Jump to
S1C2
Energy calculated at B97D3/6-311G**
| hartrees |
Energy at 0K | -5229.490523 |
Energy at 298.15K | |
HF Energy | -5229.490523 |
Nuclear repulsion energy | 412.316579 |
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 B97D3/6-311G**
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 |
3062 |
3018 |
0.00 |
168.43 |
0.05 |
0.10 |
2 |
Ag |
1463 |
1442 |
0.00 |
11.67 |
0.75 |
0.86 |
3 |
Ag |
1253 |
1235 |
0.00 |
38.92 |
0.51 |
0.68 |
4 |
Ag |
1045 |
1030 |
0.00 |
20.75 |
0.64 |
0.78 |
5 |
Ag |
615 |
606 |
0.00 |
138.92 |
0.29 |
0.45 |
6 |
Ag |
180 |
178 |
0.00 |
5.68 |
0.35 |
0.51 |
7 |
Au |
3149 |
3104 |
3.45 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1079 |
1064 |
4.40 |
0.00 |
0.00 |
0.00 |
9 |
Au |
754 |
743 |
5.50 |
0.00 |
0.00 |
0.00 |
10 |
Au |
104 |
102 |
4.31 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3125 |
3080 |
0.00 |
96.83 |
0.75 |
0.86 |
12 |
Bg |
1262 |
1244 |
0.00 |
3.09 |
0.75 |
0.86 |
13 |
Bg |
925 |
912 |
0.00 |
6.06 |
0.75 |
0.86 |
14 |
Bu |
3070 |
3026 |
9.95 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1456 |
1435 |
5.86 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1187 |
1170 |
60.07 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
544 |
536 |
90.53 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
175 |
173 |
8.27 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12224.0 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 12049.2 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 B97D3/6-311G**
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.500 |
0.565 |
0.000 |
C2 |
-0.500 |
-0.565 |
0.000 |
Br3 |
-0.500 |
2.292 |
0.000 |
Br4 |
0.500 |
-2.292 |
0.000 |
H5 |
1.119 |
0.578 |
0.897 |
H6 |
1.119 |
0.578 |
-0.897 |
H7 |
-1.119 |
-0.578 |
0.897 |
H8 |
-1.119 |
-0.578 |
-0.897 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5087 | 1.9951 | 2.8573 | 1.0903 | 1.0903 | 2.1756 | 2.1756 |
C2 | 1.5087 | | 2.8573 | 1.9951 | 2.1756 | 2.1756 | 1.0903 | 1.0903 | Br3 | 1.9951 | 2.8573 | | 4.6918 | 2.5223 | 2.5223 | 3.0705 | 3.0705 | Br4 | 2.8573 | 1.9951 | 4.6918 | | 3.0705 | 3.0705 | 2.5223 | 2.5223 | H5 | 1.0903 | 2.1756 | 2.5223 | 3.0705 | | 1.7938 | 2.5200 | 3.0932 | H6 | 1.0903 | 2.1756 | 2.5223 | 3.0705 | 1.7938 | | 3.0932 | 2.5200 | H7 | 2.1756 | 1.0903 | 3.0705 | 2.5223 | 2.5200 | 3.0932 | | 1.7938 | H8 | 2.1756 | 1.0903 | 3.0705 | 2.5223 | 3.0932 | 2.5200 | 1.7938 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
108.473 |
|
C1 |
C2 |
H7 |
112.676 |
C1 |
C2 |
H8 |
112.676 |
|
C2 |
C1 |
Br3 |
108.473 |
C2 |
C1 |
H5 |
112.676 |
|
C2 |
C1 |
H6 |
112.676 |
Br3 |
C1 |
H5 |
105.918 |
|
Br3 |
C1 |
H6 |
105.918 |
Br4 |
C2 |
H7 |
105.918 |
|
Br4 |
C2 |
H8 |
105.918 |
H5 |
C1 |
H6 |
110.694 |
|
H7 |
C2 |
H8 |
110.694 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.295 |
|
|
|
2 |
C |
-0.295 |
|
|
|
3 |
Br |
-0.076 |
|
|
|
4 |
Br |
-0.076 |
|
|
|
5 |
H |
0.185 |
|
|
|
6 |
H |
0.185 |
|
|
|
7 |
H |
0.185 |
|
|
|
8 |
H |
0.185 |
|
|
|
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 |
-48.698 |
1.355 |
0.000 |
y |
1.355 |
-55.769 |
0.000 |
z |
0.000 |
0.000 |
-49.376 |
|
Traceless |
| x | y | z |
x |
3.875 |
1.355 |
0.000 |
y |
1.355 |
-6.732 |
0.000 |
z |
0.000 |
0.000 |
2.857 |
|
Polar |
3z2-r2 | 5.714 |
x2-y2 | 7.071 |
xy | 1.355 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.868 |
-2.235 |
0.000 |
y |
-2.235 |
13.830 |
0.000 |
z |
0.000 |
0.000 |
5.551 |
<r2> (average value of r
2) Å
2
