Please use this identifier to cite or link to this item: https://open.uns.ac.rs/handle/123456789/14079
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dc.contributor.authorRadujkov V.en
dc.contributor.authorPavlov M.en
dc.date.accessioned2020-03-03T14:54:50Z-
dc.date.available2020-03-03T14:54:50Z-
dc.date.issued1986-01-01en
dc.identifier.issn00224073en
dc.identifier.urihttps://open.uns.ac.rs/handle/123456789/14079-
dc.description.abstractThe influence of the glass-to-plasma boundary layers on the continuum radiation of hydrogen plasma has been experimenally checked at the Hβ wavelength by introducing an additional number of boundary layers into the observed plasmas produced inside of a T-shaped electromagnetic shock tube. In the first case (case A), the plasma was observed (by using a monochromator) with the two usual boundary layers. In the second case (case B), four additional boundary layers were created by introducing two glass plates into the plasma. During the first microsecond, after the reflected shock front had passed the point of observation, no major differece was noted between the continuum intensities in cases A and B. At 1.5 μs and later, the difference amounted to about 10 to 20% with case B being more intense, depending on time, that is on the plasma parameters and boundary-layer thickness. © 1986.en
dc.relation.ispartofJournal of Quantitative Spectroscopy and Radiative Transferen
dc.titleMeasurements of the glass-to-plasma boundary-layer influence on continuum radiation in a T-tubeen
dc.typeJournal/Magazine Articleen
dc.identifier.doi10.1016/0022-4073(86)90035-Xen
dc.identifier.scopus2-s2.0-46149133347en
dc.identifier.urlhttps://api.elsevier.com/content/abstract/scopus_id/46149133347en
dc.relation.lastpage482en
dc.relation.firstpage479en
dc.relation.issue6en
dc.relation.volume35en
item.fulltextNo Fulltext-
item.grantfulltextnone-
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