Jump to
S1C2
Energy calculated at BLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -5226.880343 |
| Energy at 298.15K | -5226.890324 |
| HF Energy | -5226.880343 |
| Nuclear repulsion energy | 408.238192 |
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 BLYP/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 |
Ag |
3029 |
3034 |
0.00 |
|
|
|
| 2 |
Ag |
1426 |
1429 |
0.00 |
|
|
|
| 3 |
Ag |
1210 |
1212 |
0.00 |
|
|
|
| 4 |
Ag |
1030 |
1032 |
0.00 |
|
|
|
| 5 |
Ag |
606 |
607 |
0.00 |
|
|
|
| 6 |
Ag |
176 |
176 |
0.00 |
|
|
|
| 7 |
Au |
3115 |
3120 |
1.97 |
|
|
|
| 8 |
Au |
1041 |
1043 |
2.84 |
|
|
|
| 9 |
Au |
743 |
744 |
4.53 |
|
|
|
| 10 |
Au |
97 |
98 |
3.71 |
|
|
|
| 11 |
Bg |
3092 |
3097 |
0.00 |
|
|
|
| 12 |
Bg |
1231 |
1233 |
0.00 |
|
|
|
| 13 |
Bg |
893 |
895 |
0.00 |
|
|
|
| 14 |
Bu |
3036 |
3041 |
7.23 |
|
|
|
| 15 |
Bu |
1417 |
1419 |
3.47 |
|
|
|
| 16 |
Bu |
1145 |
1147 |
56.00 |
|
|
|
| 17 |
Bu |
538 |
539 |
84.51 |
|
|
|
| 18 |
Bu |
172 |
173 |
7.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 11999.3 cm
-1
Scaled (by 1.0016) Zero Point Vibrational Energy (zpe) 12018.5 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 BLYP/cc-pVDZ
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.501 |
0.570 |
0.000 |
| C2 |
-0.501 |
-0.570 |
0.000 |
| Br3 |
-0.501 |
2.317 |
0.000 |
| Br4 |
0.501 |
-2.317 |
0.000 |
| H5 |
1.130 |
0.587 |
0.906 |
| H6 |
1.130 |
0.587 |
-0.906 |
| H7 |
-1.130 |
-0.587 |
0.906 |
| H8 |
-1.130 |
-0.587 |
-0.906 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5183 | 2.0135 | 2.8873 | 1.1031 | 1.1031 | 2.1955 | 2.1955 |
C2 | 1.5183 | | 2.8873 | 2.0135 | 2.1955 | 2.1955 | 1.1031 | 1.1031 | Br3 | 2.0135 | 2.8873 | | 4.7410 | 2.5443 | 2.5443 | 3.1064 | 3.1064 | Br4 | 2.8873 | 2.0135 | 4.7410 | | 3.1064 | 3.1064 | 2.5443 | 2.5443 | H5 | 1.1031 | 2.1955 | 2.5443 | 3.1064 | | 1.8122 | 2.5466 | 3.1256 | H6 | 1.1031 | 2.1955 | 2.5443 | 3.1064 | 1.8122 | | 3.1256 | 2.5466 | H7 | 2.1955 | 1.1031 | 3.1064 | 2.5443 | 2.5466 | 3.1256 | | 1.8122 | H8 | 2.1955 | 1.1031 | 3.1064 | 2.5443 | 3.1256 | 2.5466 | 1.8122 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.865 |
|
C1 |
C2 |
H7 |
112.804 |
| C1 |
C2 |
H8 |
112.804 |
|
C2 |
C1 |
Br3 |
108.865 |
| C2 |
C1 |
H5 |
112.804 |
|
C2 |
C1 |
H6 |
112.804 |
| Br3 |
C1 |
H5 |
105.703 |
|
Br3 |
C1 |
H6 |
105.703 |
| Br4 |
C2 |
H7 |
105.703 |
|
Br4 |
C2 |
H8 |
105.703 |
| H5 |
C1 |
H6 |
110.448 |
|
H7 |
C2 |
H8 |
110.448 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.034 |
|
|
|
| 2 |
C |
-0.034 |
|
|
|
| 3 |
Br |
-0.106 |
|
|
|
| 4 |
Br |
-0.106 |
|
|
|
| 5 |
H |
0.070 |
|
|
|
| 6 |
H |
0.070 |
|
|
|
| 7 |
H |
0.070 |
|
|
|
| 8 |
H |
0.070 |
|
|
|
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 |
-48.533 |
1.124 |
0.000 |
| y |
1.124 |
-54.817 |
0.000 |
| z |
0.000 |
0.000 |
-49.229 |
|
| Traceless |
| | x | y | z |
| x |
3.490 |
1.124 |
0.000 |
| y |
1.124 |
-5.936 |
0.000 |
| z |
0.000 |
0.000 |
2.446 |
|
| Polar |
| 3z2-r2 | 4.892 |
| x2-y2 | 6.284 |
| xy | 1.124 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.666 |
-2.149 |
0.000 |
| y |
-2.149 |
13.315 |
0.000 |
| z |
0.000 |
0.000 |
5.446 |
<r2> (average value of r
2) Å
2
| <r2> |
441.794 |
| (<r2>)1/2 |
21.019 |
Jump to
S1C1
Energy calculated at BLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -5226.876252 |
| Energy at 298.15K | |
| HF Energy | -5226.876252 |
