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Characterization and Modification of Edge-Driven Instabilities in the DIII-D Tokamak

John R. Ferron, Lang L. Lao, Thomas H. Osborne, E. J. Strait, A. D. Turnbull, R. Miller, T. S. Taylor, E. J. Doyle, Bradley W. Rice, C. Zhang, L. Chen, L. R. Baylor, M. Murakami, M. R. Wade

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Abstract

The character of edge localized modes (ELMs) and the height of the edge pressure pedestal in DIII-D tokamak H-mode discharges have been modified by varying the discharge shape (triangularity and squareness) and the safety factor, increasing the edge radiation, and injecting deuterium pellets. Changes in the ELM frequency and amplitude, and the magnitude of the edge pressure gradient, and changes in the calculated extent of the region of access to the ballooning mode second stability regime are observed.

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What this paper is about

The character of edge localized modes (ELMs) and the height of the edge pressure pedestal in DIII-D tokamak H-mode discharges have been modified by varying the discharge shape (triangularity and squareness) and the safety factor, increasing the edge radiation, and injecting deuterium pellets. Changes in the ELM frequency and amplitude, and the magnitude of the edge pressure gradient, and changes in the calculated extent of the region of access to the ballooning mode second stability regime are observed.

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Available abstract

The character of edge localized modes (ELMs) and the height of the edge pressure pedestal in DIII-D tokamak H-mode discharges have been modified by varying the discharge shape (triangularity and squareness) and the safety factor, increasing the edge radiation, and injecting deuterium pellets. Changes in the ELM frequency and amplitude, and the magnitude of the edge pressure gradient, and changes in the calculated extent of the region of access to the ballooning mode second stability regime are observed.

Key concepts: DIII-D, Pedestal, Tokamak, Ballooning, Enhanced Data Rates for GSM Evolution, Amplitude, Pressure gradient, Physics

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