Jump to
S1C2
Energy calculated at wB97X-D/3-21G
| hartrees |
Energy at 0K | -5201.841382 |
Energy at 298.15K | |
HF Energy | -5201.841382 |
Nuclear repulsion energy | 413.039395 |
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 wB97X-D/3-21G
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 |
3166 |
3166 |
0.00 |
150.47 |
0.08 |
0.15 |
2 |
Ag |
1539 |
1539 |
0.00 |
24.83 |
0.75 |
0.86 |
3 |
Ag |
1350 |
1350 |
0.00 |
42.68 |
0.48 |
0.65 |
4 |
Ag |
1070 |
1070 |
0.00 |
26.81 |
0.64 |
0.78 |
5 |
Ag |
706 |
706 |
0.00 |
77.52 |
0.32 |
0.48 |
6 |
Ag |
195 |
195 |
0.00 |
5.09 |
0.40 |
0.58 |
7 |
Au |
3253 |
3253 |
0.58 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1170 |
1170 |
2.15 |
0.00 |
0.00 |
0.00 |
9 |
Au |
783 |
783 |
10.11 |
0.00 |
0.00 |
0.00 |
10 |
Au |
107 |
107 |
4.48 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3229 |
3229 |
0.00 |
100.20 |
0.75 |
0.86 |
12 |
Bg |
1352 |
1352 |
0.00 |
12.73 |
0.75 |
0.86 |
13 |
Bg |
954 |
954 |
0.00 |
16.43 |
0.75 |
0.86 |
14 |
Bu |
3174 |
3174 |
4.25 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1537 |
1537 |
23.33 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1284 |
1284 |
40.69 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
638 |
638 |
59.06 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
187 |
187 |
6.29 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12845.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12845.6 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 wB97X-D/3-21G
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.497 |
0.569 |
0.000 |
C2 |
-0.497 |
-0.569 |
0.000 |
Br3 |
-0.497 |
2.289 |
0.000 |
Br4 |
0.497 |
-2.289 |
0.000 |
H5 |
1.117 |
0.565 |
0.894 |
H6 |
1.117 |
0.565 |
-0.894 |
H7 |
-1.117 |
-0.565 |
0.894 |
H8 |
-1.117 |
-0.565 |
-0.894 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5117 | 1.9869 | 2.8587 | 1.0877 | 1.0877 | 2.1661 | 2.1661 |
C2 | 1.5117 | | 2.8587 | 1.9869 | 2.1661 | 2.1661 | 1.0877 | 1.0877 | Br3 | 1.9869 | 2.8587 | | 4.6856 | 2.5254 | 2.5254 | 3.0549 | 3.0549 | Br4 | 2.8587 | 1.9869 | 4.6856 | | 3.0549 | 3.0549 | 2.5254 | 2.5254 | H5 | 1.0877 | 2.1661 | 2.5254 | 3.0549 | | 1.7877 | 2.5038 | 3.0765 | H6 | 1.0877 | 2.1661 | 2.5254 | 3.0549 | 1.7877 | | 3.0765 | 2.5038 | H7 | 2.1661 | 1.0877 | 3.0549 | 2.5254 | 2.5038 | 3.0765 | | 1.7877 | H8 | 2.1661 | 1.0877 | 3.0549 | 2.5254 | 3.0765 | 2.5038 | 1.7877 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
108.832 |
|
C1 |
C2 |
H7 |
111.841 |
C1 |
C2 |
H8 |
111.841 |
|
C2 |
C1 |
Br3 |
108.832 |
C2 |
C1 |
H5 |
111.841 |
|
C2 |
C1 |
H6 |
111.841 |
Br3 |
C1 |
H5 |
106.765 |
|
Br3 |
C1 |
H6 |
106.765 |
Br4 |
C2 |
H7 |
106.765 |
|
Br4 |
C2 |
H8 |
106.765 |
H5 |
C1 |
H6 |
110.522 |
|
H7 |
C2 |
H8 |
110.522 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.640 |
|
|
|
2 |
C |
-0.640 |
|
|
|
3 |
Br |
0.058 |
|
|
|
4 |
Br |
0.058 |
|
|
|
5 |
H |
0.291 |
|
|
|
6 |
H |
0.291 |
|
|
|
7 |
H |
0.291 |
|
|
|
8 |
H |
0.291 |
|
|
|
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 |
-48.343 |
1.530 |
0.000 |
y |
1.530 |
-55.993 |
0.000 |
z |
0.000 |
0.000 |
-48.903 |
|
Traceless |
| x | y | z |
x |
4.105 |
1.530 |
0.000 |
y |
1.530 |
-7.370 |
0.000 |
z |
0.000 |
0.000 |
3.265 |
|
Polar |
3z2-r2 | 6.530 |
x2-y2 | 7.650 |
xy | 1.530 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.964 |
-2.611 |
0.000 |
y |
-2.611 |
10.687 |
0.000 |
z |
0.000 |
0.000 |
3.613 |
<r2> (average value of r
2) Å
2
<r2> |
