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Thermal ionization

In thermal ionization, also referred to as surface ionization, chemically-purified material loaded onto a filament which is then heated to cause some of the material to be ionized as it boils off the hot filament. Filaments are generally flat pieces of metal around 1-2mm wide, 0.1mm thick, bent into an upside-down U shape and welded to steel posts that supply a current.


Saha-Langmuir equation

The likelihood of ionisation is a function of the filament temperature, the work function of the filament substrate and the ionization energy of the element.

This is summarised in the Saha-Langmuir equation:[1]

\frac{Y_1}{Y_0}  =  \frac{g_1}{g_0} \exp \Bigg(\frac{\phi-IP}{kT}\Bigg)
\frac{Y_1}{Y_0} = ion to neutral ratio
\frac{g_1}{g_0} = statistical weights of ion and neutral states
φ = surface work function
IP = element ionization potential
k = Boltzmann's constant
T = surface temperature

Thermal ionization mass spectrometry

One application of thermal ionization is thermal ionization mass spectrometry (TIMS). The ions being produced at the filament are directed into a mass spectrometer to analyze the elements or isotopes present in the sample.[2]

See also


  1. ^ Dresser, M. J. (January 1968). "The Saha-Langmuir Equation and its Application" (PDF). Journal of Applied Physics 39 (1): 338-339. doi:10.1063/1.1655755 . Retrieved on 2007-10-11.
  2. ^ Aggarwal SK, Kinter M, Fitzgerald RL, Herold DA (1994). "Mass spectrometry of trace elements in biological samples". Critical reviews in clinical laboratory sciences 31 (1): 35–87. PMID 8049033.
This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Thermal_ionization". A list of authors is available in Wikipedia.
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