The Polaris Linear Plasma Device

dc.contributor.authorAntar, Ghassan Y.
dc.contributor.authorYounes, Joan
dc.contributor.authorDarwish, Marwan S.
dc.contributor.authorCostantine, Joseph
dc.contributor.authorRoumié, Mohamad
dc.contributor.authorHabchi, Charbel
dc.contributor.departmentDepartment of Physics
dc.contributor.departmentDepartment of Mechanical Engineering
dc.contributor.departmentDepartment of Electrical and Computer Engineering
dc.contributor.facultyFaculty of Arts and Sciences (FAS)
dc.contributor.facultyFaculty of Medicine (FM)
dc.contributor.facultyMaroun Semaan Faculty of Engineering and Architecture (MSFEA)
dc.contributor.institutionAmerican University of Beirut
dc.date.accessioned2025-01-24T11:25:16Z
dc.date.available2025-01-24T11:25:16Z
dc.date.issued2021
dc.description.abstractWe report the construction of Polaris, a new linear plasma device with an axial magnetic field dedicated to research and education at the American University of Beirut in Lebanon. The goal is to initiate the investigation of topics related to basic magnetized plasma physics and nuclear fusion. We discuss the novel technical solutions found to set up various components of the device. We start with the magnetic coils where we use power cables to generate the required axial magnetic field. They are included in a stainless steel case for water-cooling. Then, we present the vacuum and the gas inlet systems with which we control the neutral pressure. The way we manufacture the water-cooled radio frequency (RF) antenna allows the production of a variety of designs. Polaris is thus built to operate in a steady state. Using a reciprocating Langmuir probe, we determine the plasma properties as a function of the various control parameters. As the plasma remains in the 'blue mode,' we show that the increase in the main magnetic field leads to an increase in the density but a decrease in the plasma temperature. The increase in neutral pressure yields the same effects. However, the increase in RF power leads to an increase in both density and temperature. Finally, plans for future investigations are briefly described. © 1973-2012 IEEE.
dc.identifier.doihttps://doi.org/10.1109/TPS.2021.3070638
dc.identifier.eid2-s2.0-85104266781
dc.identifier.urihttp://hdl.handle.net/10938/26273
dc.language.isoen
dc.publisherInstitute of Electrical and Electronics Engineers Inc.
dc.relation.ispartofIEEE Transactions on Plasma Science
dc.sourceScopus
dc.subjectHelicon plasma
dc.subjectMagnetized plasma device
dc.subjectPlasma properties
dc.subjectRadio frequency (rf) antenna
dc.subjectRf waves
dc.subjectAntennas
dc.subjectCooling water
dc.subjectMagnetic fields
dc.subjectManufacture
dc.subjectPlasma devices
dc.subjectStars
dc.subjectAxial magnetic field
dc.subjectControl parameters
dc.subjectMagnetized plasmas
dc.subjectMain magnetic fields
dc.subjectNeutral pressures
dc.subjectPlasma temperature
dc.subjectRadio frequencies
dc.subjectTechnical solutions
dc.subjectMagnetoplasma
dc.titleThe Polaris Linear Plasma Device
dc.typeArticle

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