Jump to
S1C2
Energy calculated at TPSSh/Def2TZVPP
| hartrees |
Energy at 0K | -5226.804718 |
Energy at 298.15K | |
HF Energy | -5226.804718 |
Nuclear repulsion energy | 416.447714 |
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 TPSSh/Def2TZVPP
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 |
3106 |
3106 |
0.00 |
163.50 |
0.03 |
0.07 |
2 |
Ag |
1496 |
1496 |
0.00 |
7.64 |
0.75 |
0.86 |
3 |
Ag |
1269 |
1269 |
0.00 |
40.07 |
0.42 |
0.59 |
4 |
Ag |
1065 |
1065 |
0.00 |
12.42 |
0.71 |
0.83 |
5 |
Ag |
648 |
648 |
0.00 |
109.72 |
0.28 |
0.44 |
6 |
Ag |
185 |
185 |
0.00 |
4.55 |
0.28 |
0.44 |
7 |
Au |
3190 |
3190 |
0.37 |
0.00 |
0.00 |
0.00 |
8 |
Au |
1090 |
1090 |
2.87 |
0.00 |
0.00 |
0.00 |
9 |
Au |
751 |
751 |
3.24 |
0.00 |
0.00 |
0.00 |
10 |
Au |
99 |
99 |
4.60 |
0.00 |
0.00 |
0.00 |
11 |
Bg |
3167 |
3167 |
0.00 |
77.86 |
0.75 |
0.86 |
12 |
Bg |
1285 |
1285 |
0.00 |
2.33 |
0.75 |
0.86 |
13 |
Bg |
937 |
937 |
0.00 |
2.24 |
0.75 |
0.86 |
14 |
Bu |
3114 |
3114 |
5.48 |
0.00 |
0.00 |
0.00 |
15 |
Bu |
1492 |
1492 |
6.23 |
0.00 |
0.00 |
0.00 |
16 |
Bu |
1199 |
1199 |
56.31 |
0.00 |
0.00 |
0.00 |
17 |
Bu |
584 |
584 |
81.07 |
0.00 |
0.00 |
0.00 |
18 |
Bu |
169 |
169 |
7.93 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 12422.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12422.4 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 TPSSh/Def2TZVPP
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.496 |
0.565 |
0.000 |
C2 |
-0.496 |
-0.565 |
0.000 |
Br3 |
-0.496 |
2.267 |
0.000 |
Br4 |
0.496 |
-2.267 |
0.000 |
H5 |
1.114 |
0.578 |
0.892 |
H6 |
1.114 |
0.578 |
-0.892 |
H7 |
-1.114 |
-0.578 |
0.892 |
H8 |
-1.114 |
-0.578 |
-0.892 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5049 | 1.9703 | 2.8328 | 1.0855 | 1.0855 | 2.1677 | 2.1677 |
C2 | 1.5049 | | 2.8328 | 1.9703 | 2.1677 | 2.1677 | 1.0855 | 1.0855 | Br3 | 1.9703 | 2.8328 | | 4.6421 | 2.4989 | 2.4989 | 3.0455 | 3.0455 | Br4 | 2.8328 | 1.9703 | 4.6421 | | 3.0455 | 3.0455 | 2.4989 | 2.4989 | H5 | 1.0855 | 2.1677 | 2.4989 | 3.0455 | | 1.7847 | 2.5109 | 3.0805 | H6 | 1.0855 | 2.1677 | 2.4989 | 3.0455 | 1.7847 | | 3.0805 | 2.5109 | H7 | 2.1677 | 1.0855 | 3.0455 | 2.4989 | 2.5109 | 3.0805 | | 1.7847 | H8 | 2.1677 | 1.0855 | 3.0455 | 2.4989 | 3.0805 | 2.5109 | 1.7847 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
108.461 |
|
C1 |
C2 |
H7 |
112.602 |
C1 |
C2 |
H8 |
112.602 |
|
C2 |
C1 |
Br3 |
108.461 |
C2 |
C1 |
H5 |
112.602 |
|
C2 |
C1 |
H6 |
112.602 |
Br3 |
C1 |
H5 |
106.071 |
|
Br3 |
C1 |
H6 |
106.071 |
Br4 |
C2 |
H7 |
106.071 |
|
Br4 |
C2 |
H8 |
106.071 |
H5 |
C1 |
H6 |
110.581 |
|
H7 |
C2 |
H8 |
110.581 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.063 |
|
|
|
2 |
C |
-0.063 |
|
|
|
3 |
Br |
-0.163 |
|
|
|
4 |
Br |
-0.163 |
|
|
|
5 |
H |
0.113 |
|
|
|
6 |
H |
0.113 |
|
|
|
7 |
H |
0.113 |
|
|
|
8 |
H |
0.113 |
|
|
|
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
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
8.267 |
-1.930 |
0.000 |
y |
-1.930 |
14.364 |
0.000 |
z |
0.000 |
0.000 |
7.214 |
<r2> (average value of r
2) Å
2
<r2> |
425.488 |
(<r2>)1/2 |
20.627 |
Jump to