| Nuclear repulsion energy | 440.457031 |
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 BLYP/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 |
3067 |
3072 |
0.02 |
115.10 |
0.74 |
0.85 |
| 2 |
A |
3002 |
3007 |
16.00 |
278.65 |
0.02 |
0.03 |
| 3 |
A |
1396 |
1398 |
0.74 |
4.44 |
0.71 |
0.83 |
| 4 |
A |
1246 |
1248 |
23.61 |
4.49 |
0.58 |
0.74 |
| 5 |
A |
1131 |
1133 |
3.30 |
17.87 |
0.75 |
0.86 |
| 6 |
A |
996 |
997 |
2.06 |
3.57 |
0.56 |
0.72 |
| 7 |
A |
862 |
863 |
8.23 |
10.35 |
0.49 |
0.66 |
| 8 |
A |
512 |
513 |
9.43 |
17.12 |
0.08 |
0.14 |
| 9 |
A |
219 |
219 |
1.24 |
2.20 |
0.38 |
0.55 |
| 10 |
A |
73 |
73 |
0.19 |
1.62 |
0.71 |
0.83 |
| 11 |
B |
3080 |
3085 |
2.68 |
31.30 |
0.75 |
0.86 |
| 12 |
B |
2992 |
2997 |
2.02 |
71.90 |
0.75 |
0.86 |
| 13 |
B |
1389 |
1391 |
7.41 |
16.59 |
0.75 |
0.86 |
| 14 |
B |
1211 |
1212 |
78.68 |
2.63 |
0.75 |
0.86 |
| 15 |
B |
1066 |
1068 |
1.76 |
6.36 |
0.75 |
0.86 |
| 16 |
B |
805 |
807 |
20.04 |
0.88 |
0.75 |
0.86 |
| 17 |
B |
543 |
544 |
19.60 |
9.80 |
0.75 |
0.86 |
| 18 |
B |
338 |
338 |
8.21 |
3.76 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11963.0 cm
-1
Scaled (by 1.0016) Zero Point Vibrational Energy (zpe) 11982.1 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 BLYP/cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.314 |
0.692 |
1.199 |
| C2 |
-0.314 |
-0.692 |
1.199 |
| Br3 |
-0.314 |
1.857 |
-0.298 |
| Br4 |
0.314 |
-1.857 |
-0.298 |
| H5 |
0.022 |
1.231 |
2.122 |
| H6 |
1.414 |
0.659 |
1.116 |
| H7 |
-0.022 |
-1.231 |
2.122 |
| H8 |
-1.414 |
-0.659 |
1.116 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5201 | 1.9979 | 2.9564 | 1.1073 | 1.1039 | 2.1594 | 2.1949 |
C2 | 1.5201 | | 2.9564 | 1.9979 | 2.1594 | 2.1949 | 1.1073 | 1.1039 | Br3 | 1.9979 | 2.9564 | | 3.7669 | 2.5218 | 2.5340 | 3.9339 | 3.0888 | Br4 | 2.9564 | 1.9979 | 3.7669 | | 3.9339 | 3.0888 | 2.5218 | 2.5340 | H5 | 1.1073 | 2.1594 | 2.5218 | 3.9339 | | 1.8096 | 2.4624 | 2.5779 | H6 | 1.1039 | 2.1949 | 2.5340 | 3.0888 | 1.8096 | | 2.5779 | 3.1200 | H7 | 2.1594 | 1.1073 | 3.9339 | 2.5218 | 2.4624 | 2.5779 | | 1.8096 | H8 | 2.1949 | 1.1039 | 3.0888 | 2.5340 | 2.5779 | 3.1200 | 1.8096 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.665 |
|
C1 |
C2 |
H7 |
109.542 |
| C1 |
C2 |
H8 |
112.575 |
|
C2 |
C1 |
Br3 |
113.665 |
| C2 |
C1 |
H5 |
109.542 |
|
C2 |
C1 |
H6 |
112.575 |
| Br3 |
C1 |
H5 |
104.952 |
|
Br3 |
C1 |
H6 |
105.932 |
| Br4 |
C2 |
H7 |
104.952 |
|
Br4 |
C2 |
H8 |
105.932 |
| H5 |
C1 |
H6 |
109.842 |
|
H7 |
C2 |
H8 |
109.842 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.038 |
|
|
|
| 2 |
C |
-0.038 |
|
|
|
| 3 |
Br |
-0.095 |
|
|
|
| 4 |
Br |
-0.095 |
|
|
|
| 5 |
H |
0.063 |
|
|
|
| 6 |
H |
0.070 |
|
|
|
| 7 |
H |
0.063 |
|
|
|
| 8 |
H |
0.070 |
|
|
|
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 |
2.470 |
2.470 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.941 |
0.755 |
0.000 |
| y |
0.755 |
-53.027 |
0.000 |
| z |
0.000 |
0.000 |
-44.900 |
|
| Traceless |
| | x | y | z |
| x |
0.023 |
0.755 |
0.000 |
| y |
0.755 |
-6.106 |
0.000 |
| z |
0.000 |
0.000 |
6.084 |
|
| Polar |
| 3z2-r2 | 12.167 |
| x2-y2 | 4.086 |
| xy | 0.755 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.922 |
-0.823 |
0.000 |
| y |
-0.823 |
9.475 |
0.000 |
| z |
0.000 |
0.000 |
8.199 |
<r2> (average value of r
2) Å
2
| <r2> |
328.687 |
| (<r2>)1/2 |
18.130 |