432.435 |
(<r2>)1/2 |
20.795 |
Jump to
S1C1
Energy calculated at wB97X-D/3-21G
| hartrees |
Energy at 0K | -5201.837944 |
Energy at 298.15K | |
HF Energy | -5201.837944 |
Nuclear repulsion energy | 447.192523 |
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 wB97X-D/3-21G
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 |
3214 |
3214 |
0.00 |
107.29 |
0.75 |
0.86 |
2 |
A |
3152 |
3152 |
8.17 |
195.22 |
0.02 |
0.03 |
3 |
A |
1520 |
1520 |
1.91 |
8.99 |
0.73 |
0.84 |
4 |
A |
1372 |
1372 |
18.80 |
5.88 |
0.62 |
0.77 |
5 |
A |
1246 |
1246 |
1.25 |
27.34 |
0.75 |
0.86 |
6 |
A |
1057 |
1057 |
3.14 |
3.96 |
0.64 |
0.78 |
7 |
A |
922 |
922 |
11.71 |
15.04 |
0.53 |
0.70 |
8 |
A |
578 |
578 |
6.94 |
17.42 |
0.13 |
0.23 |
9 |
A |
236 |
236 |
1.31 |
2.05 |
0.44 |
0.62 |
10 |
A |
80 |
80 |
0.29 |
2.14 |
0.74 |
0.85 |
11 |
B |
3227 |
3227 |
0.78 |
29.04 |
0.75 |
0.86 |
12 |
B |
3144 |
3144 |
1.89 |
53.33 |
0.75 |
0.86 |
13 |
B |
1524 |
1524 |
26.31 |
24.32 |
0.75 |
0.86 |
14 |
B |
1344 |
1344 |
46.69 |
1.97 |
0.75 |
0.86 |
15 |
B |
1189 |
1189 |
1.81 |
10.95 |
0.75 |
0.86 |
16 |
B |
865 |
865 |
26.86 |
1.96 |
0.75 |
0.86 |
17 |
B |
618 |
618 |
13.11 |
15.50 |
0.75 |
0.86 |
18 |
B |
369 |
369 |
5.32 |
4.31 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12827.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12827.7 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 wB97X-D/3-21G
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.314 |
0.688 |
1.201 |
C2 |
-0.314 |
-0.688 |
1.201 |
Br3 |
-0.314 |
1.816 |
-0.298 |
Br4 |
0.314 |
-1.816 |
-0.298 |
H5 |
0.032 |
1.218 |
2.112 |
H6 |
1.398 |
0.635 |
1.123 |
H7 |
-0.032 |
-1.218 |
2.112 |
H8 |
-1.398 |
-0.635 |
1.123 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5124 | 1.9785 | 2.9182 | 1.0909 | 1.0883 | 2.1407 | 2.1652 |
C2 | 1.5124 | | 2.9182 | 1.9785 | 2.1407 | 2.1652 | 1.0909 | 1.0883 | Br3 | 1.9785 | 2.9182 | | 3.6849 | 2.5069 | 2.5188 | 3.8849 | 3.0332 | Br4 | 2.9182 | 1.9785 | 3.6849 | | 3.8849 | 3.0332 | 2.5069 | 2.5188 | H5 | 1.0909 | 2.1407 | 2.5069 | 3.8849 | | 1.7849 | 2.4376 | 2.5413 | H6 | 1.0883 | 2.1652 | 2.5188 | 3.0332 | 1.7849 | | 2.5413 | 3.0714 | H7 | 2.1407 | 1.0909 | 3.8849 | 2.5069 | 2.4376 | 2.5413 | | 1.7849 | H8 | 2.1652 | 1.0883 | 3.0332 | 2.5188 | 2.5413 | 3.0714 | 1.7849 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
112.748 |
|
C1 |
C2 |
H7 |
109.566 |
C1 |
C2 |
H8 |
111.684 |
|
C2 |
C1 |
Br3 |
112.748 |
C2 |
C1 |
H5 |
109.566 |
|
C2 |
C1 |
H6 |
111.684 |
Br3 |
C1 |
H5 |
105.861 |
|
Br3 |
C1 |
H6 |
106.806 |
Br4 |
C2 |
H7 |
105.861 |
|
Br4 |
C2 |
H8 |
106.806 |
H5 |
C1 |
H6 |
109.979 |
|
H7 |
C2 |
H8 |
109.979 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.647 |
|
|
|
2 |
C |
-0.647 |
|
|
|
3 |
Br |
0.073 |
|
|
|
4 |
Br |
0.073 |
|
|
|
5 |
H |
0.284 |
|
|
|
6 |
H |
0.291 |
|
|
|
7 |
H |
0.284 |
|
|
|
8 |
H |
0.291 |
|
|
|
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 |
2.712 |
2.712 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.667 |
0.915 |
0.000 |
y |
0.915 |
-53.132 |
0.000 |
z |
0.000 |
0.000 |
-44.900 |
|
Traceless |
| x | y | z |
x |
0.349 |
0.915 |
0.000 |
y |
0.915 |
-6.348 |
0.000 |
z |
0.000 |
0.000 |
5.999 |
|
Polar |
3z2-r2 | 11.999 |
x2-y2 | 4.465 |
xy | 0.915 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.147 |
-1.072 |
0.000 |
y |
-1.072 |
7.076 |
0.000 |
z |
0.000 |
0.000 |
6.800 |
<r2> (average value of r
2) Å
2
<r2> |
317.705 |
(<r2>)1/2 |
17.824 |