AAWSAP DIRD, Inertial Electrostatic Confinement Fusion, March 2010
DOW-UAP-D125 · page 64 of 72
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UNCLASSIFIED//FOR OFFI&I.\k Wfili Ql"lk¥ Confined ¥' Plasma Sol nod Cotl -·•· emholtz Field Cotl.s Floatm Figure 5.7. Illustration of a Three-Unit MCSA Device Next we consider in more detail the new physics concepts, recirculation and retrapping, that provide the basis for magnet channel coupling. Recirculation of Radial Belt Cone Losses The field configuration and a hypothetical particle trajectory through a belt cusp are shown in Figure 5.8. Because the magnetic field lines that exit the cusp-like field reconnect to the confinement region within the coils, plasma particles that exit through the belt cusp loss cone will recirculate back into the confinement region. This recirculation significantly increases the confinement time verses that of a simple cusp devise, leading to a favorable concept. The linear scaling of an MCSA fusion device with plasma radius, as well as successful operations of multiple units in the array, is in large part controlled by this recirculation effect. ..._ l I II \, /: : I~- .._Ir . I ~ \ /..r'" . • ,· _,,,.-"" Recirculation .icle Figure 5.8. Diagram of Belt-Cu,sp Fields and Particle Recirculation UNCLASSIFIED/ /FOR OFFiiiIAk W&lii OPtkY 57