共查询到20条相似文献,搜索用时 62 毫秒
1.
中国散裂中子源(CSNS)是基于强流质子加速器的大科学装置,通过高功率质子束流轰击重金属靶产生高通量中子用于开展中子散射研究,CSNS是世界上第四台、发展中国家第一台脉冲型散裂中子源。CSNS包括高功率强流质子加速器、中子靶站和中子谱仪以及相应的配套设施等。加速器由80 MeV负氢直线加速器、1.6 GeV快循环同步加速器及相应的束流输运线组成。CSNS加速器是我国第一台中高能强流高功率质子加速器,本文将介绍CSNS加速器的设计、关键技术、设备研制以及束流调试过程和其中关键问题。 相似文献
2.
作为中国原子能科学研究院四大工程之一的串列加速器升级工程,将成为在我国核科学技术领域开展国防、基础和应用的创新性与先导研究的平台。作为其中的重要组成部分,100MeV强流质子回旋加速器建成后能够提供75~100MeV的质子束流。此回旋加速器建成后,首先利用束流调试管道和束流收集器进行加速器调试,然后根据不同应用的要求,将调试好的束流通过ISOL系统质子管道、同位素研制质子管道、准单能中子源质子管道、白光中子源质子管道、生物医学研究质子管道、单粒子效应质子管道等将质子束传输到各终端用户使用。 相似文献
3.
4.
针对一台用于加速器驱动洁净核能源系统研究、高占空比的强流质子加速器,开展强流质子加速器时序控制系统的研究工作.强流质子加速器时序控制系统提供加速器开机运行过程中所需要的触发信号和时钟信号,该系统的准确性和稳定性对于整个直线加速器的正常运行有重要的影响.介绍了基于ALTERA公司Cyclone Ⅲ系列FPGA串口通信硬件... 相似文献
5.
中国散裂中子源(CSNS)是基于强流质子加速器的大科学装置,通过高功率质子束流轰击重金属靶产生高通量中子用于开展中子散射研究,CSNS是世界上第四台、发展中国家第一台脉冲型散裂中子源。CSNS包括高功率强流质子加速器、中子靶站和中子谱仪以及相应的配套设施等。加速器由80 MeV负氢直线加速器、1.6 GeV快循环同步加速器及相应的束流输运线组成。CSNS加速器是我国第一台中高能强流高功率质子加速器,本文将介绍CSNS加速器的设计、关键技术、设备研制以及束流调试过程和其中关键问题。 相似文献
6.
7.
8.
100MeV强流回旋加速器要求引出质子束流强达到200μA,并计划提供脉冲束流。为达到高的平均流强,并具有提供脉冲束的能力,轴向注入系统的设计有两种方案,即对应于1#和2#注入线,如图1所示。 相似文献
9.
注入系统是中国散裂中子源(CSNS)加速器的核心组成部分,对束流功率提升和稳定供束运行具有重要意义。注入束流损失是快循环同步加速器(RCS)能否在高功率下运行的决定因素之一。本文首先研究CSNS加速器注入束流损失的主要来源,包括注入参数不匹配、注入方式选择、剥离膜散射粒子损失、未被剥离的粒子损失等。其次,根据加速器的束流调节进程,对不同来源的束流损失进行调节和优化,降低注入束流损失,提高注入效率。最后,总结注入束流损失调节结果,初步测量得到注入效率约99%,并对进一步降低注入束流损失、提高注入效率提出改进方法和意见。 相似文献
10.
11.
12.
13.
先进裂变核能的关键核数据测量和CSNS白光中子源 总被引:1,自引:1,他引:0
在设计加速器驱动的次临界系统(ADS)、核废料嬗变装置及钍基熔盐堆时亟需一些关键核数据,当前核数据库受实验条件或中子能区的限制,存在核数据精度不高甚至少部分核素数据缺失的情况。本文综述了国内外相关的核数据研究和相应的白光中子源情况。基于中国散裂中子源(CSNS)的反角通道白光中子源实验终端的中子束流具有非常宽的能谱(0.01 eV~200 MeV)和很好的时间特性。模拟得到距靶80 m处的实验终端的中子注量率为9.3×106cm-2•s-1,1 eV ~ 1 MeV能量间隔内的中子数占总中子数的53%;同时,加速器运行在双束团模式或单束团模式,时间分辨率均在0.3%~0.9%之间,适合开展核数据测量。 相似文献
14.
《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2011,269(24):3251-3257
A few years ago, the neutron time-of-flight facility n_TOF was built at CERN to address some of the urgent needs of high-accuracy nuclear data for Accelerator Driven Systems and other advanced nuclear energy systems, as well as for nuclear astrophysics and fundamental nuclear physics. Thanks to the characteristics of the neutron beam, and to state-of-the-art detection and acquisition systems, high quality neutron cross-section data have been obtained for a variety of isotopes, many of which radioactive. Following an important upgrade of the spallation target and of the experimental area, a new measurement campaign has started last year. After a brief review of the most important results obtained so far at n_TOF, the new features of the facility are presented, together with the first results on the commissioning of the neutron beam. The plans for future measurements, in particular related to nuclear technology are finally discussed. 相似文献
15.
