Radial Distribution Functions for the Hydrogen Atom
Radial Distribution Functions for the Hydrogen Atom
Radial Distribution Functions for the Hydrogen Atom
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Chemistry 362<br />
Spring 2013<br />
Dr. Jean M. Standard<br />
March 29, 2013<br />
<strong>Radial</strong> <strong>Distribution</strong> <strong>Functions</strong> <strong>for</strong> <strong>the</strong> <strong>Hydrogen</strong> <strong>Atom</strong><br />
The <strong>Radial</strong> <strong>Distribution</strong> Function (RDF) gives <strong>the</strong> probability density <strong>for</strong> finding <strong>the</strong> electron at a radius r from <strong>the</strong><br />
nucleus. The RDF is defined as<br />
RDF = r 2 [ R n ( r)<br />
] 2 .<br />
Plots of <strong>the</strong> <strong>Radial</strong> <strong>Distribution</strong> <strong>Functions</strong> <strong>for</strong> <strong>the</strong> 1s, 2s, and 3s orbitals of <strong>the</strong> hydrogen atom are shown in Figure<br />
1.<br />
€<br />
0.6<br />
0.5<br />
1s<br />
0.4<br />
RDF<br />
0.3<br />
0.2<br />
2s<br />
0.1<br />
3s<br />
0.0<br />
0 5 10 15 20 25<br />
r (a.u.)<br />
Figure 1. RDF plots <strong>for</strong> 1s, 2s, and 3s orbitals of <strong>the</strong> H atom.<br />
Note that as <strong>the</strong> principal quantum number increases, <strong>the</strong> maximum in <strong>the</strong> probability density occurs at larger<br />
distances <strong>for</strong> orbitals of <strong>the</strong> same angular momentum type. For example, <strong>the</strong> maximum probability <strong>for</strong> <strong>the</strong> 1s<br />
orbital occurs at 1 bohr (0.529 Å), <strong>for</strong> <strong>the</strong> 2s orbital <strong>the</strong> primary maximum occurs at 5.3 bohr, and <strong>for</strong> <strong>the</strong> 3s orbital<br />
<strong>the</strong> primary maximum occurs at about 13 bohr.<br />
Similar trends are observed as <strong>the</strong> principal quantum number increases <strong>for</strong> <strong>the</strong> higher angular momentum orbitals<br />
(e.g., p-type, d-type, or f-type orbitals). For example, plots of <strong>the</strong> <strong>Radial</strong> <strong>Distribution</strong> <strong>Functions</strong> <strong>for</strong> <strong>the</strong> 2p and 3p<br />
orbitals are shown in Figure 2.
2<br />
0.25<br />
0.20<br />
2p<br />
0.15<br />
RDF<br />
0.10<br />
3p<br />
0.05<br />
0.00<br />
0 5 10 15 20 25<br />
r (a.u.)<br />
Figure 2. RDF plots <strong>for</strong> 2p and 3p orbitals of <strong>the</strong> H atom.<br />
In contrast, if <strong>the</strong> principal quantum number is held fixed and <strong>the</strong> angular momentum type of <strong>the</strong> orbital is varied, we<br />
see from <strong>the</strong> example in Figure 3 that <strong>the</strong> position of <strong>the</strong> primary maximum in <strong>the</strong> probability distribution decreases<br />
as <strong>the</strong> angular momentum increases.<br />
0.15<br />
0.10<br />
3d<br />
3p<br />
3s<br />
RDF<br />
0.05<br />
0.00<br />
0 5 10 15 20 25<br />
r (a.u.)<br />
Figure 3. RDF plots <strong>for</strong> 3s, 3p, and 3d orbitals of <strong>the</strong> H atom.