[go: up one dir, main page]

CN115144886B - High-throughput neutron dose assessment method and device - Google Patents

High-throughput neutron dose assessment method and device Download PDF

Info

Publication number
CN115144886B
CN115144886B CN202211077060.4A CN202211077060A CN115144886B CN 115144886 B CN115144886 B CN 115144886B CN 202211077060 A CN202211077060 A CN 202211077060A CN 115144886 B CN115144886 B CN 115144886B
Authority
CN
China
Prior art keywords
neutron
human body
organ
digital model
abdomen
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN202211077060.4A
Other languages
Chinese (zh)
Other versions
CN115144886A (en
Inventor
张晓敏
许旭
宁静
谢向东
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Academy of Military Medical Sciences AMMS of PLA
Original Assignee
Academy of Military Medical Sciences AMMS of PLA
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Academy of Military Medical Sciences AMMS of PLA filed Critical Academy of Military Medical Sciences AMMS of PLA
Priority to CN202211077060.4A priority Critical patent/CN115144886B/en
Publication of CN115144886A publication Critical patent/CN115144886A/en
Application granted granted Critical
Publication of CN115144886B publication Critical patent/CN115144886B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/02Dosimeters
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T3/00Measuring neutron radiation
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Data Mining & Analysis (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Molecular Biology (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Theoretical Computer Science (AREA)
  • Mathematical Physics (AREA)
  • Health & Medical Sciences (AREA)
  • Mathematical Optimization (AREA)
  • Mathematical Analysis (AREA)
  • Computational Mathematics (AREA)
  • Pure & Applied Mathematics (AREA)
  • Databases & Information Systems (AREA)
  • Software Systems (AREA)
  • General Engineering & Computer Science (AREA)
  • Algebra (AREA)
  • Radiation-Therapy Devices (AREA)

Abstract

本发明涉及核应急医学救援领域,提供一种高通量中子剂量评估方法及装置,通过提前进行中子剂量到周围剂量当量率的转换计算,在评估人体受照中子剂量时,不需要利用能谱仪对人体24Na的比活度进行测量,而只需利用辐射巡测仪在几秒钟时间内测量人体腹部位置的周围剂量当量率,就能实现对一个人员中子剂量的初步判断和评估;相比传统方法,本发明极大地节省了中子剂量评估的时间,尤其适用于核灾难后大批量人员需要进行中子剂量评估与筛查的场景。

Figure 202211077060

The invention relates to the field of nuclear emergency medical rescue, and provides a high-throughput neutron dose assessment method and device. By performing the conversion calculation from the neutron dose to the surrounding dose equivalent rate in advance, when evaluating the neutron dose of the human body, no The energy spectrometer is used to measure the specific activity of 24 Na in the human body, and the preliminary neutron dose of a person can be realized only by using the radiation survey instrument to measure the surrounding dose equivalent rate at the abdomen position of the human body within a few seconds. Judgment and assessment: Compared with traditional methods, the present invention greatly saves the time for neutron dose assessment, and is especially suitable for scenarios where a large number of personnel need to perform neutron dose assessment and screening after a nuclear disaster.

Figure 202211077060

Description

高通量中子剂量评估方法及装置High-throughput neutron dose assessment method and device

技术领域technical field

本发明涉及核应急医学救援领域,涉及一种高通量中子剂量评估方法及装置。The invention relates to the field of nuclear emergency medical rescue, and relates to a high-throughput neutron dose assessment method and device.

背景技术Background technique

在核爆与核事故中,中子外照射是人体辐射的重要来源。因此,当人员受到核辐射后,及时准确地对中子外照射剂量进行评估,对于伤员医学处置以及事故危害程度评估都具有重要的价值。尤其是在核灾难事件发生的场景中,有大批量人员受到中子照射,需要在尽可能短的时间内,完成大批量人员受中子照射程度严重程度的评估,然后按照评估的严重程度进行针对性救治,以达到科学分配医疗资源,避免发生医疗资源挤兑的目的。In nuclear explosions and nuclear accidents, neutron external exposure is an important source of human radiation. Therefore, when personnel are exposed to nuclear radiation, timely and accurate assessment of neutron external exposure dose is of great value for the medical treatment of the wounded and the assessment of the degree of accident hazard. Especially in the scenario of a nuclear disaster, a large number of people are exposed to neutrons, and it is necessary to complete the assessment of the severity of the neutron exposure of a large number of people in the shortest possible time, and then proceed according to the severity of the assessment. Targeted treatment, in order to achieve the scientific allocation of medical resources, to avoid the purpose of running out of medical resources.

现有技术中通常利用中子与人体23Na元素反应产生的24Na的多少来判断中子剂量大小。但是,存在的弊端如下:In the prior art, the amount of 24 Na produced by the reaction of neutrons and 23 Na elements in the human body is usually used to judge the neutron dose. However, the disadvantages are as follows:

1)需要对人体24Na含量进行测量与分析,流程复杂,单个人员测量可能需要数十分钟,耗费时间长;1) It is necessary to measure and analyze the 24 Na content of the human body, the process is complicated, and the measurement of a single person may take tens of minutes, which is time-consuming;

2)测量技术难度较高,需要检测人员具有较丰富的专业知识;2) The measurement technology is difficult and requires the inspectors to have rich professional knowledge;

3)测量需要用到价格昂贵的能谱仪。3) The measurement requires an expensive energy spectrometer.

