Jump to
S1C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -5229.503031 |
| Energy at 298.15K | |
| HF Energy | -5229.503031 |
| Nuclear repulsion energy | 413.562198 |
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 B97D3/6-311+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 |
3055 |
3015 |
0.00 |
153.85 |
0.02 |
0.04 |
| 2 |
Ag |
1460 |
1441 |
0.00 |
5.32 |
0.74 |
0.85 |
| 3 |
Ag |
1242 |
1226 |
0.00 |
57.30 |
0.28 |
0.44 |
| 4 |
Ag |
1043 |
1029 |
0.00 |
12.59 |
0.67 |
0.80 |
| 5 |
Ag |
618 |
610 |
0.00 |
145.26 |
0.26 |
0.41 |
| 6 |
Ag |
181 |
178 |
0.00 |
6.18 |
0.22 |
0.35 |
| 7 |
Au |
3141 |
3100 |
0.48 |
0.00 |
0.00 |
0.00 |
| 8 |
Au |
1073 |
1059 |
2.35 |
0.00 |
0.00 |
0.00 |
| 9 |
Au |
747 |
737 |
3.27 |
0.00 |
0.00 |
0.00 |
| 10 |
Au |
101 |
99 |
4.29 |
0.00 |
0.00 |
0.00 |
| 11 |
Bg |
3116 |
3076 |
0.00 |
73.08 |
0.75 |
0.86 |
| 12 |
Bg |
1257 |
1241 |
0.00 |
1.72 |
0.75 |
0.86 |
| 13 |
Bg |
921 |
909 |
0.00 |
0.90 |
0.75 |
0.86 |
| 14 |
Bu |
3064 |
3024 |
5.33 |
0.00 |
0.00 |
0.00 |
| 15 |
Bu |
1455 |
1437 |
6.15 |
0.00 |
0.00 |
0.00 |
| 16 |
Bu |
1178 |
1163 |
50.55 |
0.00 |
0.00 |
0.00 |
| 17 |
Bu |
548 |
541 |
87.81 |
0.00 |
0.00 |
0.00 |
| 18 |
Bu |
175 |
172 |
7.47 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12185.9 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 12027.5 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 B97D3/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.499 |
0.564 |
0.000 |
| C2 |
-0.499 |
-0.564 |
0.000 |
| Br3 |
-0.499 |
2.285 |
0.000 |
| Br4 |
0.499 |
-2.285 |
0.000 |
| H5 |
1.118 |
0.579 |
0.895 |
| H6 |
1.118 |
0.579 |
-0.895 |
| H7 |
-1.118 |
-0.579 |
0.895 |
| H8 |
-1.118 |
-0.579 |
-0.895 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5057 | 1.9886 | 2.8487 | 1.0884 | 1.0884 | 2.1725 | 2.1725 |
C2 | 1.5057 | | 2.8487 | 1.9886 | 2.1725 | 2.1725 | 1.0884 | 1.0884 | Br3 | 1.9886 | 2.8487 | | 4.6767 | 2.5146 | 2.5146 | 3.0633 | 3.0633 | Br4 | 2.8487 | 1.9886 | 4.6767 | | 3.0633 | 3.0633 | 2.5146 | 2.5146 | H5 | 1.0884 | 2.1725 | 2.5146 | 3.0633 | | 1.7898 | 2.5176 | 3.0890 | H6 | 1.0884 | 2.1725 | 2.5146 | 3.0633 | 1.7898 | | 3.0890 | 2.5176 | H7 | 2.1725 | 1.0884 | 3.0633 | 2.5146 | 2.5176 | 3.0890 | | 1.7898 | H8 | 2.1725 | 1.0884 | 3.0633 | 2.5146 | 3.0890 | 2.5176 | 1.7898 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
108.432 |
|
C1 |
C2 |
H7 |
112.767 |
| C1 |
C2 |
H8 |
112.767 |
|
C2 |
C1 |
Br3 |
108.432 |
| C2 |
C1 |
H5 |
112.767 |
|
C2 |
C1 |
H6 |
112.767 |
| Br3 |
C1 |
H5 |
105.878 |
|
Br3 |
C1 |
H6 |
105.878 |
| Br4 |
C2 |
H7 |
105.878 |
|
Br4 |
C2 |
H8 |
105.878 |
| H5 |
C1 |
H6 |
110.617 |
|
H7 |
C2 |
H8 |
110.617 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.236 |
|
|
|
| 2 |
C |
-0.236 |
|
|
|
| 3 |
Br |
-0.116 |
|
|
|
| 4 |
Br |
-0.116 |
|
|
|
| 5 |
H |
0.176 |
|
|
|
| 6 |
H |
0.176 |
|
|
|
| 7 |
H |
0.176 |
|
|
|
| 8 |
H |
0.176 |
|
|
|
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 |
-48.921 |
1.482 |
0.000 |
| y |
1.482 |
-56.056 |
0.000 |
| z |
0.000 |
0.000 |
-49.551 |
|
| Traceless |
| | x | y | z |
| x |
3.883 |
1.482 |
0.000 |
| y |
1.482 |
-6.820 |
0.000 |
| z |
0.000 |
0.000 |
2.937 |
|
| Polar |
| 3z2-r2 | 5.874 |
| x2-y2 | 7.135 |
| xy | 1.482 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.383 |
-1.792 |
0.000 |
| y |
-1.792 |
15.774 |
0.000 |
| z |
0.000 |
0.000 |
8.519 |
<r2> (average value of r
2) Å
2
| <r2> |
431.274 |
| (<r2>)1/2 |
20.767 |
Jump to
