2009
DOI: 10.1088/0029-5515/49/7/075017
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Concept of magnet systems for LHD-type reactor

Abstract: Heliotron reactors have attractive features for fusion power plants, such as no need for current drive and a wide space between the helical coils for the maintenance of in-vessel components. Their main disadvantage was considered the necessarily large size of their magnet systems. According to the recent reactor studies based on the experimental results in the Large Helical Device, the major radius of plasma of 14 to 17 m with a central toroidal field of 6 to 4 T is needed to attain the self-ignition condition… Show more

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Cited by 36 publications
(21 citation statements)
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“…For FFHR, the ∼40-m diameter helical coils are required [1,2]. There are three options for the superconductor selection: the cable-in-conduit (CIC) conductor using lowtemperature superconducting (LTS) strands such as Nb 3 Al or Nb 3 Sn [3], the indirectly-cooled solid-type conductor using LTS [4] and the indirectly-cooled solid-type conductor using high-temperature superconductors (HTS) represented by YBCO [5][6][7][8]. Presently, the well-established LTS conductors are being used in fusion devices like the Large Helical Device (LHD), and this could be the primary option for the FFHR magnet.…”
Section: Introductionmentioning
confidence: 99%
“…For FFHR, the ∼40-m diameter helical coils are required [1,2]. There are three options for the superconductor selection: the cable-in-conduit (CIC) conductor using lowtemperature superconducting (LTS) strands such as Nb 3 Al or Nb 3 Sn [3], the indirectly-cooled solid-type conductor using LTS [4] and the indirectly-cooled solid-type conductor using high-temperature superconductors (HTS) represented by YBCO [5][6][7][8]. Presently, the well-established LTS conductors are being used in fusion devices like the Large Helical Device (LHD), and this could be the primary option for the FFHR magnet.…”
Section: Introductionmentioning
confidence: 99%
“…The present design, FFHR-d1, is equipped with a pair of continuously wound helical coils, having a major radius of 15.6 m, a minor radius of 3.744 m and a helical pitch number of 10, that produce a 4.7 T toroidal magnetic field to generate 3 GW of fusion power [13]. The stored magnetic energy is 160 GJ and a 100-kA conductor is required to be used at the maximum magnetic field of ∼12 T. The primary selection for the helical windings is a CIC conductor using Nb 3 Al strands [14], which is regarded as an extension of the ITER technology. However, considering the difficulties related to CIC conductors, such as the complicated plumbing required and the degradation of the critical current due to strain, an indirectly-cooled LTS conductor using Nb 3 Sn strands and an aluminum-alloy jacket has also been considered [15].…”
Section: Design Of a 100-ka-class Hts Conductor For DC Magnets Of Fusmentioning
confidence: 99%
“…The winding pack consists of 390 turns of HTS conductors, each with an operation current of 94 kA, installed in a stainless-steel "internal plate" with circular grooves. This is the same concept employed for the CIC conductor version of the FFHR helical coils [14]. The internal plate is the layer winding version of the "radial plate" used in the ITER TF coils with pancake winding.…”
Section: Design Of a 100-ka-class Hts Conductor For DC Magnets Of Fusmentioning
confidence: 99%
“…A stored magnetic energy W mag is an index of the total mass amount of the superconducting magnet system including the supporting structure. The superconducting magnet system with W mag = 120-140 GJ can be constructed with a small extension of the ITER-relevant technology [4] and the achievable maximum value is estimated to be ∼160 GJ. Therefore, W mag ≤ 160 GJ is assumed in the design of FFHR-2m2.…”
Section: Design Window Of a Lhd-type Heliotron Reactormentioning
confidence: 99%