7780 | 2.5039 | 3.0710 | H6 | 1.0846 | 2.1600 | 2.4861 | 3.0320 | 1.7780 | | 3.0710 | 2.5039 | H7 | 2.1600 | 1.0846 | 3.0320 | 2.4861 | 2.5039 | 3.0710 | | 1.7780 | H8 | 2.1600 | 1.0846 | 3.0320 | 2.4861 | 3.0710 | 2.5039 | 1.7780 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.022 |
|
C1 |
C2 |
H7 |
112.310 |
| C1 |
C2 |
H8 |
112.310 |
|
C2 |
C1 |
Br3 |
109.022 |
| C2 |
C1 |
H5 |
112.310 |
|
C2 |
C1 |
H6 |
112.310 |
| Br3 |
C1 |
H5 |
106.372 |
|
Br3 |
C1 |
H6 |
106.372 |
| Br4 |
C2 |
H7 |
106.372 |
|
Br4 |
C2 |
H8 |
106.372 |
| H5 |
C1 |
H6 |
110.099 |
|
H7 |
C2 |
H8 |
110.099 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.260 |
|
|
|
| 2 |
C |
-0.260 |
|
|
|
| 3 |
Br |
-0.099 |
|
|
|
| 4 |
Br |
-0.099 |
|
|
|
| 5 |
H |
0.180 |
|
|
|
| 6 |
H |
0.180 |
|
|
|
| 7 |
H |
0.180 |
|
|
|
| 8 |
H |
0.180 |
|
|
|
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 |
-48.827 |
1.418 |
0.000 |
| y |
1.418 |
-55.778 |
0.000 |
| z |
0.000 |
0.000 |
-49.469 |
|
| Traceless |
| | x | y | z |
| x |
3.797 |
1.418 |
0.000 |
| y |
1.418 |
-6.630 |
0.000 |
| z |
0.000 |
0.000 |
2.833 |
|
| Polar |
| 3z2-r2 | 5.666 |
| x2-y2 | 6.952 |
| xy | 1.418 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.006 |
-1.656 |
0.000 |
| y |
-1.656 |
14.515 |
0.000 |
| z |
0.000 |
0.000 |
8.181 |
<r2> (average value of r
2) Å
2
| <r2> |
421.320 |
| (<r2>)1/2 |
20.526 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -5227.253656 |
| Energy at 298.15K | |
| HF Energy | -5227.253656 |
| Nuclear repulsion energy | 452.582478 |
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 mPW1PW91/6-311+G(3df,2p)
| 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 |
3165 |
3165 |
0.00 |
79.45 |
0.75 |
0.86 |
| 2 |
A |
3105 |
3105 |
12.29 |
237.72 |
0.02 |
0.04 |
| 3 |
A |
1466 |
1466 |
1.25 |
2.99 |
0.72 |
0.83 |
| 4 |
A |
1311 |
1311 |
16.65 |
5.16 |
0.13 |
0.24 |
| 5 |
A |
1198 |
1198 |
0.81 |
5.29 |
0.74 |
0.85 |
| 6 |
A |
1049 |
1049 |
1.24 |
1.28 |
0.53 |
0.70 |
| 7 |
A |
912 |
912 |
7.27 |
4.48 |
0.17 |
0.30 |
| 8 |
A |
574 |
574 |
6.85 |
21.73 |
0.05 |
0.09 |
| 9 |
A |
228 |
228 |
1.30 |
1.29 |
0.19 |
0.32 |
| 10 |
A |
78 |
78 |
0.24 |
0.71 |
0.62 |
0.76 |
| 11 |
B |
3179 |
3179 |
0.28 |
25.36 |
0.75 |
0.86 |
| 12 |
B |
3096 |
3096 |
1.93 |
37.60 |
0.75 |
0.86 |
| 13 |
B |
1463 |
1463 |
14.41 |
8.50 |
0.75 |
0.86 |
| 14 |
B |
1279 |
1279 |
60.13 |
3.55 |
0.75 |
0.86 |
| 15 |
B |
1128 |
1128 |
1.21 |
1.09 |
0.75 |
