Jump to
S1C2
Energy calculated at M06-2X/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -5226.956964 |
Energy at 298.15K | |
HF Energy | -5226.956964 |
Nuclear repulsion energy | 419.048313 |
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 M06-2X/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 |
3127 |
3127 |
0.00 |
141.27 |
0.03 |
0.05 |
2 |
Ag |
1495 |
1495 |
0.00 |
6.54 |
0.68 |
0.81 |
3 |
Ag |
1298 |
1298 |
0.00 |
42.45 |
0.28 |
0.44 |
4 |
Ag |
1083 |
1083 |
0.00 |
7.38 |
0.75 |
0.86 |
5 |
Ag |
701 |
701 |
0.00 |
85.31 |
0.24 |
0.39 |
6 |
Ag |
197 |
197 |
0.00 |
4.62 |
0.22 |
0.36 |
7 |
Au |
3210 |
3210 |
0.39 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1119 |
1119 |
2.23 |
0.00 |
0.00 |
0.00 |
9 |
Au |
756 |
756 |
3.02 |
0.00 |
0.00 |
0.00 |
10 |
Au |
115 |
115 |
4.58 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3188 |
3188 |
0.00 |
64.42 |
0.75 |
0.86 |
12 |
Bg |
1293 |
1293 |
0.00 |
2.22 |
0.75 |
0.86 |
13 |
Bg |
961 |
961 |
0.00 |
1.08 |
0.75 |
0.86 |
14 |
Bu |
3135 |
3135 |
3.38 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1491 |
1491 |
8.52 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1223 |
1223 |
50.65 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
631 |
631 |
70.76 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
189 |
189 |
6.28 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12605.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12605.9 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 M06-2X/6-311+G(3df,2p)
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.492 |
0.570 |
0.000 |
C2 |
-0.492 |
-0.570 |
0.000 |
Br3 |
-0.492 |
2.253 |
0.000 |
Br4 |
0.492 |
-2.253 |
0.000 |
H5 |
1.112 |
0.573 |
0.890 |
H6 |
1.112 |
0.573 |
-0.890 |
H7 |
-1.112 |
-0.573 |
0.890 |
H8 |
-1.112 |
-0.573 |
-0.890 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5063 | 1.9502 | 2.8234 | 1.0844 | 1.0844 | 2.1614 | 2.1614 |
C2 | 1.5063 | | 2.8234 | 1.9502 | 2.1614 | 2.1614 | 1.0844 | 1.0844 | Br3 | 1.9502 | 2.8234 | | 4.6132 | 2.4882 | 2.4882 | 3.0270 | 3.0270 | Br4 | 2.8234 | 1.9502 | 4.6132 | | 3.0270 | 3.0270 | 2.4882 | 2.4882 | H5 | 1.0844 | 2.1614 | 2.4882 | 3.0270 | | 1.7794 | 2.5021 | 3.0703 | H6 | 1.0844 | 2.1614 | 2.4882 | 3.0270 | 1.7794 | | 3.0703 | 2.5021 | H7 | 2.1614 | 1.0844 | 3.0270 | 2.4882 | 2.5021 | 3.0703 | | 1.7794 | H8 | 2.1614 | 1.0844 | 3.0270 | 2.4882 | 3.0703 | 2.5021 | 1.7794 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
108.864 |
|
C1 |
C2 |
H7 |
112.058 |
C1 |
C2 |
H8 |
112.058 |
|
C2 |
C1 |
Br3 |
108.864 |
C2 |
C1 |
H5 |
112.058 |
|
C2 |
C1 |
H6 |
112.058 |
Br3 |
C1 |
H5 |
106.649 |
|
Br3 |
C1 |
H6 |
106.649 |
Br4 |
C2 |
H7 |
106.649 |
|
Br4 |
C2 |
H8 |
106.649 |
H5 |
C1 |
H6 |
110.258 |
|
H7 |
C2 |
H8 |
110.258 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.434 |
|
|
|
2 |
C |
-0.434 |
|
|
|
3 |
Br |
-0.071 |
|
|
|
4 |
Br |
-0.071 |
|
|
|
5 |
H |
0.253 |
|
|
|
6 |
H |
0.253 |
|
|
|
7 |
H |
0.253 |
|
|
|
8 |
H |
0.253 |
|
|
|
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 |
-49.245 |
1.494 |
0.000 |
y |
1.494 |
-56.323 |
0.000 |
z |
0.000 |
0.000 |
-49.862 |
|
Traceless |
| x | y | z |
x |
3.847 |
1.494 |
0.000 |
y |
1.494 |
-6.770 |
0.000 |
z |
0.000 |
0.000 |
2.923 |
|
Polar |
3z2-r2 | 5.845 |
x2-y2 | 7.078 |
xy | 1.494 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.943 |
-1.665 |
0.000 |
y |
-1.665 |
14.258 |
0.000 |
z |
0.000 |
0.000 |
8.145 |
<r2> (average value of r
2) Å
2
<r2> |
