Matches in SemOpenAlex for { <https://semopenalex.org/work/W2112888924> ?p ?o ?g. }
- W2112888924 endingPage "013001" @default.
- W2112888924 startingPage "013001" @default.
- W2112888924 abstract "Abstract The confinement in JET baseline type I ELMy H-mode plasmas is compared to that in so-called hybrid H-modes in a database study of 112 plasmas in JET with the carbon fibre composite (CFC) wall. The baseline plasmas typically have β N ∼ 1.5–2, H 98 ∼ 1, whereas the hybrid plasmas have β N ∼ 2.5–3, H 98 < 1.5. The database study contains both low- ( δ ∼ 0.2–0.25) and high-triangularity ( δ ∼ 0.4) hybrid and baseline H-mode plasmas from the last JET operational campaigns in the CFC wall from the period 2008–2009. Based on a detailed confinement study of the global as well as the pedestal and core confinement, there is no evidence that the hybrid and baseline plasmas form separate confinement groups; it emerges that the transition between the two scenarios is of a gradual kind rather than demonstrating a bifurcation in the confinement. The elevated confinement enhancement factor H 98 in the hybrid plasmas may possibly be explained by the density dependence in the τ 98 scaling as n 0.41 and the fact that the hybrid plasmas operate at low plasma density compared to the baseline ELMy H-mode plasmas. A separate regression on the confinement data in this study shows a reduction in the density dependence as n 0.09±0.08 . Furthermore, inclusion of the plasma toroidal rotation in the confinement regression provides a scaling with the toroidal Alfvén Mach number as <?CDATA ${rm Mach}_{rm A}^{0.41pm 0.07}$ ?> and again a reduced density dependence as n 0.15±0.08 . The differences in pedestal confinement can be explained on the basis of linear MHD stability through a coupling of the total and pedestal poloidal pressure and the pedestal performance can be improved through plasma shaping as well as high β operation. This has been confirmed in a comparison with the EPED1 predictive pedestal code which shows a good agreement between the predicted and measured pedestal pressure within 20–30% for a wide range of β N ∼ 1.5–3.5. The core profiles show a strong degree of pressure profile consistency. No beneficial effect of core density peaking on confinement could be identified for the majority of the plasmas presented here as the density peaking is compensated by a temperature de-peaking resulting in no or only a weak variation in the pressure peaking. The core confinement could only be optimized in case the ions and electrons are decoupled, in which case the ion temperature profile peaking can be enhanced, which benefits confinement. In this study, the latter has only been achieved in the low-triangularity hybrid plasmas, and can be attributed to low-density operation. Plasma rotation has been found to reduce core profile stiffness, and can explain an increase in profile peaking at small radius ρ tor = 0.3." @default.
- W2112888924 created "2016-06-24" @default.
- W2112888924 creator A5001749589 @default.
- W2112888924 creator A5006772600 @default.
- W2112888924 creator A5015061883 @default.
- W2112888924 creator A5019126275 @default.
- W2112888924 creator A5025236752 @default.
- W2112888924 creator A5026832780 @default.
- W2112888924 creator A5026880159 @default.
- W2112888924 creator A5028335949 @default.
- W2112888924 creator A5038085546 @default.
- W2112888924 creator A5040421248 @default.
- W2112888924 creator A5041788679 @default.
- W2112888924 creator A5043933344 @default.
- W2112888924 creator A5044280486 @default.
- W2112888924 creator A5057972372 @default.
- W2112888924 creator A5059097939 @default.
- W2112888924 creator A5061847087 @default.
- W2112888924 creator A5062109572 @default.
- W2112888924 creator A5063263731 @default.
- W2112888924 creator A5069067572 @default.
- W2112888924 creator A5070451829 @default.
- W2112888924 creator A5073724995 @default.
- W2112888924 creator A5074008035 @default.
- W2112888924 creator A5077414738 @default.
- W2112888924 creator A5081608139 @default.
- W2112888924 creator A5083103072 @default.
- W2112888924 creator A5083441894 @default.
- W2112888924 creator A5090302079 @default.
- W2112888924 date "2012-12-05" @default.
- W2112888924 modified "2023-10-18" @default.
- W2112888924 title "Comparison of hybrid and baseline ELMy H-mode confinement in JET with the carbon wall" @default.
- W2112888924 cites W1967595978 @default.
- W2112888924 cites W1972119058 @default.
- W2112888924 cites W1973896528 @default.
- W2112888924 cites W1975102171 @default.
- W2112888924 cites W1975627719 @default.
- W2112888924 cites W1976034176 @default.
- W2112888924 cites W1978804706 @default.
- W2112888924 cites W1979039627 @default.
- W2112888924 cites W1985368215 @default.
- W2112888924 cites W1986545170 @default.
- W2112888924 cites W1994835364 @default.
- W2112888924 cites W1995095888 @default.
- W2112888924 cites W1995328890 @default.
- W2112888924 cites W1995520438 @default.
- W2112888924 cites W1997666441 @default.
- W2112888924 cites W2004973341 @default.
- W2112888924 cites W2011927626 @default.
- W2112888924 cites W2012961687 @default.
- W2112888924 cites W2021217921 @default.
- W2112888924 cites W2036077035 @default.
- W2112888924 cites W2036851632 @default.
- W2112888924 cites W2042613750 @default.
- W2112888924 cites W2046477827 @default.
- W2112888924 cites W2054081779 @default.
- W2112888924 cites W2055293470 @default.
- W2112888924 cites W2060726845 @default.
- W2112888924 cites W2061037071 @default.
- W2112888924 cites W2061612131 @default.
- W2112888924 cites W2066734217 @default.
- W2112888924 cites W2070387422 @default.
- W2112888924 cites W2076909268 @default.
- W2112888924 cites W2079520212 @default.
- W2112888924 cites W2082337849 @default.
- W2112888924 cites W2084930602 @default.
- W2112888924 cites W2095005575 @default.
- W2112888924 cites W2099088725 @default.
- W2112888924 cites W2109594604 @default.
- W2112888924 cites W2113585385 @default.
- W2112888924 cites W2117114033 @default.
- W2112888924 cites W2120014729 @default.
- W2112888924 cites W2121529216 @default.
- W2112888924 cites W2131982670 @default.
- W2112888924 cites W2137453930 @default.
- W2112888924 cites W2150787345 @default.
- W2112888924 cites W2162167567 @default.
- W2112888924 cites W4211151981 @default.
- W2112888924 doi "https://doi.org/10.1088/0029-5515/53/1/013001" @default.
- W2112888924 hasPublicationYear "2012" @default.
- W2112888924 type Work @default.
- W2112888924 sameAs 2112888924 @default.
- W2112888924 citedByCount "22" @default.
- W2112888924 countsByYear W21128889242013 @default.
- W2112888924 countsByYear W21128889242014 @default.
- W2112888924 countsByYear W21128889242015 @default.
- W2112888924 countsByYear W21128889242016 @default.
- W2112888924 countsByYear W21128889242017 @default.
- W2112888924 countsByYear W21128889242018 @default.
- W2112888924 countsByYear W21128889242019 @default.
- W2112888924 countsByYear W21128889242020 @default.
- W2112888924 countsByYear W21128889242021 @default.
- W2112888924 countsByYear W21128889242022 @default.
- W2112888924 crossrefType "journal-article" @default.
- W2112888924 hasAuthorship W2112888924A5001749589 @default.
- W2112888924 hasAuthorship W2112888924A5006772600 @default.
- W2112888924 hasAuthorship W2112888924A5015061883 @default.
- W2112888924 hasAuthorship W2112888924A5019126275 @default.