Issues in Zonal Flows and Drift Wave Turbulence P.H. Diamond CMTFO and CASS, UCSD; USA WCI Center for Fusion Theory, NFRI; Korea ISSI Workshop, 4-9 March, 2012 1 !" #$$ %& 2 0 !" %"! )'(&($ #) &$% *+%" ,( &! " ) -. /" 3 Preamble I planets Tokamaks Zonal Flows: m=n=0 finite kr potential fluctuations 4 Preamble II → Re:Plasma? → 2 Simple Models a.) Hasegawa-Wakatani (collisional drift inst.) b.) Hasegawa-Mima (DW) c a.) V = ẑ × ∇φ + Vpol B → ms L > λD → ∇ · J = 0 → ∇⊥ · J⊥ = −∇� J� J⊥ = (i) n|e|Vpol J� : ηJ� = −(1/c)∂t A� − ∇� φ + ∇� pe b.) dne /dt = 0 → e.s. n.b. MHD: ∂t A� v.s. ∇� φ DW: ∇� pe v.s. ∇� φ ∇� J � dne + =0 dt −n0 |e| 5 So H-W ρ2s d 2 ∇ φ̂ = −D� ∇2� (φ̂ − n̂/n0 ) + ν∇2 ∇2 φ̂ dt D� k�2 /ω d n − D0 ∇2 n̂ = −D� ∇2� (φ̂ − n̂/n0 ) dt n.b. PV = n − ρ2s ∇2 φ total density 2 D k b.) � � /ω � 1 → n̂/n0 ∼ eφ̂/Te d (φ − ρ2s ∇2 φ) + v∗ ∂y φ = 0 dt n.b. n.b. is key parameter d (PV) = 0 dt (m, n �= 0) → H-M PV = φ − ρ2s ∇2 φ + ln n0 (x) Zonal Flows: ρ2s d 2 ∇ φ = −µ∇2 φ + ν∇2 ∇2 φ dt 6 An infinity of models follow: - MHD: ideal ballooning resistive → RBM - HW + A�: drift - Alfven - HW + curv. : drift - RBM - HM + curv. + Ti: Fluid ITG - gyro-fluids - GK N.B.: Most Key advances appeared in consideration of simplest possible models 7 6 :#H I':#:#(! 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N % 7%" :'-5;<; 35 %" 5 40+1 1 U"@ ; , *, * * * * * 43 4* ' 3 ' * ?/5)!>(+ B@A@ , * * * 8 * 4 0 U" 4U" 4 ;4 4 +4 74 >'= < '+,) 36 % 1 ($ ? )8$ < * 0 - , *< *# * * 4 4 4 0 4 4 --^^ 0 G$C$ &"N 4 ?$ 3)!$N@ U-1 (!0 $"" !$ "*--U! &)9 1 !7 $ ) " 0 $)>)>$$@ --D!8 $ $" & $& >!@"N 37 1 ( 0 + 3 $ &$ 0 " $$& C &"$ $ G$C > 0 &$$"$ $N 38 --C " ?D( 1 ?D*-)GF5 &! 1 ( $)8$ B-#!"7(-' #-D )7 - >7B-+O -[7 O-O " O- 7B--\7 -D&& 7-T-!& 1 ! 9 2(,C .0 * [) 39 What is the H-mode? What is a transport barrier? 40 shows an example close to the power or density threshold where the discharge dithers between the L and I phases— illustrated by the divertor tile shunt current (/ SOL flow). Experimental motivation [Conway ‘11 PRL] shot [Schmitz, TTF ‘11] FIG. 2 (color online). (a) Tim -3) expanded reflectometer sp ! L-H threshold Power in low density region (typically lower than 3x1019m(b) FIG. 1 (color online). (a) GAM existence plot in terms of Pnet for higher intensity, with (c) ! vs I-phase a transient between high confinement, transition. centralasline averagephase density. (b) low Edgeand radial electric fieldi.e. Er L!I!H fluctuation level SD , and (d) for oscillation L (PECH in ¼prior 0:35 to MW) and I in phase (1.1 MW) rates ‘10 andPoP], turbulence ! profiles Limit cycle the transition TJ-II[Estrada ‘10 EPL],shearing NSTX[Zweben ¼ 0:8EAST[Xu MA, q95 4:5, n! e ¼ 3 ' shot 24 811, BT ¼ !2:3 T,‘11IpPRL], L to I phase. BT ¼ !2:3 T, Ip ASDEX Upgrade[Conway ‘11#PRL] 19 m!3 , T # 3 keV, P 1019 m!3 , Teo # 2:4 keV, and favorable lower X point. 10 eo ECH ! Radial structure of mean flow shear in the I-phase limit-cycle oscillation ! Dual shear layer in DIII-D [Schmitz, TTF ‘11] 065001-2 ! Poloidal rotation involving in the transition process in JT-60U [Kamiya ‘10 PRL] 41 42 43 44 → EAST Results (G.S. Xu, et.al., ’11) → hardened, reciprocating probes → quasi-periodic Er oscillation (f < 4 kHz), with associated turbulence modulation → Er and �ṽr ṽθ �E exhibits correlated spikes prior to transition → support key role of zonal flow in L→H transition Power spectra peaks at f < 4kHz spike in Er and �ṽr ṽθ �E 45 1 %$) F G/0/ C< ( "D#E ( ( (+ 0 0 0+ - - 45 "6 +.- 5 .- 75 "># 5 +$ 182 1 $8 $5$ P<$"$& --$"$ & $ $" !5$ *.-3"># ' "># & $ *'-O 7%--75;;_ +7 %--75;;J +$$ $& ? $ 1 :D7( 0 ) C7D 0 . 0 "># .C)C 46 # 6 , " /+* " 25" :#J! "! '( #)" *$) &%#4 5 + % ,)/+*)4 55 4 ,:# '' -' 47 Slow Power Ramp Indicates L!I!H Evolution. L-mode Intermediate phase Limit Cycle Oscillations H-mode a) turbulence b) ZF c) log(MF) 7 r/a time 48 Cycle is propagating nonlinear wave in edge layer ZF Period of cycle increases approaching transition. Turbulence intensity Mean flow shear • Turbulence intensity peaks just prior to transition. • Mean shear (i.e. profiles) also oscillates in I-phase. 49 Mean shear location comparisons indicate inward propagation. 50 1 9%97"4 )& !7& 1 +! $!$ 1 !$) 1 +"$ " ! & &" $ ) COP 1 R" 77))7$ $ ))9B+77+ !7+% !9 U &3@ 51 If you build it, they will came... Basic experiment: - large, rotating, ∼ QG (tilted caps) liquid metal or equivalent with Rm ∼ 100 - extend domain of PPPL experiment of H. Ji, et.al. - aims: - MHD dynamics of zonal flows, jets - zonal fields, QG dynamo (L-Smith, Tobias) - aspects of MHD momentum transport (i.e. solar tachocline physics) 52 ‘Confinement’ experiments: (EAST?) - high power, low τext ITB - multi-channel DBS imaging study of qmin region, on meso-scale -multi-channel CHS to eliminate mean flows (including poloidal) - high space-time resolution profile evolution, i.e. corrugations? 53 1 (-($ !7 ! " "1 # $" ) !B4 &"& N 54