0.86 |
| 16 |
B |
851 |
851 |
18.77 |
0.99 |
0.75 |
0.86 |
| 17 |
B |
607 |
607 |
14.57 |
7.50 |
0.75 |
0.86 |
| 18 |
B |
358 |
358 |
5.98 |
1.67 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12523.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12523.9 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 mPW1PW91/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.309 |
0.685 |
1.173 |
| C2 |
-0.309 |
-0.685 |
1.173 |
| Br3 |
-0.309 |
1.800 |
-0.292 |
| Br4 |
0.309 |
-1.800 |
-0.292 |
| H5 |
0.028 |
1.211 |
2.083 |
| H6 |
1.391 |
0.645 |
1.095 |
| H7 |
-0.028 |
-1.211 |
2.083 |
| H8 |
-1.391 |
-0.645 |
1.095 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5021 | 1.9419 | 2.8840 | 1.0881 | 1.0853 | 2.1298 | 2.1592 |
C2 | 1.5021 | | 2.8840 | 1.9419 | 2.1298 | 2.1592 | 1.0881 | 1.0853 | Br3 | 1.9419 | 2.8840 | | 3.6522 | 2.4693 | 2.4789 | 3.8451 | 3.0115 | Br4 | 2.8840 | 1.9419 | 3.6522 | | 3.8451 | 3.0115 | 2.4693 | 2.4789 | H5 | 1.0881 | 2.1298 | 2.4693 | 3.8451 | | 1.7757 | 2.4236 | 2.5367 | H6 | 1.0853 | 2.1592 | 2.4789 | 3.0115 | 1.7757 | | 2.5367 | 3.0658 | H7 | 2.1298 | 1.0881 | 3.8451 | 2.4693 | 2.4236 | 2.5367 | | 1.7757 | H8 | 2.1592 | 1.0853 | 3.0115 | 2.4789 | 2.5367 | 3.0658 | 1.7757 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.117 |
|
C1 |
C2 |
H7 |
109.590 |
| C1 |
C2 |
H8 |
112.123 |
|
C2 |
C1 |
Br3 |
113.117 |
| C2 |
C1 |
H5 |
109.590 |
|
C2 |
C1 |
H6 |
112.123 |
| Br3 |
C1 |
H5 |
105.688 |
|
Br3 |
C1 |
H6 |
106.489 |
| Br4 |
C2 |
H7 |
105.688 |
|
Br4 |
C2 |
H8 |
106.489 |
| H5 |
C1 |
H6 |
109.578 |
|
H7 |
C2 |
H8 |
109.578 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.226 |
|
|
|
| 2 |
C |
-0.226 |
|
|
|
| 3 |
Br |
-0.100 |
|
|
|
| 4 |
Br |
-0.100 |
|
|
|
| 5 |
H |
0.157 |
|
|
|
| 6 |
H |
0.169 |
|
|
|
| 7 |
H |
0.157 |
|
|
|
| 8 |
H |
0.169 |
|
|
|
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 |
2.605 |
2.605 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.235 |
0.995 |
0.000 |
| y |
0.995 |
-53.885 |
0.000 |
| z |
0.000 |
0.000 |
-45.060 |
|
| Traceless |
| | x | y | z |
| x |
0.238 |
0.995 |
0.000 |
| y |
0.995 |
-6.738 |
0.000 |
| z |
0.000 |
0.000 |
6.500 |
|
| Polar |
| 3z2-r2 | 13.000 |
| x2-y2 | 4.650 |
| xy | 0.995 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.465 |
-0.677 |
0.000 |
| y |
-0.677 |
11.727 |
0.000 |
| z |
0.000 |
0.000 |
9.950 |
<r2> (average value of r
2) Å
2
| <r2> |
312.228 |
| (<r2>)1/2 |
17.670 |