因此,亟需一种测量效率高的高通量中子剂量评估方法。Therefore, there is an urgent need for a high-throughput neutron dose assessment method with high measurement efficiency.

发明内容Contents of the invention

本发明提供一种高通量中子剂量评估方法、装置及电子设备,只需利用简单的便携式辐射巡测仪,通过测量受辐射人群的体内由中子照射后产生的24Na感生放射性强弱,来快速反映中子剂量的大小,进而实现对大批量人员受中子照射的严重程度进行快速判断的技术效果。The present invention provides a high-throughput neutron dose assessment method, device and electronic equipment, which only need to use a simple portable radiation survey instrument to measure the 24 Na-induced radioactive intensity produced by neutron irradiation in the body of the irradiated population. Weakness, to quickly reflect the size of the neutron dose, and then achieve the technical effect of quickly judging the severity of a large number of personnel exposed to neutrons.

为实现上述目的,本发明提供的一种高通量中子剂量评估方法,方法包括:In order to achieve the above object, the present invention provides a high-throughput neutron dose assessment method, the method comprising:

利用辐射测量仪测量待检测人员的距离人体腹部设定距离处的周围剂量当量率;Use a radiation measuring instrument to measure the surrounding dose equivalent rate of the person to be detected at a set distance from the abdomen of the human body;

根据待检测人员受中子照射结束时间至接受辐射测量仪测量时间的间隔时间和预获取的中子照射结束时刻距离人体数字模型腹部设定距离处的周围剂量当量率,获取间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率;Acquire the distance corresponding to the interval time according to the interval time from the end time of neutron irradiation to the measurement time of the radiation measuring instrument and the pre-acquired surrounding dose equivalent rate at the set distance from the abdomen of the digital model of the human body at the end time of neutron irradiation Ambient dose equivalent rate at a set distance from the abdomen of the digital human model;

根据间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率和距离人体腹部设定距离处的实际测量的周围剂量当量率,判定待检测人员的中子剂量是否大于中子剂量限制值;其中,Determine whether the neutron dose of the person to be detected is greater than the neutron dose limit according to the surrounding dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time and the actually measured surrounding dose equivalent rate at the set distance from the abdomen of the human body value; where,

当距离人体腹部设定距离处实际测量的周围剂量当量率大于间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率时,判定待检测人员的中子剂量大于中子剂量限制值。When the actual measured ambient dose equivalent rate at the set distance from the abdomen of the human body is greater than the ambient dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time, it is determined that the neutron dose of the person to be detected is greater than the neutron dose limit value .

进一步,优选的,距离人体数字模型腹部设定距离处的周围剂量当量率的获取方法,包括,Further, preferably, the method for obtaining the surrounding dose equivalent rate at a set distance from the abdomen of the digital human body model includes,

利用预设的人体断层图像数据集建立人体数字模型,并获取每个器官组织的像素数量;Use the preset human body tomographic image data set to establish a digital model of the human body, and obtain the number of pixels of each organ tissue;

为人体数字模型的各个器官组织赋予相应的元素组成和密度值,并根据密度值确定每个器官组织质量;Assign corresponding element composition and density value to each organ tissue of the digital human body model, and determine the mass of each organ tissue according to the density value;

获取每个器官组织的23Na质量百分比,进而根据每个器官组织的23Na质量百分比、器官组织质量以及阿伏伽德罗常数获得人体数字模型中每个器官组织的23Na原子个数;Obtain the 23 Na mass percentage of each organ tissue, and then obtain the 23 Na atom number of each organ tissue in the digital model of the human body according to the 23 Na mass percentage of each organ tissue, the organ tissue mass and Avogadro constant;

利用粒子输运模拟程序,获取能量为E、不同照射几何方式下的单能中子在人体数字模型中每个器官组织内的中子注量,并根据人体数字模型中每个器官组织的中子注量和23Na原子个数,获取单位注量单能中子外照射情况下人体数字模型中每个器官组织的24Na产额;Use the particle transport simulation program to obtain the neutron fluence of monoenergetic neutrons in each organ and tissue in the human body digital model under the energy E and different irradiation geometric modes, and according to the neutron fluence of each organ tissue in the human body digital model The sub-fluence and the number of 23 Na atoms, to obtain the 24 Na output of each organ and tissue in the digital model of the human body under the condition of single-energy neutron external irradiation of unit fluence;

利用粒子输运模拟程序,将各个器官组织设置为光子源,将能量为E、不同照射几何方式下的单能中子在人体数字模型中每个器官组织内的24Na产额设置为各个器官组织的光子源的光子抽样概率,建立具有24Na含量分布的人体光子源模型;Using the particle transport simulation program, set each organ and tissue as a photon source, and set the 24 Na yield in each organ and tissue of the digital model of the human body under the energy E and different irradiation geometry as each organ The photon sampling probability of the photon source of the organization, and the establishment of a human body photon source model with 24 Na content distribution;

