{"title":"Deposition of aerosol flowing past a cylindrical fiber in a uniform electric field","authors":"G Zebel","doi":"10.1016/0095-8522(65)90033-4","DOIUrl":null,"url":null,"abstract":"<div><p>The deposition of aerosol particles from an air stream of velocity <em>V</em><sub>0</sub> upon a circular cylindrical fiber perpendicular to the stream in a homogeneous electrical field <em>E</em><sub>0</sub>, has been investigated theoretically. The dielectric constant <em>ϵ</em><sub><em>c</em></sub> of the fiber controls by means of the parameter <span><math><mtext>a = </mtext><mtext>(ϵ</mtext><msub><mi></mi><mn>c</mn></msub><mtext> − 1)</mtext><mtext>(ϵ</mtext><msub><mi></mi><mn>c</mn></msub><mtext> + 1)</mtext></math></span> the additive inhomogeneous field of the fiber, which effectuates the deposition of the particles. When computing the trajectories, both inertia and image forces for charged particles have been neglected. The computations have been made for frictionless potential flow and for viscous flow according to Lamb.</p><p>For uncharged particles, the dimensionless parameter <em>F</em> ∼ <em>r</em><sub>8</sub><sup>3</sup><em>E</em><sub>0</sub><sup>2</sup><em>B</em>/<em>r</em><sub><em>c</em></sub><em>V</em><sub>0</sub> (where <em>r</em><sub><em>s</em></sub>, <em>B</em> = radius and mobility of the particle; <em>r</em><sub><em>c</em></sub> = radius of the fiber) determines the value of the deposition coefficient. Exact solutions for the limiting case <em>a</em> = 0 as well as some approximate solutions for <em>a</em> ≠ 0, obtained by the Runge-Kutta method, are given.</p><p>For particles carrying an electrical charge <em>q</em>, the dimensionless parameter <em>G</em> = <em>E</em><sub>0</sub><em>qB</em>/<em>V</em><sub>0</sub> is decisive. From the exact solutions the deposition coefficient is given by <span><math><mtext>ζ = </mtext><mtext>G(a + 1)</mtext><mtext>(G + 1)</mtext><mtext>, </mtext><mtext>if</mtext><mtext> G > 0</mtext></math></span>, for ideal and viscous flow. With negative <em>G</em>, the fiber may be surrounded by a “dust-free space.”</p></div>","PeriodicalId":15437,"journal":{"name":"Journal of Colloid Science","volume":"20 6","pages":"Pages 522-543"},"PeriodicalIF":0.0000,"publicationDate":"1965-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0095-8522(65)90033-4","citationCount":"102","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Colloid Science","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0095852265900334","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 102
Abstract
The deposition of aerosol particles from an air stream of velocity V0 upon a circular cylindrical fiber perpendicular to the stream in a homogeneous electrical field E0, has been investigated theoretically. The dielectric constant ϵc of the fiber controls by means of the parameter the additive inhomogeneous field of the fiber, which effectuates the deposition of the particles. When computing the trajectories, both inertia and image forces for charged particles have been neglected. The computations have been made for frictionless potential flow and for viscous flow according to Lamb.
For uncharged particles, the dimensionless parameter F ∼ r83E02B/rcV0 (where rs, B = radius and mobility of the particle; rc = radius of the fiber) determines the value of the deposition coefficient. Exact solutions for the limiting case a = 0 as well as some approximate solutions for a ≠ 0, obtained by the Runge-Kutta method, are given.
For particles carrying an electrical charge q, the dimensionless parameter G = E0qB/V0 is decisive. From the exact solutions the deposition coefficient is given by , for ideal and viscous flow. With negative G, the fiber may be surrounded by a “dust-free space.”