Proceedings of the 61\textsuperscript{st} ICFA ABDW on High-Intensity and High-Brightness Hadron Beams 2018
DOI: 10.18429/jacow-hb2018-wep1wb02
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Beam Dynamics Simulation and Measurements for the IFMIF/EVEDA Project

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“…A goal of 𝑡 𝑝 = 3600 s is set for giant fusion sources, while 𝑡 𝑝 2 × 10 4 s (about one working day) was repeatedly achieved in NIO1. A fusion plant will require a 20 year operation (or more), that is a BOT of 𝑡 𝑏 6 × 10 8 s, while an ambitious practical goal for a compact test source is an integrated beam time per year about 2 × 10 6 s. Even with this large scaling factor, a compact test installation can give useful experience on beam scattering damages, ion back-streaming, while material fatigue is actively studied in the so-called broader approach [5]. On the other end of time scales, we have the 20 ms period of the 50 Hz power supply and beam ripple (with harmonics) contributing to fatigue, the typical pulse length (in the order of one minute), and the observed evolution of transients in NIO1 (ten minutes).…”
Section: Introductionmentioning
confidence: 99%
“…A goal of 𝑡 𝑝 = 3600 s is set for giant fusion sources, while 𝑡 𝑝 2 × 10 4 s (about one working day) was repeatedly achieved in NIO1. A fusion plant will require a 20 year operation (or more), that is a BOT of 𝑡 𝑏 6 × 10 8 s, while an ambitious practical goal for a compact test source is an integrated beam time per year about 2 × 10 6 s. Even with this large scaling factor, a compact test installation can give useful experience on beam scattering damages, ion back-streaming, while material fatigue is actively studied in the so-called broader approach [5]. On the other end of time scales, we have the 20 ms period of the 50 Hz power supply and beam ripple (with harmonics) contributing to fatigue, the typical pulse length (in the order of one minute), and the observed evolution of transients in NIO1 (ten minutes).…”
Section: Introductionmentioning
confidence: 99%