S1C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -5229.499394 |
| Energy at 298.15K | |
| HF Energy | -5229.499394 |
| Nuclear repulsion energy | 446.500038 |
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 B97D3/6-311+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 |
3093 |
3053 |
0.01 |
83.88 |
0.74 |
0.85 |
| 2 |
A |
3030 |
2991 |
16.53 |
269.16 |
0.02 |
0.04 |
| 3 |
A |
1435 |
1416 |
0.76 |
2.92 |
0.74 |
0.85 |
| 4 |
A |
1272 |
1256 |
17.20 |
6.60 |
0.15 |
0.26 |
| 5 |
A |
1157 |
1142 |
1.32 |
6.55 |
0.75 |
0.86 |
| 6 |
A |
1009 |
996 |
1.72 |
1.79 |
0.43 |
0.60 |
| 7 |
A |
881 |
870 |
7.62 |
5.86 |
0.20 |
0.34 |
| 8 |
A |
523 |
516 |
8.29 |
23.58 |
0.05 |
0.09 |
| 9 |
A |
225 |
222 |
1.44 |
1.87 |
0.16 |
0.27 |
| 10 |
A |
77 |
76 |
0.23 |
0.78 |
0.61 |
0.76 |
| 11 |
B |
3108 |
3067 |
1.51 |
26.64 |
0.75 |
0.86 |
| 12 |
B |
3021 |
2982 |
1.98 |
48.74 |
0.75 |
0.86 |
| 13 |
B |
1431 |
1413 |
11.01 |
9.46 |
0.75 |
0.86 |
| 14 |
B |
1239 |
1223 |
69.49 |
4.24 |
0.75 |
0.86 |
| 15 |
B |
1094 |
1080 |
1.21 |
1.14 |
0.75 |
0.86 |
| 16 |
B |
826 |
816 |
19.54 |
0.75 |
0.75 |
0.86 |
| 17 |
B |
555 |
548 |
19.14 |
7.75 |
0.75 |
0.86 |
| 18 |
B |
346 |
342 |
7.79 |
2.22 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12160.8 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 12002.7 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 B97D3/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.314 |
0.685 |
1.187 |
| C2 |
-0.314 |
-0.685 |
1.187 |
| Br3 |
-0.314 |
1.828 |
-0.295 |
| Br4 |
0.314 |
-1.828 |
-0.295 |
| H5 |
0.033 |
1.219 |
2.098 |
| H6 |
1.399 |
0.647 |
1.098 |
| H7 |
-0.033 |
-1.219 |
2.098 |
| H8 |
-1.399 |
-0.647 |
1.098 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5078 | 1.9738 | 2.9174 | 1.0926 | 1.0892 | 2.1394 | 2.1722 |
C2 | 1.5078 | | 2.9174 | 1.9738 | 2.1394 | 2.1722 | 1.0926 | 1.0892 | Br3 | 1.9738 | 2.9174 | | 3.7089 | 2.4933 | 2.5040 | 3.8843 | 3.0401 | Br4 | 2.9174 | 1.9738 | 3.7089 | | 3.8843 | 3.0401 | 2.4933 | 2.5040 | H5 | 1.0926 | 2.1394 | 2.4933 | 3.8843 | | 1.7869 | 2.4391 | 2.5558 | H6 | 1.0892 | 2.1722 | 2.5040 | 3.0401 | 1.7869 | | 2.5558 | 3.0829 | H7 | 2.1394 | 1.0926 | 3.8843 | 2.4933 | 2.4391 | 2.5558 | | 1.7869 | H8 | 2.1722 | 1.0892 | 3.0401 | 2.5040 | 2.5558 | 3.0829 | 1.7869 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.166 |
|
C1 |
C2 |
H7 |
109.680 |
| C1 |
C2 |
H8 |
112.532 |
|
C2 |
C1 |
Br3 |
113.166 |
| C2 |
C1 |
H5 |
109.680 |
|
C2 |
C1 |
H6 |
112.532 |
| Br3 |
C1 |
H5 |
105.143 |
|
Br3 |
C1 |
H6 |
106.035 |
| Br4 |
C2 |
H7 |
105.143 |
|
Br4 |
C2 |
H8 |
106.035 |
| H5 |
C1 |
H6 |
109.973 |
|
H7 |
C2 |
H8 |
109.973 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.208 |
|
|
|
| 2 |
C |
-0.208 |
|
|
|
| 3 |
Br |
-0.116 |
|
|
|
| 4 |
Br |
-0.116 |
|
|
|
| 5 |
H |
0.159 |
|
|
|
| 6 |
H |
0.165 |
|
|
|
| 7 |
H |
0.159 |
|
|
|
| 8 |
H |
0.165 |
|
|
|
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 |
2.621 |
2.621 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.312 |
1.030 |
0.000 |
| y |
1.030 |
-54.169 |
0.000 |
| z |
0.000 |
0.000 |
-45.104 |
|
| Traceless |
| | x | y | z |
| x |
0.324 |
1.030 |
0.000 |
| y |
1.030 |
-6.961 |
0.000 |
| z |
0.000 |
0.000 |
6.637 |
|
| Polar |
| 3z2-r2 | 13.274 |
| x2-y2 | 4.857 |
| xy | 1.030 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.818 |
-0.712 |
0.000 |
| y |
-0.712 |
12.430 |
0.000 |
| z |
0.000 |
0.000 |
10.365 |
<r2> (average value of r
2) Å
2
| <r2> |
320.419 |
| (<r2>)1/2 |
17.900 |