FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W1966302537> ?p ?o ?g. }

• W1966302537 endingPage "073042" @default.
• W1966302537 startingPage "073042" @default.
• W1966302537 abstract "Linear, two-fluid, resistive modelling of the plasma response to applied non-axisymmetric fields shows significant displacement of edge temperature and density profiles. The calculated displacements, often of 2 cm or more in H-mode pedestals with parameters appropriate to DIII-D, are due to the helical distortions resulting from stable edge modes being driven to finite amplitude by the applied fields. In many cases, these displacements are greater in magnitude, and different in phase, than the distortions of the separatrix manifolds predicted from vacuum modelling. Comparison of these results with experimental measurements from Thomson scattering and soft x-ray imaging finds good quantitative agreement. In these experiments, the phase of the applied non-axisymmetric magnetic field was flipped or rotated in order to probe the non-axisymmetric features of the response. The poloidal structures measured by x-ray imaging show clear indications of a helical response, as opposed to simply a change in the axisymmetric transport. Inclusion of two-fluid effects and rotation are found to be important in obtaining quantitative agreement with Thomson scattering data. Modelling shows screening of islands in the H-mode pedestal, but island penetration near the top of the pedestal where the electron rotation vanishes in plasmas with co-current rotation. Enhanced transport due to these islands may provide a mechanism for maintaining the pedestal width below the stability threshold of edge-localized modes. For typical DIII-D parameters, it is shown that the linear approximation is often near or beyond the limit of validity in the H-mode edge; however, the general agreement with experimental measurements indicates that these linear results nevertheless maintain good predictive value for profile displacements." @default.
• W1966302537 created "2016-06-24" @default.
• W1966302537 creator A5002670428 @default.
• W1966302537 creator A5008292006 @default.
• W1966302537 creator A5008654555 @default.
• W1966302537 creator A5012120152 @default.
• W1966302537 creator A5024582470 @default.
• W1966302537 creator A5031861334 @default.
• W1966302537 creator A5048368712 @default.
• W1966302537 creator A5055929376 @default.
• W1966302537 creator A5059537600 @default.
• W1966302537 creator A5085859739 @default.
• W1966302537 date "2013-06-24" @default.
• W1966302537 modified "2023-09-29" @default.
• W1966302537 title "Role of plasma response in displacements of the tokamak edge due to applied non-axisymmetric fields" @default.
• W1966302537 cites W1965784948 @default.
• W1966302537 cites W1976415743 @default.
• W1966302537 cites W1982070549 @default.
• W1966302537 cites W1984354620 @default.
• W1966302537 cites W1986545170 @default.
• W1966302537 cites W1994774681 @default.
• W1966302537 cites W2001450944 @default.
• W1966302537 cites W2002108619 @default.
• W1966302537 cites W2012686850 @default.
• W1966302537 cites W2012782895 @default.
• W1966302537 cites W2013727240 @default.
• W1966302537 cites W2015328600 @default.
• W1966302537 cites W2023983509 @default.
• W1966302537 cites W2027663903 @default.
• W1966302537 cites W2035302624 @default.
• W1966302537 cites W2039928824 @default.
• W1966302537 cites W2040641278 @default.
• W1966302537 cites W2045363728 @default.
• W1966302537 cites W2055518234 @default.
• W1966302537 cites W2056617296 @default.
• W1966302537 cites W2067165040 @default.
• W1966302537 cites W2078630188 @default.
• W1966302537 cites W2082112515 @default.
• W1966302537 cites W2083447730 @default.
• W1966302537 cites W2087699219 @default.
• W1966302537 cites W2088273479 @default.
• W1966302537 cites W2089924030 @default.
• W1966302537 cites W2100697473 @default.
• W1966302537 cites W2124368479 @default.
• W1966302537 cites W2130208330 @default.
• W1966302537 cites W2138002966 @default.
• W1966302537 cites W2142892973 @default.
• W1966302537 cites W2161159252 @default.
• W1966302537 cites W2167090960 @default.
• W1966302537 cites W2168339958 @default.
• W1966302537 doi "https://doi.org/10.1088/0029-5515/53/7/073042" @default.
• W1966302537 hasPublicationYear "2013" @default.
• W1966302537 type Work @default.
• W1966302537 sameAs 1966302537 @default.
• W1966302537 citedByCount "56" @default.
• W1966302537 countsByYear W19663025372013 @default.
• W1966302537 countsByYear W19663025372014 @default.
• W1966302537 countsByYear W19663025372015 @default.
• W1966302537 countsByYear W19663025372016 @default.
• W1966302537 countsByYear W19663025372017 @default.
• W1966302537 countsByYear W19663025372018 @default.
• W1966302537 countsByYear W19663025372019 @default.
• W1966302537 countsByYear W19663025372020 @default.
• W1966302537 countsByYear W19663025372021 @default.
• W1966302537 countsByYear W19663025372022 @default.
• W1966302537 countsByYear W19663025372023 @default.
• W1966302537 crossrefType "journal-article" @default.
• W1966302537 hasAuthorship W1966302537A5002670428 @default.
• W1966302537 hasAuthorship W1966302537A5008292006 @default.
• W1966302537 hasAuthorship W1966302537A5008654555 @default.
• W1966302537 hasAuthorship W1966302537A5012120152 @default.
• W1966302537 hasAuthorship W1966302537A5024582470 @default.
• W1966302537 hasAuthorship W1966302537A5031861334 @default.
• W1966302537 hasAuthorship W1966302537A5048368712 @default.
• W1966302537 hasAuthorship W1966302537A5055929376 @default.
• W1966302537 hasAuthorship W1966302537A5059537600 @default.
• W1966302537 hasAuthorship W1966302537A5085859739 @default.
• W1966302537 hasConcept C116515362 @default.
• W1966302537 hasConcept C119599485 @default.
• W1966302537 hasConcept C120665830 @default.
• W1966302537 hasConcept C121332964 @default.
• W1966302537 hasConcept C127413603 @default.
• W1966302537 hasConcept C166957645 @default.
• W1966302537 hasConcept C191486275 @default.
• W1966302537 hasConcept C207821765 @default.
• W1966302537 hasConcept C2524010 @default.
• W1966302537 hasConcept C2778495671 @default.
• W1966302537 hasConcept C2778611943 @default.
• W1966302537 hasConcept C2779146573 @default.
• W1966302537 hasConcept C30475298 @default.
• W1966302537 hasConcept C33026886 @default.
• W1966302537 hasConcept C33923547 @default.
• W1966302537 hasConcept C57879066 @default.
• W1966302537 hasConcept C62520636 @default.
• W1966302537 hasConcept C6899612 @default.
• W1966302537 hasConcept C74050887 @default.
• W1966302537 hasConcept C82706917 @default.
• W1966302537 hasConcept C95457728 @default.

• next