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Coronas, plasma, and arcs

Particularly in mass spectrometry, where discharges are used to enhance or produce ions from sample materials, mostly coronas, plasmas, and arcs are used. The gas pressure is normally atmospheric, and the electrodes are arranged to give nonuniform electric fields. Usually, coronas and plasmas are struck between electrodes that are not of similar shapes, complicating any description of the discharge because the resulting electric-field gradients are not uniform between the electrodes. [Pg.38]

This chapter should be read in conjunction with Chapter 6, Coronas, Plasmas, and Arcs. A plasma is defined as a gaseous phase containing neutral molecules, ions, and electrons. The numbers of ions and electrons are usually almost equal. In a plasma torch, the plasma is normally formed in a monatomic gas such as argon flowing between two concentric quartz tubes (Figure 14.1). [Pg.87]


See other pages where Coronas, plasma, and arcs is mentioned: [Pg.29]    [Pg.31]    [Pg.33]    [Pg.35]    [Pg.37]    [Pg.39]    [Pg.41]    [Pg.43]    [Pg.44]    [Pg.122]    [Pg.123]    [Pg.129]    [Pg.151]    [Pg.387]    [Pg.32]    [Pg.34]    [Pg.36]    [Pg.38]    [Pg.40]    [Pg.42]    [Pg.44]    [Pg.46]    [Pg.47]    [Pg.123]    [Pg.129]    [Pg.151]    [Pg.387]   
See also in sourсe #XX -- [ Pg.14 , Pg.29 ]

See also in sourсe #XX -- [ Pg.29 , Pg.44 ]




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Corona

Corona plasma

Plasma Arcing

Plasma arc

Plasmas, and Arcs

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