Jump to
S2C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -2610.695719 |
| Energy at 298.15K | -2610.698454 |
| HF Energy | -2610.695719 |
| Nuclear repulsion energy | 70.146214 |
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 HF/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.025 |
1.554 |
0.000 |
| Br2 |
0.025 |
-0.317 |
0.000 |
| H3 |
-1.042 |
1.788 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
| C1 | | 1.8710 | 1.0931 |
Br2 | 1.8710 | | 2.3604 | H3 | 1.0931 | 2.3604 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
102.369 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.114 |
|
|
|
| 2 |
Br |
-0.018 |
|
|
|
| 3 |
H |
0.132 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.654 |
-0.117 |
0.000 |
1.658 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.640 |
-3.506 |
0.000 |
| y |
-3.506 |
-25.442 |
0.000 |
| z |
0.000 |
0.000 |
-24.083 |
|
| Traceless |
| | x | y | z |
| x |
-0.877 |
-3.506 |
0.000 |
| y |
-3.506 |
-0.581 |
0.000 |
| z |
0.000 |
0.000 |
1.458 |
|
| Polar |
| 3z2-r2 | 2.917 |
| x2-y2 | -0.197 |
| xy | -3.506 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.690 |
-0.307 |
0.000 |
| y |
-0.307 |
5.860 |
0.000 |
| z |
0.000 |
0.000 |
2.405 |
<r2> (average value of r
2) Å
2
| <r2> |
37.966 |
| (<r2>)1/2 |
6.162 |
Jump to
S1C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -2610.724036 |
| Energy at 298.15K | -2610.726769 |
| HF Energy | -2610.724036 |
| Nuclear repulsion energy | 70.397609 |
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 HF/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.021 |
1.519 |
0.000 |
| Br2 |
0.021 |
-0.322 |
0.000 |
| H3 |
-0.845 |
2.153 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
| C1 | | 1.8405 | 1.0736 |
Br2 | 1.8405 | | 2.6223 | H3 | 1.0736 | 2.6223 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.169 |
|
|
|
| 2 |
Br |
0.005 |
|
|
|
| 3 |
H |
0.164 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.669 |
0.836 |
0.000 |
1.070 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.601 |
-1.561 |
0.000 |
| y |
-1.561 |
-21.506 |
0.000 |
| z |
0.000 |
0.000 |
-25.704 |
|
| Traceless |
| | x | y | z |
| x |
-0.996 |
-1.561 |
0.000 |
| y |
-1.561 |
3.646 |
0.000 |
| z |
0.000 |
0.000 |
-2.650 |
|
| Polar |
| 3z2-r2 | -5.300 |
| x2-y2 | -3.095 |
| xy | -1.561 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.369 |
-0.218 |
0.000 |
| y |
-0.218 |
5.155 |
0.000 |
| z |
0.000 |
0.000 |
2.081 |
<r2> (average value of r
2) Å
2
| <r2> |
37.784 |
| (<r2>)1/2 |
6.147 |