Suppose we have an infinite line of charge such that the linear charge distri- bution is given by -a² /a² X(x) : a where a is a constant with dimension of length. We can determine the electrostatic...


Suppose we have an infinite line of charge such that the linear charge distri-<br>bution is given by<br>-a² /a²<br>X(x) :<br>a<br>where a is a constant with dimension of length. We can determine the electrostatic potential<br>some perpendicular distance z above the line to be (in SI units)<br>20<br>V(2) =<br>e-a²/a?<br>xp:<br>V1+ x²/z²<br>4T€oaz<br>and of course we would like to evaluate the integral.<br>(a) (paper) Make the change of variables x = aq, so that you get<br>e-q?<br>2Q<br>V (2) =<br>roo<br>(1)<br>V1 +a²q² /zzdq<br>and then with y = z/(v2a), show that this can be written as<br>Q<br>V(z) =<br>-e²Ko(y²),<br>4περα<br>where Ko is a modifed Bessel function. Do this by looking up integral forms of the Bessel<br>function and compare them to Eq. (1).<br>

Extracted text: Suppose we have an infinite line of charge such that the linear charge distri- bution is given by -a² /a² X(x) : a where a is a constant with dimension of length. We can determine the electrostatic potential some perpendicular distance z above the line to be (in SI units) 20 V(2) = e-a²/a? xp: V1+ x²/z² 4T€oaz and of course we would like to evaluate the integral. (a) (paper) Make the change of variables x = aq, so that you get e-q? 2Q V (2) = roo (1) V1 +a²q² /zzdq and then with y = z/(v2a), show that this can be written as Q V(z) = -e²Ko(y²), 4περα where Ko is a modifed Bessel function. Do this by looking up integral forms of the Bessel function and compare them to Eq. (1).

Jun 05, 2022
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