{"title":"利用流体代码 LINDA-NU 对线性等离子体装置中的分离氢等离子体进行多流体建模的初步结果","authors":"Kento Sugiura, Taichi Ido, Hirohiko Tanaka, Hiroki Natsume, Shota Masuda, Kazuo Hoshino, Keiji Sawada, Noriyasu Ohno","doi":"10.1002/ctpp.202300150","DOIUrl":null,"url":null,"abstract":"<p>In order to simulate hydrogen (H) plasma in the linear plasma device NAGDIS-II, we have modified the fluid code LINDA-NU to allow the simultaneous calculation of multiple ion species consisting of hydrogen atomic ions (<span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mi>H</mi>\n <mo>+</mo>\n </msup>\n </mrow>\n <annotation>$$ {\\mathrm{H}}^{+} $$</annotation>\n </semantics></math>) and molecular ions (<span></span><math>\n <semantics>\n <mrow>\n <msubsup>\n <mi>H</mi>\n <mn>2</mn>\n <mo>+</mo>\n </msubsup>\n <mo>,</mo>\n <msubsup>\n <mi>H</mi>\n <mn>3</mn>\n <mo>+</mo>\n </msubsup>\n </mrow>\n <annotation>$$ {\\mathrm{H}}_2^{+},{\\mathrm{H}}_3^{+} $$</annotation>\n </semantics></math>). In this simulation, H and <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>H</mi>\n <mn>2</mn>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{H}}_2 $$</annotation>\n </semantics></math> neutrals are assumed to be uniformly distributed in space in order to obtain initial qualitative results. The fraction of <span></span><math>\n <semantics>\n <mrow>\n <msubsup>\n <mi>H</mi>\n <mn>3</mn>\n <mo>+</mo>\n </msubsup>\n </mrow>\n <annotation>$$ {\\mathrm{H}}_3^{+} $$</annotation>\n </semantics></math> ions increases as the <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>H</mi>\n <mn>2</mn>\n </msub>\n </mrow>\n <annotation>$$ {\\mathrm{H}}_2 $$</annotation>\n </semantics></math> molecular density increases, and the recombination process between <span></span><math>\n <semantics>\n <mrow>\n <msubsup>\n <mi>H</mi>\n <mn>3</mn>\n <mo>+</mo>\n </msubsup>\n </mrow>\n <annotation>$$ {\\mathrm{H}}_3^{+} $$</annotation>\n </semantics></math> and electrons is observed to reduce the particle flux to the target plate. With an increase in H density, the electron density increases due to the decrease in ion flow velocity due to the change exchange process, and the electron temperature decreases to less than 1 eV, leading to the detached plasma formation attributed to the electron-ion recombination process.</p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"64 7-8","pages":""},"PeriodicalIF":1.3000,"publicationDate":"2024-06-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/ctpp.202300150","citationCount":"0","resultStr":"{\"title\":\"First results of multi-fluid modeling of detached hydrogen plasmas in a linear plasma device using fluid code LINDA-NU\",\"authors\":\"Kento Sugiura, Taichi Ido, Hirohiko Tanaka, Hiroki Natsume, Shota Masuda, Kazuo Hoshino, Keiji Sawada, Noriyasu Ohno\",\"doi\":\"10.1002/ctpp.202300150\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>In order to simulate hydrogen (H) plasma in the linear plasma device NAGDIS-II, we have modified the fluid code LINDA-NU to allow the simultaneous calculation of multiple ion species consisting of hydrogen atomic ions (<span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mi>H</mi>\\n <mo>+</mo>\\n </msup>\\n </mrow>\\n <annotation>$$ {\\\\mathrm{H}}^{+} $$</annotation>\\n </semantics></math>) and molecular ions (<span></span><math>\\n <semantics>\\n <mrow>\\n <msubsup>\\n <mi>H</mi>\\n <mn>2</mn>\\n <mo>+</mo>\\n </msubsup>\\n <mo>,</mo>\\n <msubsup>\\n <mi>H</mi>\\n <mn>3</mn>\\n <mo>+</mo>\\n </msubsup>\\n </mrow>\\n <annotation>$$ {\\\\mathrm{H}}_2^{+},{\\\\mathrm{H}}_3^{+} $$</annotation>\\n </semantics></math>). In this simulation, H and <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>H</mi>\\n <mn>2</mn>\\n </msub>\\n </mrow>\\n <annotation>$$ {\\\\mathrm{H}}_2 $$</annotation>\\n </semantics></math> neutrals are assumed to be uniformly distributed in space in order to obtain initial qualitative results. The fraction of <span></span><math>\\n <semantics>\\n <mrow>\\n <msubsup>\\n <mi>H</mi>\\n <mn>3</mn>\\n <mo>+</mo>\\n </msubsup>\\n </mrow>\\n <annotation>$$ {\\\\mathrm{H}}_3^{+} $$</annotation>\\n </semantics></math> ions increases as the <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>H</mi>\\n <mn>2</mn>\\n </msub>\\n </mrow>\\n <annotation>$$ {\\\\mathrm{H}}_2 $$</annotation>\\n </semantics></math> molecular density increases, and the recombination process between <span></span><math>\\n <semantics>\\n <mrow>\\n <msubsup>\\n <mi>H</mi>\\n <mn>3</mn>\\n <mo>+</mo>\\n </msubsup>\\n </mrow>\\n <annotation>$$ {\\\\mathrm{H}}_3^{+} $$</annotation>\\n </semantics></math> and electrons is observed to reduce the particle flux to the target plate. With an increase in H density, the electron density increases due to the decrease in ion flow velocity due to the change exchange process, and the electron temperature decreases to less than 1 eV, leading to the detached plasma formation attributed to the electron-ion recombination process.</p>\",\"PeriodicalId\":10700,\"journal\":{\"name\":\"Contributions to Plasma Physics\",\"volume\":\"64 7-8\",\"pages\":\"\"},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2024-06-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1002/ctpp.202300150\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Contributions to Plasma Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/ctpp.202300150\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, FLUIDS & PLASMAS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Contributions to Plasma Physics","FirstCategoryId":"101","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/ctpp.202300150","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
引用次数: 0
摘要
为了模拟线性等离子体装置 NAGDIS-II 中的氢(H)等离子体,我们修改了流体代码 LINDA-NU,使其能够同时计算由氢原子离子()和分子离子()组成的多个离子种类。在该模拟中,假定氢和中性物质在空间均匀分布,以获得初步定性结果。随着分子密度的增加,离子的比例也在增加,并且观察到电子和离子之间的重组过程降低了目标板的粒子通量。随着 H 密度的增加,电子密度会因变化交换过程导致的离子流速降低而增加,电子温度会降低到 1 eV 以下,从而导致电子-离子重组过程所形成的分离等离子体。
First results of multi-fluid modeling of detached hydrogen plasmas in a linear plasma device using fluid code LINDA-NU
In order to simulate hydrogen (H) plasma in the linear plasma device NAGDIS-II, we have modified the fluid code LINDA-NU to allow the simultaneous calculation of multiple ion species consisting of hydrogen atomic ions () and molecular ions (). In this simulation, H and neutrals are assumed to be uniformly distributed in space in order to obtain initial qualitative results. The fraction of ions increases as the molecular density increases, and the recombination process between and electrons is observed to reduce the particle flux to the target plate. With an increase in H density, the electron density increases due to the decrease in ion flow velocity due to the change exchange process, and the electron temperature decreases to less than 1 eV, leading to the detached plasma formation attributed to the electron-ion recombination process.