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The application of the generalized Bohm criterion to Emmert’s solution of the warm ion collisionless plasma equation
Emmert e t a l. [Phys. Fluids 2 3, 803 (1980)] have modeled the flow of a one‐dimensional collisionless plasma to a material wall by formulating and solving the warm‐ion plasma equation. In contrast to the result of the cold‐ion plasma equation it was found that the electric field at the plasma–shea...
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Published in: | The Physics of fluids (1958) 1987-07, Vol.30 (7), p.2264-2265 |
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container_end_page | 2265 |
container_issue | 7 |
container_start_page | 2264 |
container_title | The Physics of fluids (1958) |
container_volume | 30 |
creator | Bissell, R. C. |
description | Emmert e
t
a
l. [Phys. Fluids 2
3, 803 (1980)] have modeled the flow of a one‐dimensional collisionless plasma to a material wall by formulating and solving the warm‐ion plasma equation. In contrast to the result of the cold‐ion plasma equation it was found that the electric field at the plasma–sheath boundary was finite. It is first shown that Emmert’s solution satisfies the generalized Bohm criterion, and is thus a valid solution, before discussing the cause of the difference in the results of the two models in calculating the boundary electric field. |
doi_str_mv | 10.1063/1.866160 |
format | article |
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a
l. [Phys. Fluids 2
3, 803 (1980)] have modeled the flow of a one‐dimensional collisionless plasma to a material wall by formulating and solving the warm‐ion plasma equation. In contrast to the result of the cold‐ion plasma equation it was found that the electric field at the plasma–sheath boundary was finite. It is first shown that Emmert’s solution satisfies the generalized Bohm criterion, and is thus a valid solution, before discussing the cause of the difference in the results of the two models in calculating the boundary electric field.</description><subject>Exact sciences and technology</subject><subject>Physics</subject><subject>Physics of gases, plasmas and electric discharges</subject><subject>Physics of plasmas and electric discharges</subject><subject>Plasma dynamics and flow</subject><issn>0031-9171</issn><issn>2163-4998</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1987</creationdate><recordtype>article</recordtype><recordid>eNp1kE1OwzAQhS0EEqUgcQQvWMAiZWynTryEqvxIldiUdTRxHGrkNMFOQXTFNbgeJyFpEGLDamaevnmjeYScMpgwkOKSTVIpmYQ9MuJMiihWKt0nIwDBIsUSdkiOQngG4DGLxYi8LleGYtM4q7G19ZrWJW076cmsjUdnt6ag1_Wqotrb1vieaGs6ryrj26-Pz0BD7TZ_F9_QV7Sfde2cDV3nTAi0cRgqpOZlsztzTA5KdMGc_NQxebyZL2d30eLh9n52tYg0lxwiXQADAzCVSmrFNJpiKiDvxVxCnDKZKGUwjpOiSLlMDWjkCaYiV6XIdSnG5Hzw1b4OwZsya7yt0L9nDLI-r4xlQ14dejagDQaNrvS41jb88kks-FSIDrsYsKBtu_vlf8tvljN5eA</recordid><startdate>198707</startdate><enddate>198707</enddate><creator>Bissell, R. C.</creator><general>American Institute of Physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>198707</creationdate><title>The application of the generalized Bohm criterion to Emmert’s solution of the warm ion collisionless plasma equation</title><author>Bissell, R. C.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2620-cd010e005696c91caed530b010eb604816799ea447dd8268e0ca27a83b9f3bcf3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1987</creationdate><topic>Exact sciences and technology</topic><topic>Physics</topic><topic>Physics of gases, plasmas and electric discharges</topic><topic>Physics of plasmas and electric discharges</topic><topic>Plasma dynamics and flow</topic><toplevel>online_resources</toplevel><creatorcontrib>Bissell, R. C.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>The Physics of fluids (1958)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bissell, R. C.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The application of the generalized Bohm criterion to Emmert’s solution of the warm ion collisionless plasma equation</atitle><jtitle>The Physics of fluids (1958)</jtitle><date>1987-07</date><risdate>1987</risdate><volume>30</volume><issue>7</issue><spage>2264</spage><epage>2265</epage><pages>2264-2265</pages><issn>0031-9171</issn><eissn>2163-4998</eissn><coden>PFLDAS</coden><abstract>Emmert e
t
a
l. [Phys. Fluids 2
3, 803 (1980)] have modeled the flow of a one‐dimensional collisionless plasma to a material wall by formulating and solving the warm‐ion plasma equation. In contrast to the result of the cold‐ion plasma equation it was found that the electric field at the plasma–sheath boundary was finite. It is first shown that Emmert’s solution satisfies the generalized Bohm criterion, and is thus a valid solution, before discussing the cause of the difference in the results of the two models in calculating the boundary electric field.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.866160</doi><tpages>2</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Exact sciences and technology Physics Physics of gases, plasmas and electric discharges Physics of plasmas and electric discharges Plasma dynamics and flow |
title | The application of the generalized Bohm criterion to Emmert’s solution of the warm ion collisionless plasma equation |
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