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JOURNALS // Uspekhi Fizicheskikh Nauk // Archive

UFN, 2017 Volume 187, Number 5, Pages 547–574 (Mi ufn5740)

This article is cited in 55 papers

INSTRUMENTS AND METHODS OF INVESTIGATION

Gas dynamic trap: experimental results and future prospects

A. A. Ivanovab, V. V. Prikhodkocab

a Budker Institute of Nuclear Physics, Siberian Branch of Russian Academy of Sciences, Novosibirsk
b Novosibirsk State University
c Nuclear Safety Institute, Russian Academy of Sciences (IBRAE), Moscow

Abstract: The gas dynamic trap (GDT) is a version of a magnetic mirror with a long mirror-to-mirror distance far exceeding the effective mean free path of ion scattering into the loss cone, with a large mirror ratio ($R \sim 100$, $R=B_{\text{max}}/B_{\text{min}}$ is the ratio of magnetic field inductions at the mirror and at the trap center) and with axial symmetry. Under these conditions, in contrast to a conventional magnetic mirror, the plasma confined in a GDT is isotropic and Maxwellian. The plasma loss rate through the ends is governed by a set of simple gas dynamic equations; hence, the name of the device. The plasma lifetime in a GDT is on the order of $L R/V_{\text{Ti}}$, where $L$ is the mirror-to-mirror distance, and $V_{\text{Ti}}$ is the ion thermal velocity. Thus, increasing both the length of the device and the mirror ratio can, in principle, make the plasma lifetime sufficient for fusion applications. This paper discusses plasma confinement and heating results from the Novosibirsk GDT facility and examines prospects for using GDTs to develop a high-flux volumetric neutron source for fusion material testing and for driving subcritical fission reactors.

PACS: 28.52.-s, 52.50.-b, 52.55.Jd

Received: July 4, 2016
Revised: September 20, 2016
Accepted: September 30, 2016

DOI: 10.3367/UFNr.2016.09.037967


 English version:
Physics–Uspekhi, 2017, 60:5, 509–533

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