基于具有24Na含量分布的人体光子源模型,利用粒子输运模拟程序,获取不同照射几何方式下距离人体数字模型腹部设定距离处的光子注量;Based on the photon source model of the human body with 24 Na content distribution, the particle transport simulation program is used to obtain the photon fluence at the set distance from the abdomen of the digital model of the human body under different irradiation geometries;

计算人体中子剂量限值对应的中子注量,并根据人体中子剂量限值对应的中子注量和单位注量单能中子外照射情况下人体数字模型中每个器官组织的24Na产额获取人体中子剂量限值相对应的各个器官产生的24Na活度;Calculate the neutron fluence corresponding to the human neutron dose limit, and according to the neutron fluence corresponding to the human neutron dose limit and the unit fluence single-energy neutron external irradiation 24 Na production obtains the 24 Na activity produced by each organ corresponding to the neutron dose limit of the human body;

根据不同照射几何方式下距离人体数字模型腹部设定距离处的光子注量以及人体中子剂量限值相对应各个器官产生的24Na活度,获取中子照射结束时刻距离人体数字模型腹部设定距离处的周围剂量当量率。According to the photon fluence at the set distance from the abdomen of the digital model of the human body under different irradiation geometric modes and the 24 Na activity produced by each organ corresponding to the neutron dose limit of the human body, the distance from the abdomen of the digital model of the human body to the end time of neutron irradiation is obtained. Ambient dose equivalent rate at distance.

进一步,优选的,利用预设的人体断层图像数据集建立人体数字模型,并获取每个器官组织的像素数量的方法,包括,Further, preferably, the method for establishing a digital model of a human body by using a preset human body tomographic image data set, and obtaining the number of pixels of each organ tissue includes,

从人体断层图像数据集的第一张图像的第1个像素开始,遍历所有人体断层图像的每一个像素的颜色值;Starting from the first pixel of the first image of the human body tomographic image dataset, traverse the color value of each pixel of all human tomographic images;

按照各个器官组织相对应的颜色值Cn(a,b,c),获取每个器官组织的全部像素数;其中, a,b, c分别代表RGB色空间中的红色R、绿色G、蓝色B的整数分量值,且0≤a≤255,0≤b≤255,0≤c≤255;器官组织包括皮肤、骨骼、脑、心脏、肺、肝脏、肾脏、脾、胃、大肠、小肠和肌肉;According to the color value C n (a, b, c) corresponding to each organ tissue, obtain the total number of pixels of each organ tissue; where, a, b, c represent red R, green G, blue Integer component value of color B, and 0≤a≤255, 0≤b≤255, 0≤c≤255; organs and tissues include skin, bone, brain, heart, lung, liver, kidney, spleen, stomach, large intestine, small intestine and muscles;

将每个器官组织的全部像素数进行累加,获得每个器官组织的像素数量PnAll the pixel numbers of each organ tissue are accumulated to obtain the pixel number P n of each organ tissue.

进一步,优选的,根据每个器官组织的23Na质量百分比、器官组织质量以及阿伏伽德罗常数获得人体数字模型中每个器官组织的23Na原子个数,通过以下公式实现:Further, preferably, the number of 23 Na atoms in each organ and tissue in the human body digital model is obtained according to the 23 Na mass percentage of each organ tissue, the mass of the organ tissue and Avogadro's constant, and is realized by the following formula:

Sn=Mn×Yn(Na,p)/23×NA S n =M n ×Y n (N a , p)/23×N A

其中,Sn表示人体数字模型中每个器官组织的23Na原子个数, NA表示阿伏伽德罗常数,Yn(Na,p)表示器官组织的23Na质量百分比;Mn表示器官组织质量;另,Among them, S n represents the number of 23 Na atoms in each organ and tissue in the digital model of the human body, N A represents Avogadro’s constant, Y n (N a , p) represents the mass percentage of 23 Na in the organ and tissue; M n represents organ tissue quality; in addition,

器官组织质量通过以下公式获得:Mn= R×Pn×ρn,n∈(1,2,3…T),T为器官组织的数量,R为人体数字模型的分辨率,Pn为器官组织的像素数量,ρn为每个器官组织的密度。The mass of organs and tissues is obtained by the following formula: M n = R×P n ×ρ n , n∈(1,2,3…T), T is the quantity of organs and tissues, R is the resolution of the human body digital model, and P n is The number of pixels of organ tissue, ρ n is the density of each organ tissue.

