Excitation of high frequency pressure driven modes by non-axisymmetric equilibrium at high βpol in PBX-M
Creators
- Sesnic, S.1
- Kaita, R.1
- Kaye, S.1
- Okabayashi, M.1
- Takahashi, H.1
- Bell, R.E.1
- Bernabei, S.1
- Chance, M.S.1
- Hatcher, R.E.1
- Jardin, S.C.1
- Kessel, C.E.1
- Kugel, H.W.1
- LeBlanc, B.1
- Manickam, J.1
- Ono, M.1
- Paul, S.F.1
- Sauthoff, N.R.1
- Holland, A.2
- Asakura, N.3
- Duperrex, P.A.4
- Fonck, R.J.5
- Gammel, G.M.6
- Greene, G.J.7
- Jiang, T.W.8
- Levinton, F.M.9
- Powell, E.T.10
- Roberts, D.W.10
- Qin, Y.11
- Princeton Univ., NJ (United States). Plasma Physics Lab
- 1. Princeton Univ., NJ (United States). Plasma Physics Lab.
- 2. ARACOR, Sunnyvale, CA (United States)
- 3. Japan Atomic Energy Research Inst., Tokai, Ibaraki (Japan)
- 4. Lab. pour l'Armenment, Berne (Switzerland)
- 5. Wisconsin Univ., Madison, WI (United States). Dept. of Nuclear Engineering
- 6. Grumman Aerospace Corp., Bethpage, NY (United States)
- 7. Greene (G.J.), West Trenton, NJ (United States)
- 8. Academia Sinica, Hefei, AH (China). Inst. of Plasma Physics
- 9. Fusion Physics and Technology, Torrance, CA (United States)
- 10. Lawrence Livermore National Lab., CA (United States)
- 11. Southwest Inst. of Physics, Leshan, SC (China)
Description
High-frequency pressure-driven modes have been observed in high-poloidal-β discharges in the Princeton Beta Experiment-Modification (PBX-M). These modes are excited in a non-axisymmetric equilibrium characterized by a large, low frequency m1=1/n1=1 island, and they are capable of expelling fast ions. The modes reside on or very close to the q=1 surface, and have mode numbers with either mh=nh or (less probably) mh/nh=mh/(mh-1), with mh varying between 3 and 10. Occasionally, these modes are, simultaneously localized in the vicinity of the m1=2/n1=1 island. The high frequency modes near the q=1 surface also exhibit a ballooning character, being significantly stronger on the large major radius side of the plasma. When a large m1=1/n1=1 island is present the mode is poloidally localized in the immediate vicinity of the x-point of the island. The modes, which occur exclusively in high-β discharges, appear to be driven by the plasma pressure or pressure gradient. They can thus be a manifestation of either a toroidicity-induced shear Alfven eigenmode (TAE) at q=(2mh+ 1)/2nh, a kinetic ballooning mode (KBM), or some other type of pressure-driven mode. Theory predicts that the TAE mode is a gap mode, but the high frequency modes in PBX-M are found exclusively on or in the immediate neighborhood of magnetic surfaces with low rational numbers
Availability note (English)
MF available from INIS under the Report Number; Also available from OSTI as DE93016722; NTIS; US Govt. Printing Office Dep.Files
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Additional details
Publishing Information
- Imprint Pagination
- 44 p.
- Report number
- PPPL--2916
INIS
- Country of Publication
- United States
- Country of Input or Organization
- United States
- INIS RN
- 25013232
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY; S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Descriptors DEI
- ALFVEN WAVES; ASYMMETRY; BALLOONING INSTABILITY; BETA RATIO; EXCITATION; FREQUENCY DEPENDENCE; H-MODE PLASMA CONFINEMENT; MAGNETIC ISLANDS; MHD EQUILIBRIUM; PBX DEVICES; PLASMA PRESSURE; PRESSURE GRADIENTS
- Descriptors DEC
- CLOSED PLASMA DEVICES; CONFINEMENT; ENERGY-LEVEL TRANSITIONS; EQUILIBRIUM; HYDROMAGNETIC WAVES; INSTABILITY; MAGNETIC FIELD CONFIGURATIONS; PLASMA CONFINEMENT; PLASMA INSTABILITY; PLASMA MACROINSTABILITIES; THERMONUCLEAR DEVICES; TOKAMAK DEVICES
Optional Information
- Contract/Grant/Project number
- Contract AC02-76CH03073
- Funding organization
- USDOE, Washington, DC (United States).