散裂中子源靶站和中子散射谱仪的概念设计 总被引:5,自引:0,他引:5
本文介绍了可应用于多学科应用的散裂中子源(CSNS)靶站和中子散射谱仪概念设计的进展。CSNS靶站将由重水冷却多片钨靶,铍/铁反射体和铁/重混凝土生物屏蔽体组成。采用三个WING型慢化器:水(室温),液体甲烷(100K)和液体氢(20K),设有18个水平中子孔道。MonteCarlo模拟显示优化的靶截面高宽比为1:2.5左右。额定的100kW核功率的质子束轰击后,慢化器处钨靶溢出的脉冲中子通量约为2.4×1016cm?2·s?1。有限元方法计算表明,钨靶体内的总发热量是47kJ/s。即使使用截面较小的钨靶,在通常的水冷速率下,靶体温度也仅略高于90°C。靶体的热应力形变最大不超过0.2mm。根据经济实用原则选择建造粉末衍射仪、小角散射仪、反射仪及直接几何非弹性散射仪等四类有代表性的中子散射谱仪,就能覆盖>80%的中子散射研究领域。 相似文献
16.
Hiroyuki Kogawa Takashi Wakui Takashi Naoe Katsuhiro Haga Hiroshi Takada Masatoshi Futakawa 《Journal of Nuclear Science and Technology》2020,57(5):487-494
ABSTRACTNeutron flux per pulse reached world record at neutron source in Japan Proton Accelerator Research Complex (J-PARC). In the J-PARC, mercury target system is used as a spallation neutron source. A target vessel has a multi-walled protection system that comprises a mercury vessel enclosed with a double-walled water shroud. This is to prevent the leakage of the mercury outside the target vessel. The multi-walled structure needed to be complicated with a lot of welding lines. However, during the operation, we faced an unscheduled shutdown due to water leakage to the intermediate layer between the mercury vessel and water shroud. An investigation on the cause of the leakage was carried out. It is deduced that the leakage path was formed due to the crack propagation from welding defects that are caused by the complicated multi-walled structure. The crack propagation is attributed to the repeated stress by pressure waves generated in the mercury target. Based on the investigation results, the design was improved to remove the welding line on the complicated structure and to realize the stable operation with 1 MW proton beam, which is the final design value of the neutron source in J-PARC. 相似文献
17.
中国先进研究堆冷中子源核发热和冷中子增益研究 总被引:3,自引:3,他引:0
为准确计算和研究中国先进研究堆(CARR)冷中子源装置氢系统的核发热和冷中子增益,建立了一整套计算方法。对参考堆的验证计算证明了该方法的正确性和有效性。对影响CARR冷中子源核发热和冷中子增益的各种因素(如慢化剂、冷包材料、冷包形状等)进行了计算和优化选择。结果表明:在核发热量较小的条件下获得了较好的冷中子增益。 相似文献
18.
The dense Z-pinch (DZP) is one of the earliest and simplest plasma heating and confinement schemes. Recent experimental advances based on plasma initiation from hair-like (10s m in radius) solid hydrogen filaments have so far not encountered the usually devastating MHD instabilities that plagued early DZP experimenters. These encouraging results along with the debut of a number of proof-of principle, high-current (1–2 MA in 10–100 ns) experiments have prompted consideration of the DZP as a pulsed source of DT fusion neutrons of sufficient strength (S
N
1019 n/s) to provide uncollided neutron fluxes in excess ofI
w
= 5–10 MW/m2 over test volumes of 10–30 liters or greater. While this neutron source would be pulsed (100s ns pulse widths, 10–100 Hz pulse rate), giving flux time compressions in the range 105–106, its simplicity, near-term feasibility, low cost, high-Q operation, and relevance to fusion systems thatmay provide a pulsed commercial end-product, e.g., inertial confinement or the DZP itself, together create the impetus for preliminary consideration as a neutron source for fusion nuclear technology and materials testings. The results of a preliminary parametric systems study (focusing primarily on physics issues), conceptual design, and cost vs. performance analyses are presented. The DZP promises an inexpensive and efficient means to provide pulsed DT neutrons at an average rate in excess of 1019 n/s, with neutron currents Iw10 MW/m2 over volumes Vexp 30 liter using single-pulse technologies that differ little from those being used in present-day experiments.Work supported by U.S. DOE. 相似文献
19.
20.
设计了用于非弹性散射谱和俘获谱测量的时间、幅度可调离子源脉冲电源。采用单端正激式结构和软开关技术,逆变输出高压脉冲,占空比从0.1~0.5可调,最小脉宽8μs。目前该脉冲电源已成功应用于煤质快速分析仪中,测量精度明显优于直流方式。 相似文献