Jump to
S2C1
Energy calculated at HSEh1PBE/6-311G*
| hartrees |
Energy at 0K | -5185.549106 |
Energy at 298.15K | -5185.554126 |
HF Energy | -5185.549106 |
Nuclear repulsion energy | 325.966296 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at HSEh1PBE/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.995 |
Br2 |
0.000 |
1.554 |
-0.085 |
Br3 |
0.000 |
-1.554 |
-0.085 |
Atom - Atom Distances (Å)
|
C1 |
Br2 |
Br3 |
C1 | | 1.8929 | 1.8929 |
Br2 | 1.8929 | | 3.1083 | Br3 | 1.8929 | 3.1083 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
Br3 |
110.384 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.213 |
|
|
|
2 |
Br |
0.106 |
|
|
|
3 |
Br |
0.106 |
|
|
|
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 |
-1.274 |
1.274 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-41.272 |
0.000 |
0.000 |
y |
0.000 |
-39.599 |
0.000 |
z |
0.000 |
0.000 |
-44.928 |
|
Traceless |
| x | y | z |
x |
0.992 |
0.000 |
0.000 |
y |
0.000 |
3.501 |
0.000 |
z |
0.000 |
0.000 |
-4.493 |
|
Polar |
3z2-r2 | -8.985 |
x2-y2 | -1.673 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.359 |
0.000 |
0.000 |
y |
0.000 |
11.266 |
0.000 |
z |
0.000 |
0.000 |
5.193 |
<r2> (average value of r
2) Å
2
<r2> |
201.724 |
(<r2>)1/2 |
14.203 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| hartrees |
Energy at 0K | -5185.533358 |
Energy at 298.15K | -5185.538398 |
HF Energy | -5185.533358 |
Nuclear repulsion energy | 316.676660 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at HSEh1PBE/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.715 |
Br2 |
0.000 |
1.659 |
-0.061 |
Br3 |
0.000 |
-1.659 |
-0.061 |
Atom - Atom Distances (Å)
|
C1 |
Br2 |
Br3 |
C1 | | 1.8318 | 1.8318 |
Br2 | 1.8318 | | 3.3185 | Br3 | 1.8318 | 3.3185 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.255 |
|
|
|
2 |
Br |
0.127 |
|
|
|
3 |
Br |
0.127 |
|
|
|
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 |
-0.593 |
0.593 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-42.848 |
0.000 |
0.000 |
y |
0.000 |
-38.258 |
0.000 |
z |
0.000 |
0.000 |
-42.197 |
|
Traceless |
| x | y | z |
x |
-2.620 |
0.000 |
0.000 |
y |
0.000 |
4.265 |
0.000 |
z |
0.000 |
0.000 |
-1.645 |
|
Polar |
3z2-r2 | -3.289 |
x2-y2 | -4.590 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.262 |
0.000 |
0.000 |
y |
0.000 |
10.497 |
0.000 |
z |
0.000 |
0.000 |
4.285 |
<r2> (average value of r
2) Å
2
<r2> |
221.716 |
(<r2>)1/2 |
14.890 |