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Atomic Orbitals

Light has wave properties, which we characterize by frequency and wavelength, and particle properties as shown by the the photoelectric effect.

In 1923 a French physicist Louis de Broglie  postulated, by analogy with light, that matter must have both particle and wave properties.  De Broglie proposed that a particle with a mass m moving at a speed u will have a wavelength given by

= h / m · u

The mathematical description of atomic structure based on the wave properties of subatomic particles is called quantum mechanics.  A model of the hydrogen atom based on the wave nature of the electron was developed principally by the Austrian physicist Erwin Schrodinger.  Mathematical equations describing the nature of electron waves in atoms that give acceptable (acceptable here means physically reasonable) solutions to the Schrodinger equation are known as wave functions.  In order to obtain one of these wave functions, we must assign integral values known as quantum numbers to three quantities in the wave equation, similar to the integral value of n required in the Bohr equation for the hydrogen atom.

A given set of these three quantum numbers yields a wave function for an electron called an atomic orbital.  Although they are only mathematical expressions, atomic orbitals allow us to visualize a three-dimensional region in an atom in which there is a high probability of finding electrons.  A fourth quantum number refers to a magnetic property of electrons called spin.  A description of the quantum numbers follows

 

Letter s p d f...
l 0 1 2 3...

 

 

The quantum numbers n, l and ml arise from Schrodinger's treatment of the electron in a hydrogen atom as a matter wave; by analogy, this concept can be applied to electrons in other atoms as well.  Although these three quantum numbers are sufficient to fully characterize the orbitals in an atom, there is a need for a fourth quantum number to describe the electrons that occupy these orbitals.  







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