进一步,优选的,根据人体数字模型中每个器官组织的中子注量和23Na原子个数,获取单位注量单能中子外照射情况下人体数字模型中每个器官组织的24Na产额,通过以下公式实现,Further, preferably, according to the neutron fluence and the number of 23 Na atoms of each organ and tissue in the digital human body model, obtain the 24 Na production of each organ and tissue in the human body digital model under the condition of unit fluence monoenergetic neutron external irradiation. Amount, realized by the following formula,

Pn(G,E)/Φ(G,E)= Φn(G,E,ε)×σ(ε)×Sn×A Pn (G,E)/Φ(G,E)= Φn (G,E,ε)×σ(ε)× Sn ×A

其中,Pn(G,E)/Φ(G,E)表示单位注量单能中子外照射情况下人体数字模型中每个器官组织的24Na产额; Pn(G,E)表示不同照射几何方式下能量为E的单能中子在各个器官组织产生的24Na原子个数,Φ(G,E)表示不同照射几何方式下能量为E的中子源的注量;Φn(G,E,ε)表示人体数字模型中每个器官组织的中子注量;σ(ε)表示能量为ε的中子与23Na发生俘获反应的截面; Sn 表示人体数字模型中每个器官组织的23Na原子个数; A表示中子源的截面积;另,Among them, P n (G, E)/Φ (G, E) represents the 24 Na output of each organ and tissue in the digital model of the human body under the condition of unit fluence monoenergetic neutron external irradiation; P n (G, E) represents The number of 24 Na atoms produced by monoenergetic neutrons with energy E under different irradiation geometries in various organs and tissues, Φ(G, E) represents the fluence of neutron sources with energy E under different irradiation geometries; Φ n (G, E, ε) represents the neutron fluence of each organ and tissue in the digital human body model; σ(ε) represents the cross-section of the capture reaction between neutrons with energy ε and 23 Na; S n represents each The number of 23 Na atoms in an organ or tissue; A represents the cross-sectional area of the neutron source; in addition,

人体数字模型中每个器官组织的中子注量Φn(G,E,ε)通过以下公式获取:The neutron fluence Φ n (G, E, ε) of each organ tissue in the digital human body model is obtained by the following formula:

Φn(G,E,ε)= Ln/( R×Pn)Φ n (G, E, ε) = L n /( R×P n )

G表示中子外照射几何方式,G∈(LLAT,RLAT,AP,PA,ISO),其中,LLAT表示左侧向照射、RLAT表示右侧向照射、AP表示前向照射、PA表示后向照射、ISO表示各向同性照射;E表示入射到人体的初始单能中子能量,ε表示初始单能中子能量在经过其他器官组织慢化作用后进入到器官组织n的中子能量;Ln表示中子在器官组织内运动径迹长度,R表示人体数字模型的分辨率,Pn为器官组织的像素数量。G represents the geometry of neutron external radiation, G∈(LLAT, RLAT, AP, PA, ISO), where LLAT represents left lateral radiation, RLAT represents right lateral radiation, AP represents forward radiation, and PA represents backward radiation , ISO means isotropic irradiation; E means the initial monoenergetic neutron energy incident to the human body, ε means the neutron energy of the initial monoenergetic neutron energy entering the organ tissue n after being slowed down by other organs and tissues; L n Indicates the length of the neutron movement track in the organ tissue, R indicates the resolution of the digital model of the human body, and P n is the number of pixels in the organ tissue.

进一步,优选的,将各个器官组织设置为光子源的方法,包括,Further, preferably, the method of setting each organ tissue as a photon source includes,

从人体断层图像数据集的第一张图像的第1个像素开始,遍历所有人体断层图像的每一个像素的颜色值;Starting from the first pixel of the first image of the human body tomographic image dataset, traverse the color value of each pixel of all human tomographic images;

筛选颜色值为某个器官组织对应的颜色值的像素,并将像素对应的发射的粒子类型设置为光子,将像素对应的发射粒子的概率设置为单位注量单能中子外照射情况下人体数字模型中某个器官组织的24Na产额Pn(G,E)/Φ(G,E);Screen the pixels whose color value corresponds to the color value of a certain organ tissue, and set the type of emitted particles corresponding to the pixel to photons, and set the probability of emitted particles corresponding to the pixel to unit fluence in the case of single-energy neutron external irradiation of the human body 24Na production P n (G, E)/Φ (G, E) of a certain organ tissue in the digital model;

遍历人体断层图像数据集的所有图像的所有像素,完成各个器官组织的光子源设置;其中,各个器官组织光子源中的光子能量设置为1.369MeV与2.754MeV。Traversing all the pixels of all the images in the human body tomographic image data set, complete the photon source setting of each organ tissue; wherein, the photon energy in the photon source of each organ tissue is set to 1.369MeV and 2.754MeV.

进一步,优选的,距离人体数字模型腹部设定距离为辐射测量仪垂直于腹部表面检测时辐射测量仪与待检测人员的腹部的距离d,5 cm≤d≤30 cm。Further, preferably, the set distance from the abdomen of the digital human body model is the distance d between the radiation measuring instrument and the abdomen of the person to be detected when the radiation measuring instrument is perpendicular to the abdomen surface, and 5 cm≤d≤30 cm.

