JP2019179025A - Collision type nuclear fusion reactor - Google Patents
Collision type nuclear fusion reactor Download PDFInfo
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- JP2019179025A JP2019179025A JP2019022194A JP2019022194A JP2019179025A JP 2019179025 A JP2019179025 A JP 2019179025A JP 2019022194 A JP2019022194 A JP 2019022194A JP 2019022194 A JP2019022194 A JP 2019022194A JP 2019179025 A JP2019179025 A JP 2019179025A
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E30/00—Energy generation of nuclear origin
- Y02E30/10—Nuclear fusion reactors
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Abstract
【課題】燃料の供給と圧縮を加速機で行うことで球対称性が確保され核融合の点火を可能とし、保管された燃料から装填及び点火に至るまでを短時間で行う核融合炉を提供する。【解決手段】加速機を複数台使い、加速機から同時発射された物体は炉中心部で衝突する。加速機1の弾体の頭部に燃料球9を取り付け、2,3,4加速機は弾体のみとする。衝突前に加熱エネルギーを照射し、衝突による弾帯頭部の変形により一定時間封じ込め、均等に球状圧縮され点火に至る。【選択図】図2An object of the present invention is to provide a fusion reactor in which spherical symmetry is ensured by performing fuel supply and compression by an accelerator to enable ignition of fusion, and from storage of fuel to loading and ignition in a short time. I do. A plurality of accelerators are used, and objects simultaneously fired from the accelerator collide at the furnace center. The fuel ball 9 is attached to the head of the ram of the accelerator 1, and the 2, 3, and 4 accelerators are only the ram. Irradiation of heating energy before the collision, the confinement of the head of the band due to the collision for a certain period of time, uniform spherical compression, leading to ignition. [Selection] Figure 2
Description
本発明は、特開2018−137986号公報の加速機を利用し物体の速度と質量による衝突力で核融合反応を点火させる技術に関するものである。 The present invention relates to a technique for igniting a nuclear fusion reaction with a collision force caused by the velocity and mass of an object using an accelerator disclosed in Japanese Patent Application Laid-Open No. 2018-137986.
図1a及びbは、炉体11の炉心10に向かって加速機1,2,3,4を等間隔で配置する。図2aは加速器の配置図であり、正三角錐の4頂点から中心点に向かう線上に加速機を4台設置する。加速機の性能は同一とする。 In FIGS. 1 a and b, accelerators 1, 2, 3, and 4 are arranged at equal intervals toward the core 10 of the furnace body 11. FIG. 2A is an arrangement diagram of accelerators, and four accelerators are installed on a line from the four apexes of the equilateral triangular pyramid toward the center point. The performance of the accelerator is the same.
図2bは加速機から発射する弾体の形状であり、図1の5,6,7,8はすべて同一である。弾体の構造は、図2b13の磁性体部と14の衝突時に燃料球を包み込む最適の物質が接続される。先端部15の形状は、衝突の瞬時における密閉性を確保するため120度の角度とする。弾体は発射後に姿勢のねじれが少し発生するため、工夫が必要である。 FIG. 2b shows the shape of the projectile launched from the accelerator, and 5, 6, 7 and 8 in FIG. 1 are all the same. As for the structure of the bullet body, an optimum substance that wraps the fuel ball at the time of a collision between the magnetic body portion and the magnetic body portion in FIG. The shape of the tip portion 15 is set to an angle of 120 degrees in order to ensure the sealing property at the moment of collision. The projectile needs to be devised because it slightly twists its posture after launch.
図2cは加速機1に装填する弾体5の形状であり、図2bの弾体に重水素等の燃料球9を取り付ける。最適保存温度で保管し、発射の直前に加速器1に装填する。 FIG. 2c shows the shape of the bullet 5 loaded in the accelerator 1, and a fuel ball 9 such as deuterium is attached to the bullet shown in FIG. 2b. Store at optimal storage temperature and load into Accelerator 1 just prior to launch.
図3aは、衝突前における熱エネルギー照射器12の位置図である。熱エネルギーの照射角度は、加速機1の弾道線上16から30度以内とする。 FIG. 3a is a position diagram of the thermal energy irradiator 12 before the collision. The irradiation angle of the thermal energy is within 16 degrees from 16 on the trajectory line of the accelerator 1.
