Jump to
S2C1
Energy calculated at B2PLYP/6-311G*
| hartrees |
Energy at 0K | -5185.326992 |
Energy at 298.15K | -5185.331984 |
HF Energy | -5185.197921 |
Nuclear repulsion energy | 323.674466 |
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 B2PLYP/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
1.000 |
Br2 |
0.000 |
1.566 |
-0.086 |
Br3 |
0.000 |
-1.566 |
-0.086 |
Atom - Atom Distances (Å)
|
C1 |
Br2 |
Br3 |
C1 | | 1.9053 | 1.9053 |
Br2 | 1.9053 | | 3.1312 | Br3 | 1.9053 | 3.1312 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Br2 |
C1 |
Br3 |
110.508 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.195 |
|
|
|
2 |
Br |
0.097 |
|
|
|
3 |
Br |
0.097 |
|
|
|
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 |
-1.253 |
1.253 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-41.489 |
0.000 |
0.000 |
y |
0.000 |
-39.917 |
0.000 |
z |
0.000 |
0.000 |
-45.164 |
|
Traceless |
| x | y | z |
x |
1.051 |
0.000 |
0.000 |
y |
0.000 |
3.409 |
0.000 |
z |
0.000 |
0.000 |
-4.461 |
|
Polar |
3z2-r2 | -8.921 |
x2-y2 | -1.572 |
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 |
3.317 |
0.000 |
0.000 |
y |
0.000 |
11.551 |
0.000 |
z |
0.000 |
0.000 |
5.168 |
<r2> (average value of r
2) Å
2
<r2> |
204.445 |
(<r2>)1/2 |
14.298 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G*
| hartrees |
Energy at 0K | -5185.306032 |
Energy at 298.15K | -5185.311058 |
HF Energy | -5185.190936 |
Nuclear repulsion energy | 314.843517 |
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 B2PLYP/6-311G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.722 |
Br2 |
0.000 |
1.668 |
-0.062 |
Br3 |
0.000 |
-1.668 |
-0.062 |
Atom - Atom Distances (Å)
|
C1 |
Br2 |
Br3 |
C1 | | 1.8434 | 1.8434 |
Br2 | 1.8434 | | 3.3367 | Br3 | 1.8434 | 3.3367 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.242 |
|
|
|
2 |
Br |
0.121 |
|
|
|
3 |
Br |
0.121 |
|
|
|
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 |
-0.591 |
0.591 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-43.066 |
0.000 |
0.000 |
y |
0.000 |
-38.587 |
0.000 |
z |
0.000 |
0.000 |
-42.411 |
|
Traceless |
| x | y | z |
x |
-2.567 |
0.000 |
0.000 |
y |
0.000 |
4.152 |
0.000 |
z |
0.000 |
0.000 |
-1.585 |
|
Polar |
3z2-r2 | -3.170 |
x2-y2 | -4.480 |
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 |
3.210 |
0.000 |
0.000 |
y |
0.000 |
10.570 |
0.000 |
z |
0.000 |
0.000 |
4.251 |
<r2> (average value of r
2) Å
2
<r2> |
224.069 |
(<r2>)1/2 |
14.969 |