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1 Outlne 1. Introducton

2 Introducton Image of MUSES-C on engne JAXA

3 b = 4ε 9 q m V d 3 a

4 large-scale) MHD

5 MPD chokng VASIMR Super-Alfvénc flow plasma detachment

6 HITOP(HIgh densty TOhoku Plasma) Devce Magnetc Cols Spectrometer Mach Probe Array S egmented E nd-plate +0.4 MPDA Laval Nozzle Col X Plasma X(m) Y Z TMP D Movable Probe TMP 0 1 Z(m) 3 Typcal Parameters Cylndrcal chamber : length = 3.3 m, nner dameter = 0.8 m Magnetc feld : up to 0.1 T Plasma source : MPD Arcet Ion temperature : 0-40eV Electron temperature : 3-10 ev Plasma densty : ~10 15 cm -3 (near the MPDA) Ionzaton degree : 50-90%

7 MPD(Magneto-Plasma-Dynamc) Arcet Cross Secton of MPDA Fast Actng Valve Gas Flow 0.1 (m) Gas Reservor Insulator Anode φ 0.03(m) φ 0.01(m) Plasma Cathode The MPDA has a coaxal structure wth a center tungsten rod cathode and an annular molybdenum anode. By use of a fast-actng gas-puff valve, a quas-steady ( ~1 msec ), hgh-densty (up to cm -3 near the MPD outlet), hghly-onzed plasma s produced. X Y Z Prncple of Plasma Acceleraton (a) Self-Feld Acceleraton (Anode) F z = r B θ (Cathode) q z F r = z B θ F r (Anode) (b) Wth Externally-Appled Feld (Anode) B z z (Cathode) r (Anode) q = r B z B z

8 Mach Probe Calbraton up down type up down M = exp M c M c : const. Huds and Rdsky model : 0.5 Hutchnson model(flud) : 0.44 Stangeby model : 1.0 M c k para perp = U M = γ ete + γ T κ ( for M m > 1) () para perp M = exp () 1 para = exp a α M M perp Stangeby and Allen(1971) ( α = lnκ )(for < 1) (),() M = 1

9 Mach Probe Calbraton up - down type para-perp type up down = exp M M c M > 1 M < 1 = κ = exp M α M α 1 α= lnκ M c = 0.40 k = 0.33

10 Dagnostcs ~ Spectroscopc Technque ~ T Partcle Temperature = m c k λ λ 0 1 e (Doppler Broadenng) Flow Veloctes λz snφ uz = c, uθ = c λ 0 λ λ 0 θ (Doppler Shft) Measured Spectrum Lnes HeI(atom) : nm HeII(on) : nm

11 Flow Characterstcs of MPD Plasma Plasma behavor n a dvergng magnetc nozzle #1, #, #3 I d =8.kA, dm/dt=0.7g/s, He plasma

12 Standng Shock Formaton n an MPD Plasma Flow (He), measured wth the Mach probe at X=0 (a) Supersonc flow n a dvergng feld (a) (b) (c) (b) Shock formaton and deceleraton n a bump feld (c) Re-acceleraton n a Laval nozzle

13 Rankne - Hugonot Relatons n n 1 = U U 1 = ( γ + 1) ( γ 1) + M M M = ( γ 1) γ M 1 M 1 ( γ 1) Subscrpts 1 and ndcate quanttes upstream and downstream of shock regon, respectvely. + assumng g = 5/3, g e =1

14 Shock Thckness pc/w p Bow shock l 0 =pc/w p

15 Instabltes n an MPD Plasma Flow (>8kA) Plasma behavor n azmuthal drecton

16 Instabltes n an MPD Plasma Flow Plasma behavor n axal drecton Schematc helcally-twsted plasma column From the phase dfference of azmuthal and axal probe array sgnal, the plasma has twsted structure and t rotates n the same drecton of the twst.

17 Control of Instabltes n an MPD Plasma Control of plasma nstablty by adustng plasma current Kruskcal-Shafranov Crteron q = 4π µ 0 a B LI Z Z Helcal Knk Insta.

18 Instabltes n an MPD Plasma Flow Helcal Insta. :NGC461 NASA

19 Summary

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