000894359 001__ 894359 000894359 005__ 20240711085645.0 000894359 0247_ $$2doi$$a10.1007/s11666-021-01235-6 000894359 0247_ $$2ISSN$$a1059-9630 000894359 0247_ $$2ISSN$$a1544-1016 000894359 0247_ $$2Handle$$a2128/29350 000894359 0247_ $$2WOS$$aWOS:000675746800001 000894359 037__ $$aFZJ-2021-03194 000894359 041__ $$aEnglish 000894359 082__ $$a670 000894359 1001_ $$0P:(DE-HGF)0$$aZimmermann, Stephan$$b0 000894359 245__ $$aCharacterization of an Axial-Injection Plasma Spray Torch 000894359 260__ $$aBoston, Mass.$$bSpringer$$c2021 000894359 3367_ $$2DRIVER$$aarticle 000894359 3367_ $$2DataCite$$aOutput Types/Journal article 000894359 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1638854543_10164 000894359 3367_ $$2BibTeX$$aARTICLE 000894359 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000894359 3367_ $$00$$2EndNote$$aJournal Article 000894359 520__ $$aThe Axial III™ torch is a multiple-arc plasma generator with a set of three single cathode–anode units, which is still of significant importance, especially in the field of suspension plasma spraying. The division of the plasma generator into three spatially separated systems allows for central feedstock injection with improved deposition rates and efficiencies. In this work, several diagnostic methods were applied to characterize the plasma jet of an Axial III™ spray torch to further the understanding of this spray system. One important result was that the plasma temperature in the jet exhibits a triple distribution with three straight lobes arranged around the jet axis. As with every plasma torch, the total plasma power is subject to fast temporal variations. Power variations were clearly seen in the plasma jet even though it could have been anticipated that the triple jet characteristics and the natural fluctuations of the arcs generated by the three single cathode–anode units would be less pronounced after merging the three plasma streams. Unaffected by this it is nevertheless likely that the axially injected feedstock particles are caged effectively in the core of the plasma jet. Hence, the total electrical torch power and the uniformity of the single unit’s powers must be monitored to realize possible degradation and asymmetries in the plasma temperature distribution, which may influence deposition parameters. 000894359 536__ $$0G:(DE-HGF)POF4-1241$$a1241 - Gas turbines (POF4-124)$$cPOF4-124$$fPOF IV$$x0 000894359 588__ $$aDataset connected to CrossRef, Journals: juser.fz-juelich.de 000894359 7001_ $$0P:(DE-Juel1)129633$$aMauer, Georg$$b1$$eCorresponding author 000894359 7001_ $$0P:(DE-Juel1)129653$$aRauwald, Karl-Heinz$$b2$$ufzj 000894359 7001_ $$0P:(DE-HGF)0$$aSchein, Jochen$$b3 000894359 773__ $$0PERI:(DE-600)2047715-6$$a10.1007/s11666-021-01235-6$$p1724–1736$$tJournal of thermal spray technology$$v30$$x1544-1016$$y2021 000894359 8564_ $$uhttps://juser.fz-juelich.de/record/894359/files/Zimmermann2021_Article_CharacterizationOfAnAxial-Inje.pdf$$yOpenAccess 000894359 8767_ $$d2021-07-22$$eHybrid-OA$$jDEAL 000894359 909CO $$ooai:juser.fz-juelich.de:894359$$pdnbdelivery$$popenCost$$pVDB$$pdriver$$pOpenAPC_DEAL$$popen_access$$popenaire 000894359 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)129633$$aForschungszentrum Jülich$$b1$$kFZJ 000894359 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)129653$$aForschungszentrum Jülich$$b2$$kFZJ 000894359 9131_ $$0G:(DE-HGF)POF4-124$$1G:(DE-HGF)POF4-120$$2G:(DE-HGF)POF4-100$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF4-1241$$aDE-HGF$$bForschungsbereich Energie$$lMaterialien und Technologien für die Energiewende (MTET)$$vHochtemperaturtechnologien$$x0 000894359 9141_ $$y2021 000894359 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS$$d2021-01-27 000894359 915__ $$0StatID:(DE-HGF)1160$$2StatID$$aDBCoverage$$bCurrent Contents - Engineering, Computing and Technology$$d2021-01-27 000894359 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0 000894359 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search$$d2021-01-27 000894359 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bJ THERM SPRAY TECHN : 2019$$d2021-01-27 000894359 915__ $$0StatID:(DE-HGF)0113$$2StatID$$aWoS$$bScience Citation Index Expanded$$d2021-01-27 000894359 915__ $$0StatID:(DE-HGF)3002$$2StatID$$aDEAL Springer$$d2021-01-27$$wger 000894359 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection$$d2021-01-27 000894359 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5$$d2021-01-27 000894359 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess 000894359 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC$$d2021-01-27 000894359 915__ $$0StatID:(DE-HGF)0160$$2StatID$$aDBCoverage$$bEssential Science Indicators$$d2021-01-27 000894359 915__ $$0StatID:(DE-HGF)0420$$2StatID$$aNationallizenz$$d2021-01-27$$wger 000894359 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List$$d2021-01-27 000894359 915pc $$0PC:(DE-HGF)0000$$2APC$$aAPC keys set 000894359 915pc $$0PC:(DE-HGF)0001$$2APC$$aLocal Funding 000894359 915pc $$0PC:(DE-HGF)0002$$2APC$$aDFG OA Publikationskosten 000894359 915pc $$0PC:(DE-HGF)0113$$2APC$$aDEAL: Springer Nature 2020 000894359 9201_ $$0I:(DE-Juel1)IEK-1-20101013$$kIEK-1$$lWerkstoffsynthese und Herstellungsverfahren$$x0 000894359 9801_ $$aFullTexts 000894359 980__ $$ajournal 000894359 980__ $$aVDB 000894359 980__ $$aUNRESTRICTED 000894359 980__ $$aI:(DE-Juel1)IEK-1-20101013 000894359 980__ $$aAPC 000894359 981__ $$aI:(DE-Juel1)IMD-2-20101013