Jump to
S2C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -51.216944 |
| Energy at 298.15K | -51.219612 |
| HF Energy | -51.216944 |
| Nuclear repulsion energy | 15.597540 |
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/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.026 |
1.646 |
0.000 |
| Br2 |
0.026 |
-0.336 |
0.000 |
| H3 |
-1.047 |
1.892 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
| C1 | | 1.9817 | 1.1009 |
Br2 | 1.9817 | | 2.4729 | H3 | 1.1009 | 2.4729 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Br2 |
C1 |
H3 |
102.929 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.123 |
|
|
|
| 2 |
Br |
-0.046 |
|
|
|
| 3 |
H |
0.169 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.030 |
0.678 |
0.000 |
2.140 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.727 |
-4.117 |
0.000 |
| y |
-4.117 |
-22.400 |
0.000 |
| z |
0.000 |
0.000 |
-21.203 |
|
| Traceless |
| | x | y | z |
| x |
-0.925 |
-4.117 |
0.000 |
| y |
-4.117 |
-0.435 |
0.000 |
| z |
0.000 |
0.000 |
1.361 |
|
| Polar |
| 3z2-r2 | 2.721 |
| x2-y2 | -0.327 |
| xy | -4.117 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.562 |
-0.355 |
0.000 |
| y |
-0.355 |
6.397 |
0.000 |
| z |
0.000 |
0.000 |
1.415 |
<r2> (average value of r
2) Å
2
| <r2> |
35.532 |
| (<r2>)1/2 |
5.961 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -51.254853 |
| Energy at 298.15K | -51.257545 |
| HF Energy | -51.254853 |
| Nuclear repulsion energy | 15.953832 |
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/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.021 |
1.578 |
0.000 |
| Br2 |
0.021 |
-0.334 |
0.000 |
| H3 |
-0.843 |
2.217 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
Br2 |
H3 |
| C1 | | 1.9122 | 1.0743 |
Br2 | 1.9122 | | 2.6930 | H3 | 1.0743 | 2.6930 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.224 |
|
|
|
| 2 |
Br |
0.002 |
|
|
|
| 3 |
H |
0.223 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.743 |
1.229 |
0.000 |
1.436 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.553 |
-1.753 |
0.000 |
| y |
-1.753 |
-18.631 |
0.000 |
| z |
0.000 |
0.000 |
-22.688 |
|
| Traceless |
| | x | y | z |
| x |
-0.893 |
-1.753 |
0.000 |
| y |
-1.753 |
3.489 |
0.000 |
| z |
0.000 |
0.000 |
-2.596 |
|
| Polar |
| 3z2-r2 | -5.193 |
| x2-y2 | -2.921 |
| xy | -1.753 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.225 |
-0.199 |
0.000 |
| y |
-0.199 |
5.245 |
0.000 |
| z |
0.000 |
0.000 |
0.805 |
<r2> (average value of r
2) Å
2
| <r2> |
34.447 |
| (<r2>)1/2 |
5.869 |