进一步,优选的,间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率通过以下公式获取,Further, preferably, the surrounding dose equivalent rate corresponding to the interval time at a set distance from the abdomen of the digital human body model is obtained by the following formula,

Figure DEST_PATH_IMAGE001
Figure DEST_PATH_IMAGE001

其中,H*(G,E)表示间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率,H´(G,E)表示中子照射结束时刻的距离人体数字模型腹部设定距离处的周围剂量当量率,e为常数,T为24Na的半衰期;另,Among them, H * (G, E) represents the surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model corresponding to the interval time, and H´(G, E) represents the distance from the abdomen setting of the digital human body model at the end of neutron irradiation The surrounding dose equivalent rate at the distance, e is a constant, and T is the half-life of 24 Na; in addition,

中子照射结束时刻距离人体数字模型腹部设定距离处的周围剂量当量率H´(G,E)通过以下公式获取,The surrounding dose equivalent rate H´(G,E) at the set distance from the abdomen of the digital model of the human body at the end of neutron irradiation is obtained by the following formula,

Figure 100002_DEST_PATH_IMAGE002
Figure 100002_DEST_PATH_IMAGE002

Φd(G,L)表示不同照射几何方式下距离人体数字模型腹部设定距离处的光子注 量,

Figure DEST_PATH_IMAGE003
表示人体中子剂量限值相对应各个器官产生的24Na活度,
Figure 100002_DEST_PATH_IMAGE004
表示 对所有器官的24Na活度累加后获得的人体24Na总活度;F(G,E)表示单能光子单位注量-周围 剂量当量转换系数。Φ d (G, L) represents the photon fluence at a set distance from the abdomen of the digital human body model under different irradiation geometries,
Figure DEST_PATH_IMAGE003
Indicates that the human neutron dose limit corresponds to the 24 Na activity produced by each organ,
Figure 100002_DEST_PATH_IMAGE004
Indicates the total 24 Na activity of the human body obtained after summing up the 24 Na activities of all organs; F(G, E) indicates the conversion coefficient of monoenergetic photon unit fluence-surrounding dose equivalent.

为了解决上述问题,本发明还提供一种高通量中子剂量评估装置,装置包括,In order to solve the above problems, the present invention also provides a high-throughput neutron dose assessment device, which includes:

辐射测量仪测量模块,用于利用辐射测量仪测量待检测人员的距离人体腹部设定距离处的周围剂量当量率;The radiation measuring instrument measurement module is used to measure the surrounding dose equivalent rate at the set distance from the abdomen of the human body of the person to be detected by using the radiation measuring instrument;

判定阈值获取模块,用于根据待检测人员受中子照射结束时间至接受辐射测量仪测量时间的间隔时间和预获取的中子照射结束时刻距离人体数字模型腹部设定距离处的周围剂量当量率,获取间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率;The judgment threshold acquisition module is used to obtain the surrounding dose equivalent rate at the set distance from the abdomen of the digital model of the human body according to the interval time between the end time of the neutron irradiation of the person to be detected and the measurement time of the radiation measuring instrument and the pre-acquired neutron irradiation end time. , to obtain the surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model corresponding to the interval time;

判定模块,用于根据间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率和距离人体腹部设定距离处的实际测量的周围剂量当量率,判定待检测人员的中子剂量是否大于中子剂量限制值;其中,The judging module is used to determine whether the neutron dose of the person to be detected is greater than the neutron dose limit; where,

当距离人体腹部设定距离处的实际测量的周围剂量当量率大于间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率时,判定待检测人员的中子剂量大于中子剂量限制值。When the actual measured ambient dose equivalent rate at the set distance from the abdomen of the human body is greater than the ambient dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time, it is determined that the neutron dose of the person to be detected is greater than the neutron dose limit value.

为了解决上述问题,本发明还提供一种电子设备,所述电子设备包括:In order to solve the above problems, the present invention also provides an electronic device, which includes:

存储器,存储至少一个指令;及a memory storing at least one instruction; and

处理器,执行所述存储器中存储的指令以实现上述的高通量中子剂量评估方法中的步骤。A processor, executing the instructions stored in the memory to implement the steps in the above-mentioned high-throughput neutron dose assessment method.

本发明的高通量中子剂量评估方法、装置及电子设备具有的有益效果如下,The beneficial effects of the high-throughput neutron dose assessment method, device and electronic equipment of the present invention are as follows,

1)由于提前进行了中子剂量到周围剂量当量率的转换计算,在评估人体受照中子剂量时,不需要利用能谱仪对人体24Na的比活度进行测量,而只需利用辐射巡测仪在几秒钟时间内测量人体腹部位置的周围剂量当量率,就能实现对一个人员中子剂量的初步判断和评估;相比传统方法,本发明极大地节省了中子剂量评估的时间,尤其适用于核灾难后大批量人员需要进行中子剂量评估与筛查的场景;1) Due to the calculation of the conversion from neutron dose to ambient dose equivalent rate in advance, when evaluating the neutron dose to the human body, it is not necessary to use the energy spectrometer to measure the specific activity of 24 Na in the human body, but only need to use radiation The survey instrument measures the surrounding dose equivalent rate of the abdomen position of the human body in a few seconds, and can realize the preliminary judgment and evaluation of the neutron dose of a person; compared with the traditional method, the present invention greatly saves the cost of neutron dose assessment. Time, especially suitable for scenarios where a large number of personnel need to undergo neutron dose assessment and screening after a nuclear disaster;