421.016 |
(<r2>)1/2 |
20.519 |
Jump to
S1C1
Energy calculated at M06-2X/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -5226.954159 |
Energy at 298.15K | |
HF Energy | -5226.954159 |
Nuclear repulsion energy | 454.450433 |
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 M06-2X/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 |
3170 |
3170 |
0.05 |
74.17 |
0.75 |
0.86 |
2 |
A |
3111 |
3111 |
9.82 |
219.63 |
0.02 |
0.04 |
3 |
A |
1476 |
1476 |
0.76 |
3.23 |
0.69 |
0.81 |
4 |
A |
1318 |
1318 |
17.30 |
4.11 |
0.12 |
0.21 |
5 |
A |
1206 |
1206 |
0.70 |
5.00 |
0.74 |
0.85 |
6 |
A |
1050 |
1050 |
1.00 |
1.22 |
0.70 |
0.82 |
7 |
A |
923 |
923 |
7.11 |
4.06 |
0.17 |
0.29 |
8 |
A |
583 |
583 |
7.85 |
23.28 |
0.05 |
0.10 |
9 |
A |
236 |
236 |
1.13 |
1.22 |
0.20 |
0.34 |
10 |
A |
84 |
84 |
0.22 |
0.76 |
0.60 |
0.75 |
11 |
B |
3182 |
3182 |
0.04 |
25.24 |
0.75 |
0.86 |
12 |
B |
3104 |
3104 |
2.05 |
33.60 |
0.75 |
0.86 |
13 |
B |
1472 |
1472 |
13.23 |
8.24 |
0.75 |
0.86 |
14 |
B |
1287 |
1287 |
59.05 |
3.11 |
0.75 |
0.86 |
15 |
B |
1136 |
1136 |
1.11 |
1.12 |
0.75 |
0.86 |
16 |
B |
861 |
861 |
17.84 |
0.92 |
0.75 |
0.86 |
17 |
B |
618 |
618 |
14.53 |
8.01 |
0.75 |
0.86 |
18 |
B |
366 |
366 |
5.88 |
1.88 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12590.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12590.9 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 M06-2X/6-311+G(3df,2p)
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.308 |
0.688 |
1.186 |
C2 |
-0.308 |
-0.688 |
1.186 |
Br3 |
-0.308 |
1.782 |
-0.295 |
Br4 |
0.308 |
-1.782 |
-0.295 |
H5 |
0.019 |
1.218 |
2.090 |
H6 |
1.390 |
0.646 |
1.112 |
H7 |
-0.019 |
-1.218 |
2.090 |
H8 |
-1.390 |
-0.646 |
1.112 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5073 | 1.9413 | 2.8794 | 1.0873 | 1.0852 | 2.1348 | 2.1606 |
C2 | 1.5073 | | 2.8794 | 1.9413 | 2.1348 | 2.1606 | 1.0873 | 1.0852 | Br3 | 1.9413 | 2.8794 | | 3.6163 | 2.4720 | 2.4802 | 3.8433 | 3.0076 | Br4 | 2.8794 | 1.9413 | 3.6163 | | 3.8433 | 3.0076 | 2.4720 | 2.4802 | H5 | 1.0873 | 2.1348 | 2.4720 | 3.8433 | | 1.7786 | 2.4370 | 2.5332 | H6 | 1.0852 | 2.1606 | 2.4802 | 3.0076 | 1.7786 | | 2.5332 | 3.0657 | H7 | 2.1348 | 1.0873 | 3.8433 | 2.4720 | 2.4370 | 2.5332 | | 1.7786 | H8 | 2.1606 | 1.0852 | 3.0076 | 2.4802 | 2.5332 | 3.0657 | 1.7786 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
112.618 |
|
C1 |
C2 |
H7 |
109.668 |
C1 |
C2 |
H8 |
111.876 |
|
C2 |
C1 |
Br3 |
112.618 |
C2 |
C1 |
H5 |
109.668 |
|
C2 |
C1 |
H6 |
111.876 |
Br3 |
C1 |
H5 |
105.944 |
|
Br3 |
C1 |
H6 |
106.622 |
Br4 |
C2 |
H7 |
105.944 |
|
Br4 |
C2 |
H8 |
106.622 |
H5 |
C1 |
H6 |
109.904 |
|
H7 |
C2 |
H8 |
109.904 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.413 |
|
|
|
2 |
C |
-0.413 |
|
|
|
3 |
Br |
-0.067 |
|
|
|
4 |
Br |
-0.067 |
|
|
|
5 |
H |
0.234 |
|
|
|
6 |
H |
0.246 |
|
|
|
7 |
H |
0.234 |
|
|
|
8 |
H |
0.246 |
|
|
|
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 |
2.665 |
2.665 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-49.666 |
1.025 |
0.000 |
y |
1.025 |
-54.238 |
0.000 |
z |
0.000 |
0.000 |
-45.369 |
|
Traceless |
| x | y | z |
x |
0.138 |
1.025 |
0.000 |
y |
1.025 |
-6.721 |
0.000 |
z |
0.000 |
0.000 |
6.583 |
|
Polar |
3z2-r2 | 13.166 |
x2-y2 | 4.572 |
xy | 1.025 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.410 |
-0.669 |
0.000 |
y |
-0.669 |
11.547 |
0.000 |
z |
0.000 |
0.000 |
9.928 |
<r2> (average value of r
2) Å
2
<r2> |
308.593 |
(<r2>)1/2 |
17.567 |