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Magnetic mirror confinement

Fig. 2a and b. Magnetic mirror confinement systems a magnetic mirror b Yin-Yang Coils, minimum B magnetic mirror... [Pg.50]

By the end of 1977 Tokamak devices had achieved nre values in excess of 1019 m-3 s and ion temperatures of 2-3 keV. In the early summer of 1978, temperatures in excess of 7 keV were achieved in the Princeton large torus, PLT, using auxilary neutral beam heating9). Other confinement systems such as magnetic mirror devices and intertial confinement are also operating currently below the Lawson criterion but there has been continued development and substantial progress is continually being made. [Pg.49]

The problem with all the mirror approaches is that none has achieved the degree of confinement quaUty that the closed systems have. Closed systems ate characterized by magnetic field lines that close on themselves so that charged particles following the field lines remain confined within the system. [Pg.152]

Among several conceptual designs of fusion reactors, the machines based on magnetic confinement, such as Tokamak- and mirror-type reactors, employ a... [Pg.117]

See other pages where Magnetic mirror confinement is mentioned: [Pg.61]    [Pg.61]    [Pg.110]    [Pg.110]    [Pg.50]    [Pg.52]    [Pg.165]    [Pg.63]    [Pg.278]    [Pg.2767]    [Pg.388]    [Pg.130]    [Pg.312]    [Pg.2766]    [Pg.305]    [Pg.308]    [Pg.311]    [Pg.387]    [Pg.396]    [Pg.85]    [Pg.135]   
See also in sourсe #XX -- [ Pg.61 ]



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