2)本发明的中子剂量评估方法快捷方便,表现在辐射巡测仪功能简单,可以由非专业人士进行操作,因此可以配置大量人员进行中子剂量评估和筛查工作,相比传统方法需要专业人士操作的掣肘,该方法实现了高通量筛查,大幅提高了中子剂量评估效率,具有非常重要的社会和经济效益。2) The neutron dose assessment method of the present invention is quick and convenient, and the radiation survey instrument has simple functions and can be operated by non-professionals. Therefore, a large number of personnel can be allocated to carry out neutron dose assessment and screening work, which requires more than traditional methods. This method realizes high-throughput screening, greatly improves the efficiency of neutron dose assessment, and has very important social and economic benefits.

3)相较于现有技术中使用能谱仪进行中子剂量评估,本发明采用的是价格便宜的便携式辐射巡测仪,可以大量配置,进而在降低检测成本的基础上大大提高了检测效率。3) Compared with the neutron dose assessment using the energy spectrometer in the prior art, the present invention uses a cheap portable radiation survey instrument, which can be configured in large quantities, thereby greatly improving the detection efficiency on the basis of reducing the detection cost .

附图说明Description of drawings

图1为本发明一实施例提供的高通量中子剂量评估方法的流程示意图;Fig. 1 is a schematic flow chart of a high-throughput neutron dose assessment method provided by an embodiment of the present invention;

图2为本发明一实施例提供的粒子外照射几何条件原理示意图;Fig. 2 is a schematic diagram of the principle of particle external irradiation geometric conditions provided by an embodiment of the present invention;

图3为本发明一实施例提供利用辐射巡测仪测量人体腹部周围剂量当量率的场景示意图;Fig. 3 is a schematic diagram of a scene in which a radiation survey instrument is used to measure the dose equivalent rate around the abdomen of a human body according to an embodiment of the present invention;

图4为本发明一实施例提供的实现高通量中子剂量评估装置的原理示意图;4 is a schematic diagram of the principle of a high-throughput neutron dose assessment device provided by an embodiment of the present invention;

图5为本发明一实施例提供的实现高通量中子剂量评估方法的电子设备的内部结构示意图;Fig. 5 is a schematic diagram of the internal structure of electronic equipment for implementing a high-throughput neutron dose assessment method provided by an embodiment of the present invention;

本发明目的的实现、功能特点及优点将结合实施例,参照附图做进一步说明。The realization of the purpose of the present invention, functional characteristics and advantages will be further described in conjunction with the embodiments and with reference to the accompanying drawings.

具体实施方式detailed description

应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。It should be understood that the specific embodiments described here are only used to explain the present invention, not to limit the present invention.

参照图1所示,为本发明一实施例提供的高通量中子剂量评估方法的流程示意图。该方法可以由一个装置执行,该装置可以由软件和/或硬件实现。Referring to FIG. 1 , it is a schematic flowchart of a high-throughput neutron dose assessment method provided by an embodiment of the present invention. The method may be performed by a device, and the device may be implemented by software and/or hardware.

在本实施例中,高通量中子剂量评估方法包括步骤S1~S3。In this embodiment, the high-throughput neutron dose assessment method includes steps S1-S3.

S1、利用辐射测量仪测量待检测人员的距离人体腹部设定距离处的周围剂量当量率。S1. Using a radiation measuring instrument to measure the surrounding dose equivalent rate of the person to be detected at a set distance from the abdomen of the human body.

需要说明的是,辐射巡测仪,全称电离辐射巡测仪,一般采用NaI(Tl)晶体或者GM管作为探测器,再配上电子放大线路和报警指示装置,就算作一台电离辐射巡测仪。可以探测一般水平的伽马(γ)辐射。一般在普通本底水平下,若辐射水平增加一倍,常见的辐射巡测仪都可以明确的探测的到。譬如日本核泄漏后,辐射巡测仪是可以测到的。测量单位为uSv/h。It should be noted that the radiation survey instrument, the full name of the ionizing radiation survey instrument, generally uses NaI(T l ) crystal or GM tube as the detector, and is equipped with an electronic amplification circuit and an alarm indicating device, which is regarded as an ionizing radiation survey instrument. meter. Typical levels of gamma (γ) radiation can be detected. Generally, under the normal background level, if the radiation level doubles, common radiation survey instruments can clearly detect it. For example, after the Japanese nuclear leak, the radiation survey instrument can detect it. The unit of measurement is uSv/h.

S2、根据待检测人员受中子照射结束时间至接受辐射测量仪测量时间的间隔时间和预获取的距离人体数字模型腹部设定距离处的周围剂量当量率,获取间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率。S2. According to the interval time from the end of neutron irradiation to the measurement time of the radiation measuring instrument and the pre-acquired surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model, obtain the distance corresponding to the interval time from the digital human body model. Peripheral dose equivalent rate at a set distance from the abdomen.