<r2> |
433.647 |
(<r2>)1/2 |
20.824 |
Jump to
S1C1
Energy calculated at B97D3/6-311G**
| hartrees |
Energy at 0K | -5229.486668 |
Energy at 298.15K | |
HF Energy | -5229.486668 |
Nuclear repulsion energy | 445.024402 |
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 B97D3/6-311G**
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 |
3101 |
3057 |
0.16 |
107.75 |
0.75 |
0.86 |
2 |
A |
3037 |
2993 |
20.46 |
272.63 |
0.02 |
0.03 |
3 |
A |
1438 |
1417 |
0.91 |
3.79 |
0.69 |
0.82 |
4 |
A |
1282 |
1263 |
24.22 |
5.20 |
0.59 |
0.74 |
5 |
A |
1164 |
1147 |
3.08 |
16.69 |
0.75 |
0.86 |
6 |
A |
1012 |
997 |
1.05 |
3.24 |
0.52 |
0.69 |
7 |
A |
885 |
872 |
9.28 |
10.36 |
0.44 |
0.61 |
8 |
A |
519 |
512 |
9.81 |
17.19 |
0.07 |
0.14 |
9 |
A |
226 |
223 |
1.33 |
2.14 |
0.42 |
0.59 |
10 |
A |
78 |
77 |
0.21 |
1.55 |
0.73 |
0.84 |
11 |
B |
3116 |
3071 |
4.44 |
30.52 |
0.75 |
0.86 |
12 |
B |
3028 |
2985 |
2.85 |
68.26 |
0.75 |
0.86 |
13 |
B |
1431 |
1410 |
10.31 |
14.57 |
0.75 |
0.86 |
14 |
B |
1249 |
1231 |
77.76 |
2.71 |
0.75 |
0.86 |
15 |
B |
1100 |
1084 |
2.93 |
5.74 |
0.75 |
0.86 |
16 |
B |
828 |
816 |
22.94 |
1.32 |
0.75 |
0.86 |
17 |
B |
552 |
544 |
20.35 |
10.66 |
0.75 |
0.86 |
18 |
B |
346 |
341 |
8.63 |
3.28 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12194.6 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 12020.2 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 B97D3/6-311G**
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.314 |
0.687 |
1.190 |
C2 |
-0.314 |
-0.687 |
1.190 |
Br3 |
-0.314 |
1.835 |
-0.296 |
Br4 |
0.314 |
-1.835 |
-0.296 |
H5 |
0.028 |
1.220 |
2.103 |
H6 |
1.401 |
0.649 |
1.105 |
H7 |
-0.028 |
-1.220 |
2.103 |
H8 |
-1.401 |
-0.649 |
1.105 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5108 | 1.9797 | 2.9275 | 1.0946 | 1.0911 | 2.1415 | 2.1751 |
C2 | 1.5108 | | 2.9275 | 1.9797 | 2.1415 | 2.1751 | 1.0946 | 1.0911 | Br3 | 1.9797 | 2.9275 | | 3.7230 | 2.5002 | 2.5115 | 3.8945 | 3.0519 | Br4 | 2.9275 | 1.9797 | 3.7230 | | 3.8945 | 3.0519 | 2.5002 | 2.5115 | H5 | 1.0946 | 2.1415 | 2.5002 | 3.8945 | | 1.7904 | 2.4398 | 2.5552 | H6 | 1.0911 | 2.1751 | 2.5115 | 3.0519 | 1.7904 | | 2.5552 | 3.0873 | H7 | 2.1415 | 1.0946 | 3.8945 | 2.5002 | 2.4398 | 2.5552 | | 1.7904 | H8 | 2.1751 | 1.0911 | 3.0519 | 2.5115 | 2.5552 | 3.0873 | 1.7904 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.322 |
|
C1 |
C2 |
H7 |
109.524 |
C1 |
C2 |
H8 |
112.434 |
|
C2 |
C1 |
Br3 |
113.322 |
C2 |
C1 |
H5 |
109.524 |
|
C2 |
C1 |
H6 |
112.434 |
Br3 |
C1 |
H5 |
105.161 |
|
Br3 |
C1 |
H6 |
106.101 |
Br4 |
C2 |
H7 |
105.161 |
|
Br4 |
C2 |
H8 |
106.101 |
H5 |
C1 |
H6 |
110.003 |
|
H7 |
C2 |
H8 |
110.003 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.292 |
|
|
|
2 |
C |
-0.292 |
|
|
|
3 |
Br |
-0.063 |
|
|
|
4 |
Br |
-0.063 |
|
|
|
5 |
H |
0.171 |
|
|
|
6 |
H |
0.184 |
|
|
|
7 |
H |
0.171 |
|
|
|
8 |
H |
0.184 |
|
|
|
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 |
2.697 |
2.697 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.095 |
0.895 |
0.000 |
y |
0.895 |
-53.722 |
0.000 |
z |
0.000 |
0.000 |
-44.843 |
|
Traceless |
| x | y | z |
x |
0.188 |
0.895 |
0.000 |
y |
0.895 |
-6.752 |
0.000 |
z |
0.000 |
0.000 |
6.565 |
|
Polar |
3z2-r2 | 13.129 |
x2-y2 | 4.627 |
xy | 0.895 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.062 |
-0.850 |
0.000 |
y |
-0.850 |
9.796 |
0.000 |
z |
0.000 |
0.000 |
8.402 |
<r2> (average value of r
2) Å
2
<r2> |
322.320 |
(<r2>)1/2 |
17.953 |