S1C1
Energy calculated at TPSSh/Def2TZVPP
| hartrees |
Energy at 0K | -5226.800714 |
Energy at 298.15K | |
HF Energy | -5226.800714 |
Nuclear repulsion energy | 450.819023 |
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 TPSSh/Def2TZVPP
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 |
3145 |
3145 |
0.01 |
88.91 |
0.75 |
0.85 |
2 |
A |
3083 |
3083 |
15.98 |
262.79 |
0.02 |
0.04 |
3 |
A |
1472 |
1472 |
0.34 |
3.34 |
0.75 |
0.86 |
4 |
A |
1303 |
1303 |
19.51 |
2.98 |
0.40 |
0.57 |
5 |
A |
1180 |
1180 |
1.71 |
7.91 |
0.73 |
0.84 |
6 |
A |
1028 |
1028 |
1.07 |
1.77 |
0.66 |
0.79 |
7 |
A |
902 |
902 |
7.35 |
4.88 |
0.29 |
0.45 |
8 |
A |
554 |
554 |
8.48 |
18.70 |
0.06 |
0.12 |
9 |
A |
220 |
220 |
1.23 |
1.45 |
0.36 |
0.53 |
10 |
A |
74 |
74 |
0.24 |
0.99 |
0.68 |
0.81 |
11 |
B |
3159 |
3159 |
1.41 |
26.65 |
0.75 |
0.86 |
12 |
B |
3075 |
3075 |
1.89 |
49.37 |
0.75 |
0.86 |
13 |
B |
1468 |
1468 |
9.94 |
10.60 |
0.75 |
0.86 |
14 |
B |
1270 |
1270 |
68.96 |
3.14 |
0.75 |
0.86 |
15 |
B |
1115 |
1115 |
1.68 |
2.35 |
0.75 |
0.86 |
16 |
B |
842 |
842 |
18.30 |
1.11 |
0.75 |
0.86 |
17 |
B |
585 |
585 |
16.32 |
9.41 |
0.75 |
0.86 |
18 |
B |
347 |
347 |
6.73 |
2.17 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12410.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 12410.6 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 TPSSh/Def2TZVPP
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.312 |
0.686 |
1.186 |
C2 |
-0.312 |
-0.686 |
1.186 |
Br3 |
-0.312 |
1.802 |
-0.295 |
Br4 |
0.312 |
-1.802 |
-0.295 |
H5 |
0.025 |
1.220 |
2.092 |
H6 |
1.394 |
0.649 |
1.104 |
H7 |
-0.025 |
-1.220 |
2.092 |
H8 |
-1.394 |
-0.649 |
1.104 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5077 | 1.9563 | 2.8963 | 1.0896 | 1.0863 | 2.1377 | 2.1675 |
C2 | 1.5077 | | 2.8963 | 1.9563 | 2.1377 | 2.1675 | 1.0896 | 1.0863 | Br3 | 1.9563 | 2.8963 | | 3.6583 | 2.4795 | 2.4891 | 3.8621 | 3.0224 | Br4 | 2.8963 | 1.9563 | 3.6583 | | 3.8621 | 3.0224 | 2.4795 | 2.4891 | H5 | 1.0896 | 2.1377 | 2.4795 | 3.8621 | | 1.7826 | 2.4414 | 2.5462 | H6 | 1.0863 | 2.1675 | 2.4891 | 3.0224 | 1.7826 | | 2.5462 | 3.0750 | H7 | 2.1377 | 1.0896 | 3.8621 | 2.4795 | 2.4414 | 2.5462 | | 1.7826 | H8 | 2.1675 | 1.0863 | 3.0224 | 2.4891 | 2.5462 | 3.0750 | 1.7826 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
Br4 |
112.821 |
|
C1 |
C2 |
H7 |
109.729 |
C1 |
C2 |
H8 |
112.334 |
|
C2 |
C1 |
Br3 |
112.821 |
C2 |
C1 |
H5 |
109.729 |
|
C2 |
C1 |
H6 |
112.334 |
Br3 |
C1 |
H5 |
105.418 |
|
Br3 |
C1 |
H6 |
106.240 |
Br4 |
C2 |
H7 |
105.418 |
|
Br4 |
C2 |
H8 |
106.240 |
H5 |
C1 |
H6 |
110.025 |
|
H7 |
C2 |
H8 |
110.025 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.052 |
|
|
|
2 |
C |
-0.052 |
|
|
|
3 |
Br |
-0.146 |
|
|
|
4 |
Br |
-0.146 |
|
|
|
5 |
H |
0.096 |
|
|
|
6 |
H |
0.102 |
|
|
|
7 |
H |
0.096 |
|
|
|
8 |
H |
0.102 |
|
|
|
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 |
2.674 |
2.674 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.591 |
-0.747 |
0.000 |
y |
-0.747 |
11.058 |
0.000 |
z |
0.000 |
0.000 |
9.515 |
<r2> (average value of r
2) Å
2
<r2> |
313.696 |
(<r2>)1/2 |
17.711 |