距离人体数字模型腹部设定距离处的周围剂量当量率的获取方法,包括步骤S21-S28。The method for obtaining the surrounding dose equivalent rate at a set distance from the abdomen of the digital human body model includes steps S21-S28.

S21、利用预设的人体断层图像数据集建立人体数字模型,并获取每个器官组织的像素数量。S21. Establish a digital model of a human body by using a preset human body tomographic image data set, and obtain the number of pixels of each organ tissue.

需要说明的是,需要利用预设的人体断层图像数据集建立人体数字模型,用来代表受到中子外照射的人群。人体断层图像数据集包括人体序列断层图像。人体序列断层图像的数量为k,人体序列断层图像之间的厚度i,且i≤0.2 cm;序列断层图像的像素分辨率为j×j,且j×j≤0.1 cm×0.1 cm。首先要获得质量比较高的人体的序列断层图像;如CT图片、MRI或者彩色解剖图片;需要说明的是,原始断层图像数量为k, k的大小应能够包括人体全身,而不只是身体一部分。然后,对人体的序列断层图像进行预处理,进而生成三维数字模型。数字模型可以为体素模型等;可以但不限制于采用Matlab7.0和Photoshop8.0 图像处理软件处理人体序列断层图片。It should be noted that it is necessary to use the preset human tomographic image data set to establish a digital model of the human body to represent the population subjected to external neutron irradiation. The human tomographic image dataset includes sequential tomographic images of the human body. The number of human body sequence tomographic images is k, the thickness between human body sequence tomographic images is i, and i≤0.2 cm; the pixel resolution of sequence tomographic images is j×j, and j×j≤0.1 cm×0.1 cm. First of all, it is necessary to obtain high-quality sequential tomographic images of the human body; such as CT pictures, MRI or color anatomical pictures; it should be noted that the number of original tomographic images is k, and the size of k should be able to include the whole body of the human body, not just a part of the body. Then, the sequential tomographic images of the human body are preprocessed to generate a three-dimensional digital model. The digital model can be a voxel model, etc.; but not limited to, Matlab7.0 and Photoshop8.0 image processing software can be used to process the sequence tomographic images of the human body.

另外,在建立人体数字模型的过程中,需要分别对断层图像中的器官组织进行识别和分割,需要识别的器官组织至少包括:皮肤、骨骼、脑、心脏、肺、肝脏、肾脏、脾、胃、大肠、小肠、肌肉等主要包含23Na元素的器官,没有识别的组织用肌肉代替。器官组织总数量用T表示。In addition, in the process of establishing the digital model of the human body, it is necessary to identify and segment the organs and tissues in the tomographic images. The organs and tissues that need to be identified include at least: skin, bones, brain, heart, lungs, liver, kidneys, spleen, and stomach Organs that mainly contain 23 Na, such as the large intestine, small intestine, and muscle, and unrecognized tissues were replaced by muscle. The total number of organs and tissues is represented by T.

在对断层图像中的器官组织进行识别和分割后,分别对断层图像中识别出的不同器官组织用不同的颜色进行填充,填充的颜色值为Cn(a,b,c),其中n∈(1,2,3…T),T为器官组织的数量,a,b, c分别代表RGB色空间中的红色R、绿色G、蓝色B的整数分量值,且0≤a≤255,0≤b≤255,0≤c≤255。例如肌肉用颜色值C1(10,79,210)填充,骨骼用颜色值C2(130,0,75)填充。After identifying and segmenting the organs and tissues in the tomographic image, the different organs and tissues identified in the tomographic image are filled with different colors, and the filled color value is C n (a, b, c), where n∈ (1,2,3...T), T is the number of organs and tissues, a, b, c respectively represent the integer component values of red R, green G, and blue B in the RGB color space, and 0≤a≤255, 0≤b≤255, 0≤c≤255. For example muscles are filled with color values C1 (10, 79, 210) and bones are filled with color values C2 (130, 0, 75).

在一个具体的实施例中,利用预设的人体断层图像数据集建立人体数字模型,并获取每个器官组织的像素数量Pn, n∈(1,2,3…T)的方法包括:S211、从人体断层图像数据集的第一张图像的第1个像素开始,遍历所有人体断层图像的每一个像素的颜色值;S212、按照各个器官组织相对应的颜色值Cn(a,b,c),获取每个器官组织的全部像素数;其中,器官组织包括皮肤、骨骼、脑、心脏、肺、肝脏、肾脏、脾、胃、大肠、小肠和肌肉; S113、将每个器官组织的全部像素数进行累加,获得每个器官组织的像素数量Pn。也就是说,如果颜色值属于某个器官组织Cn(a,b,c),则对该器官组织的像素进行累加,直至获得该器官组织的像素数量Pn,然后对每个器官组织均如此操作。In a specific embodiment, the method for establishing a digital model of a human body by using a preset human body tomographic image data set, and obtaining the number of pixels P n of each organ tissue, n∈(1,2,3...T) includes: S211 , starting from the first pixel of the first image of the human body tomographic image data set, traverse the color value of each pixel of all human body tomographic images; S212, according to the color value C n (a, b, c) Obtain the total number of pixels of each organ tissue; wherein, the organ tissue includes skin, bone, brain, heart, lung, liver, kidney, spleen, stomach, large intestine, small intestine, and muscle; S113. All the pixel numbers are accumulated to obtain the pixel number P n of each organ tissue. That is to say, if the color value belongs to a certain organ tissue C n (a, b, c), the pixels of this organ tissue are accumulated until the number of pixels P n of this organ tissue is obtained, and then each organ tissue is Do so.

