Jump to
S1C2
Energy calculated at wB97X-D/STO-3G
| hartrees |
Energy at 0K | -5169.848086 |
Energy at 298.15K | |
HF Energy | -5169.848086 |
Nuclear repulsion energy | 415.634901 |
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/STO-3G
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 |
3372 |
3372 |
0.00 |
71.77 |
0.11 |
0.20 |
2 |
Ag |
1658 |
1658 |
0.00 |
25.07 |
0.75 |
0.86 |
3 |
Ag |
1468 |
1468 |
0.00 |
11.48 |
0.28 |
0.44 |
4 |
Ag |
1119 |
1119 |
0.00 |
9.97 |
0.75 |
0.86 |
5 |
Ag |
839 |
839 |
0.00 |
26.41 |
0.33 |
0.49 |
6 |
Ag |
211 |
211 |
0.00 |
3.06 |
0.41 |
0.58 |
7 |
Au |
3497 |
3497 |
0.17 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1244 |
1244 |
0.30 |
0.00 |
0.00 |
0.00 |
9 |
Au |
802 |
802 |
3.20 |
0.00 |
0.00 |
0.00 |
10 |
Au |
89 |
89 |
3.33 |
0.00 |
0.28 |
0.00 |
11 |
Bg |
3484 |
3484 |
0.00 |
54.99 |
0.75 |
0.86 |
12 |
Bg |
1414 |
1414 |
0.00 |
18.98 |
0.75 |
0.86 |
13 |
Bg |
1037 |
1037 |
0.00 |
8.90 |
0.75 |
0.86 |
14 |
Bu |
3378 |
3378 |
1.37 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1668 |
1668 |
3.37 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1359 |
1359 |
37.97 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
783 |
783 |
25.54 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
188 |
188 |
4.47 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 13805.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13805.1 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 wB97X-D/STO-3G
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.484 |
0.609 |
0.000 |
C2 |
-0.484 |
-0.609 |
0.000 |
Br3 |
-0.484 |
2.281 |
0.000 |
Br4 |
0.484 |
-2.281 |
0.000 |
H5 |
1.130 |
0.574 |
0.892 |
H6 |
1.130 |
0.574 |
-0.892 |
H7 |
-1.130 |
-0.574 |
0.892 |
H8 |
-1.130 |
-0.574 |
-0.892 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5553 | 1.9312 | 2.8896 | 1.1028 | 1.1028 | 2.1911 | 2.1911 |
C2 | 1.5553 | | 2.8896 | 1.9312 | 2.1911 | 2.1911 | 1.1028 | 1.1028 | Br3 | 1.9312 | 2.8896 | | 4.6626 | 2.5129 | 2.5129 | 3.0599 | 3.0599 | Br4 | 2.8896 | 1.9312 | 4.6626 | | 3.0599 | 3.0599 | 2.5129 | 2.5129 | H5 | 1.1028 | 2.1911 | 2.5129 | 3.0599 | | 1.7849 | 2.5356 | 3.1008 | H6 | 1.1028 | 2.1911 | 2.5129 | 3.0599 | 1.7849 | | 3.1008 | 2.5356 | H7 | 2.1911 | 1.1028 | 3.0599 | 2.5129 | 2.5356 | 3.1008 | | 1.7849 | H8 | 2.1911 | 1.1028 | 3.0599 | 2.5129 | 3.1008 | 2.5356 | 1.7849 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
111.498 |
|
C1 |
C2 |
H7 |
109.863 |
C1 |
C2 |
H8 |
109.863 |
|
C2 |
C1 |
Br3 |
111.498 |
C2 |
C1 |
H5 |
109.863 |
|
C2 |
C1 |
H6 |
109.863 |
Br3 |
C1 |
H5 |
108.748 |
|
Br3 |
C1 |
H6 |
108.748 |
Br4 |
C2 |
H7 |
108.748 |
|
Br4 |
C2 |
H8 |
108.748 |
H5 |
C1 |
H6 |
108.044 |
|
H7 |
C2 |
H8 |
108.044 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.185 |
|
|
|
2 |
C |
-0.185 |
|
|
|
3 |
Br |
-0.014 |
|
|
|
4 |
Br |
-0.014 |
|
|
|
5 |
H |
0.100 |
|
|
|
6 |
H |
0.100 |
|
|
|
7 |
H |
0.100 |
|
|
|
8 |
H |
0.100 |
|
|
|
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 |
-44.697 |
1.668 |
0.000 |
y |
1.668 |
-51.439 |
0.000 |
z |
0.000 |
0.000 |
-44.797 |
|
Traceless |
| x | y | z |
x |
3.421 |
1.668 |
0.000 |
y |
1.668 |
-6.692 |
0.000 |
z |
0.000 |
0.000 |
3.271 |
|
Polar |
3z2-r2 | 6.543 |
x2-y2 | 6.742 |
xy | 1.668 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.557 |
-1.708 |
0.000 |
y |
-1.708 |
5.648 |
0.000 |
z |
0.000 |
0.000 |
1.710 |
<r2> (average value of r
2) Å
2
<r2> |