図3bは、衝突時における瞬時の弾頭部変形図である。4個の弾体は、衝突により13、14が変形し燃料球を封じ込め4軸のテトラポット状になり燃料球は中心に圧縮及び縮小され点火に至る。 FIG. 3b is an instantaneous warhead deformation diagram at the time of collision. The four bullets 13 and 14 are deformed by a collision, contain the fuel ball, become a 4-axis tetrapot shape, and the fuel ball is compressed and contracted at the center to reach ignition.
解決しようとする問題点は、燃料の圧縮密度と過熱時間の相関関係を改善し、燃料の保存と扱いを簡易にすること、点火後の燃料供給機構と出力制御も加速機で行い、炉の全体構成の簡素化、費用の削減など多岐にわたる。既存技術の問題点を改善し新たな核融合炉を提供することを課題とする。 The problem to be solved is to improve the correlation between the compression density of the fuel and the overheating time, simplify the storage and handling of the fuel, perform the fuel supply mechanism and power control after ignition with the accelerator, There are various aspects such as simplification of overall configuration and cost reduction. The problem is to improve the problems of existing technology and provide a new fusion reactor.
加速機による物質の速度と質量により、衝突エネルギーを最大限に利用し燃料を圧縮し縮小点火させる技術であり、照射熱との相関関係を最適に調整することが可能であることを特徴とする。 It is a technology that compresses fuel and ignites by using the collision energy to the maximum by the speed and mass of the substance by the accelerator, and it is possible to optimally adjust the correlation with irradiation heat .
炉の全体構成は簡素小型であり、早期に実証炉及び実用炉の実現が望める。構造において燃料供給から点火までの行程を簡易及び確実に行い、核融合反応の点火と継続を実現できる。 The entire structure of the furnace is simple and small, and it is hoped that a demonstration furnace and a practical furnace will be realized at an early stage. In the structure, the process from fuel supply to ignition can be performed easily and reliably, and the ignition and continuation of the fusion reaction can be realized.
発電炉及び溶鉱炉、地域暖房熱源として利用でき、化石燃料の大幅削減が可能であり地球環境の改善に寄与できる It can be used as a power generation furnace, blast furnace, and district heating heat source, which can greatly reduce fossil fuels and contribute to the improvement of the global environment.
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| JP2019022194A JP2019179025A (en) | 2019-02-11 | 2019-02-11 | Collision type nuclear fusion reactor |
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| JP2019022194A JP2019179025A (en) | 2019-02-11 | 2019-02-11 | Collision type nuclear fusion reactor |
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Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2011080523A2 (en) * | 2010-01-04 | 2011-07-07 | Colin Jack | Method of providing impact in vacuum |
| JP2015081914A (en) * | 2013-10-21 | 2015-04-27 | 實 藤原 | Target pulse collision type nuclear fusion reactor |
| JP2015129735A (en) * | 2013-01-29 | 2015-07-16 | 長浦 善昭 | Using a semiconductor laser as an igniting means for self-ignition conditions of a fusion power generation reactor that uses D-He3 or B11-p as a fusion fuel and does not emit any neutrons, using a laser beam or a semiconductor laser A fusion power reactor that performs self-ignition. |
| JP2018137986A (en) * | 2018-04-04 | 2018-08-30 | 正一 砂畑 | Accelerator |
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Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2011080523A2 (en) * | 2010-01-04 | 2011-07-07 | Colin Jack | Method of providing impact in vacuum |
| JP2015129735A (en) * | 2013-01-29 | 2015-07-16 | 長浦 善昭 | Using a semiconductor laser as an igniting means for self-ignition conditions of a fusion power generation reactor that uses D-He3 or B11-p as a fusion fuel and does not emit any neutrons, using a laser beam or a semiconductor laser A fusion power reactor that performs self-ignition. |
| JP2015081914A (en) * | 2013-10-21 | 2015-04-27 | 實 藤原 | Target pulse collision type nuclear fusion reactor |
| JP2018137986A (en) * | 2018-04-04 | 2018-08-30 | 正一 砂畑 | Accelerator |
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