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'''Spitzer resistivity''' is a classical model of [[electrical resistivity]] that is based upon electron ion collisions:<ref name="trintchouk2003measurement">{{cite journal| author=Trintchouk, Fedor, Yamada, M, Ji, H, Kulsrud, RM, Carter, TA| title=Measurement of the transverse Spitzer resistivity during collisional magnetic reconnection| journal=Physics of Plasmas| year=2003| volume=10| pages=319| accessdate=11 August 2013}}</ref><ref name="davies2003electric">{{cite journal| author=Davies, JR| title=Electric and magnetic field generation and target heating by laser-generated fast electrons| journal=Physical Review E| year=2003| volume=68| number=5| pages=056404| publisher=APS| accessdate=11 August 2013}}</ref><br />
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<math>\eta =\dfrac {\pi Ze^{2}m^{1/2}\ln \Lambda } {\left( 4\pi \varepsilon_{0}\right) ^{2}\left( k_{B}T\right)^{3/2}}</math><br />
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where η is the Spitzer resistivity, Z is ionization of nuclei, m is the electron mass, ε is the resistivity of free space, lnΛ is the [[Coulomb logarithm]], k<sub>B</sub> is [[Boltzmann's constant]] and T is the temperature in kelvins.<br />
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This resistivity model was proposed by [[Lyman Spitzer]].<ref name="forest1994determination">{{cite journal| author=Forest, CB, Kupfer, K, Luce, TC, Politzer, PA, Lao, LL, Wade, MR, Whyte, DG, Wroblewski, D| title=Determination of the noninductive current profile in tokamak plasmas| journal=Physical review letters| year=1994| volume=73| number=18| pages=2444| publisher=APS| accessdate=11 August 2013}}</ref><br />
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Spitzer resistivity is commonly used in plasma physics.<ref name="davies2003electric"/><br />
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==References==<br />
{{reflist}}<br />
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==External links==<br />
*http://people.duke.edu/~ad159/files/p142/25.pdf<br />
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[[Category:Electronics]]</div>en>Malcolma