Linear induction accelerator: Difference between revisions

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'''Linear induction accelerators''' utilize ferrite-loaded, non-resonant [[Electromagnetic_inductionElectromagnetic induction|magnetic induction]] cavities. Each cavity can be thought of as two large washer-shaped disks connected by an outer cylindrical tube. Between the disks is a ferrite toroid. A voltage pulse applied between the two disks causes an increasing magnetic field which inductively couples power into the charged particle beam.<ref>
{{cite book
|last=Humphries |first=Stanley
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|chapter=Linear Induction Accelerators
|title=Principles of Charged Particle Acceleration
|pages=283–325
|page=283-325
|publisher=[[Wiley-Interscience]]
|isbn=978-0471878780
}}</ref>
 
The linear induction accelerator was invented by Christofilos in the 1960's. <ref>
{{cite book
|last1=Christofilos |first1=N.C.
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|url=http://inspirehep.net/record/918919/files/HEACC63_II_785-791.pdf
|title=Proceedings, 4th International Conference on High-Energy Accelerators (HEACC63)
|pages=1482–1488
|page=1482-1488
}}</ref> Linear induction accelerators are capable of accelerating very high beam currents (>1000 A) in a single short pulse. They have been used to generate X-rays for flash radiography (e.g. [[Dual-Axis_Radiographic_Hydrodynamic_Test_FacilityAxis Radiographic Hydrodynamic Test Facility|DARHT]] at [[LANL]]), and have been considered as particle injectors for [[magnetic confinement fusion]] and as drivers for [[free electron laser]]s. A compact version of a linear induction accelerator, the [[dielectric wall accelerator]], has been proposed as a proton accelerator for medical [[proton therapy]].
 
==References==
{{Reflist}}
 
{{Uncategorized|date=June 2016}}