426.666 |
(<r2>)1/2 |
20.656 |
Jump to
S1C1
Energy calculated at wB97X-D/STO-3G
| hartrees |
Energy at 0K | -5169.846248 |
Energy at 298.15K | |
HF Energy | -5169.846248 |
Nuclear repulsion energy | 450.225520 |
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/STO-3G
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 |
3477 |
3477 |
0.00 |
53.72 |
0.74 |
0.85 |
2 |
A |
3367 |
3367 |
0.17 |
81.95 |
0.05 |
0.09 |
3 |
A |
1656 |
1656 |
0.15 |
7.62 |
0.74 |
0.85 |
4 |
A |
1464 |
1464 |
13.26 |
6.61 |
0.58 |
0.74 |
5 |
A |
1324 |
1324 |
0.02 |
17.06 |
0.75 |
0.86 |
6 |
A |
1117 |
1117 |
1.34 |
3.96 |
0.74 |
0.85 |
7 |
A |
1012 |
1012 |
4.23 |
5.74 |
0.58 |
0.73 |
8 |
A |
684 |
684 |
3.45 |
11.72 |
0.11 |
0.20 |
9 |
A |
221 |
221 |
0.66 |
1.04 |
0.48 |
0.65 |
10 |
A |
71 |
71 |
0.36 |
1.07 |
0.74 |
0.85 |
11 |
B |
3484 |
3484 |
0.31 |
19.12 |
0.75 |
0.86 |
12 |
B |
3364 |
3364 |
0.36 |
16.83 |
0.75 |
0.86 |
13 |
B |
1649 |
1649 |
3.86 |
22.01 |
0.75 |
0.86 |
14 |
B |
1445 |
1445 |
49.93 |
1.01 |
0.75 |
0.86 |
15 |
B |
1256 |
1256 |
0.50 |
6.96 |
0.75 |
0.86 |
16 |
B |
938 |
938 |
7.65 |
1.29 |
0.75 |
0.86 |
17 |
B |
731 |
731 |
4.24 |
8.50 |
0.75 |
0.86 |
18 |
B |
384 |
384 |
3.63 |
2.62 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13821.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13821.4 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/STO-3G
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.296 |
0.720 |
1.183 |
C2 |
-0.296 |
-0.720 |
1.183 |
Br3 |
-0.296 |
1.807 |
-0.297 |
Br4 |
0.296 |
-1.807 |
-0.297 |
H5 |
-0.010 |
1.214 |
2.122 |
H6 |
1.398 |
0.671 |
1.169 |
H7 |
0.010 |
-1.214 |
2.122 |
H8 |
-1.398 |
-0.671 |
1.169 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5574 | 1.9286 | 2.9284 | 1.1039 | 1.1030 | 2.1692 | 2.1916 |
C2 | 1.5574 | | 2.9284 | 1.9286 | 2.1692 | 2.1916 | 1.1039 | 1.1030 | Br3 | 1.9286 | 2.9284 | | 3.6617 | 2.5066 | 2.5112 | 3.8818 | 3.0826 | Br4 | 2.9284 | 1.9286 | 3.6617 | | 3.8818 | 3.0826 | 2.5066 | 2.5112 | H5 | 1.1039 | 2.1692 | 2.5066 | 3.8818 | | 1.7839 | 2.4282 | 2.5273 | H6 | 1.1030 | 2.1916 | 2.5112 | 3.0826 | 1.7839 | | 2.5273 | 3.1005 | H7 | 2.1692 | 1.1039 | 3.8818 | 2.5066 | 2.4282 | 2.5273 | | 1.7839 | H8 | 2.1916 | 1.1030 | 3.0826 | 2.5112 | 2.5273 | 3.1005 | 1.7839 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
113.872 |
|
C1 |
C2 |
H7 |
107.981 |
C1 |
C2 |
H8 |
109.750 |
|
C2 |
C1 |
Br3 |
113.872 |
C2 |
C1 |
H5 |
107.981 |
|
C2 |
C1 |
H6 |
109.750 |
Br3 |
C1 |
H5 |
108.411 |
|
Br3 |
C1 |
H6 |
108.787 |
Br4 |
C2 |
H7 |
108.411 |
|
Br4 |
C2 |
H8 |
108.787 |
H5 |
C1 |
H6 |
107.866 |
|
H7 |
C2 |
H8 |
107.866 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.186 |
|
|
|
2 |
C |
-0.186 |
|
|
|
3 |
Br |
-0.010 |
|
|
|
4 |
Br |
-0.010 |
|
|
|
5 |
H |
0.097 |
|
|
|
6 |
H |
0.099 |
|
|
|
7 |
H |
0.097 |
|
|
|
8 |
H |
0.099 |
|
|
|
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 |
2.183 |
2.183 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-44.760 |
0.899 |
0.000 |
y |
0.899 |
-48.689 |
0.000 |
z |
0.000 |
0.000 |
-42.406 |
|
Traceless |
| x | y | z |
x |
0.787 |
0.899 |
0.000 |
y |
0.899 |
-5.106 |
0.000 |
z |
0.000 |
0.000 |
4.319 |
|
Polar |
3z2-r2 | 8.638 |
x2-y2 | 3.929 |
xy | 0.899 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.018 |
-0.687 |
0.000 |
y |
-0.687 |
3.586 |
0.000 |
z |
0.000 |
0.000 |
3.829 |
<r2> (average value of r
2) Å
2
<r2> |
312.651 |
(<r2>)1/2 |
17.682 |