S22、为人体数字模型的各个器官组织赋予相应的元素组成和密度值,并根据密度值确定每个器官组织质量。也就是说,需要对人体数字模型赋予物理属性。S22. Assign corresponding element composition and density value to each organ tissue of the digital human body model, and determine the mass of each organ tissue according to the density value. In other words, it is necessary to assign physical attributes to the digital model of the human body.

具体地说,对于不同的器官组织,赋予不同的元素组成和密度值。器官组织的元素组成用Yn{(e1,p1),(e2,p2),(e3,p3),…(ei,pi)}表示,其中 n∈(1,2,3…T),ei表示某个化学元素,pi表示该化学元素的质量百分比,且p1+p2+p3…+pi=1。每个器官的密度为ρn,n∈(1,2,3…T)。例如肌肉的物理属性为:Y1{(C,32%),(H,45%),(O,22%),(N,1%)},其密度值为ρ1=1.04 g cm-3;某个器官组织的23Na质量百分比表示为Yn(Na,p)。其中,人体数字模型的元素组成及密度值取自国际辐射单位与测量委员会(ICRU)44及ICRU46号报告。Specifically, for different organ tissues, different element compositions and density values are assigned. The element composition of organ tissue is represented by Y n {(e 1 , p 1 ), (e 2 , p 2 ), (e 3 , p 3 ),…(e i , p i )}, where n∈(1, 2,3...T), e i represents a certain chemical element, p i represents the mass percentage of the chemical element, and p 1 +p 2 +p 3 ...+p i =1. The density of each organ is ρ n , n∈(1, 2, 3...T). For example, the physical properties of muscle are: Y 1 {(C, 32%), (H, 45%), (O, 22%), (N, 1%)}, and its density value is ρ 1 =1.04 g cm - 3 ; The 23 Na mass percentage of a certain organ tissue is expressed as Y n (Na, p). Among them, the elemental composition and density values of the digital model of the human body are taken from the International Commission on Radiation Units and Measurements (ICRU) 44 and ICRU 46 reports.

器官组织质量通过以下公式获得:Mn= R×Pn×ρn,n∈(1,2,3…T),T为器官组织的数量,R为人体数字模型的分辨率,Pn为器官组织的像素数量,ρn为每个器官组织的密度。需要说明的是,R为人体数字模型的分辨率,单位为cm3,其表示为一个小立方体的体积大小,体积越小,分辨率越高;R由所利用的断层图像的像素分辨率和相邻两张断层图像之间的间隔距离决定。The mass of organs and tissues is obtained by the following formula: M n = R×P n ×ρ n , n∈(1,2,3…T), T is the quantity of organs and tissues, R is the resolution of the human body digital model, and P n is The number of pixels of organ tissue, ρ n is the density of each organ tissue. It should be noted that R is the resolution of the digital model of the human body in cm 3 , which is expressed as the volume of a small cube, the smaller the volume, the higher the resolution; R is determined by the pixel resolution of the tomographic image used and The distance between two adjacent tomographic images is determined.

S23、获取每个器官组织的23Na质量百分比,进而根据每个器官组织的23Na质量百分比、器官组织质量以及阿伏伽德罗常数获得人体数字模型中每个器官组织的23Na原子个数。S23. Obtain the 23 Na mass percentage of each organ tissue, and then obtain the 23 Na atom number of each organ tissue in the digital model of the human body according to the 23 Na mass percentage of each organ tissue, the organ tissue mass and Avogadro constant .

根据每个器官组织的23Na质量百分比、器官组织质量以及阿伏伽德罗常数获得人体数字模型中每个器官组织的23Na原子个数,通过以下公式实现:According to the mass percentage of 23 Na in each organ tissue, the mass of the organ tissue and Avogadro's constant, the number of 23 Na atoms in each organ tissue in the digital human body model is obtained through the following formula:

Sn=Mn×Yn(Na,p)/23×NA S n =M n ×Y n (Na,p)/23×N A

其中,Sn表示人体数字模型中每个器官组织的23Na原子个数, n∈(1,2,3…T), NA表示阿伏伽德罗常数,Yn(Na,p)表示器官组织的23Na质量百分比;Mn表示器官组织质量。Among them, S n represents the number of 23 Na atoms in each organ and tissue in the digital model of the human body, n∈(1,2,3…T), N A represents Avogadro’s constant, Y n (Na, p) represents 23Na mass percentage of organ tissue; M n represents mass of organ tissue.

S24、利用粒子输运模拟程序,获取能量为E、不同照射几何方式下的单能中子在人体数字模型中每个器官组织内的中子注量,并根据人体数字模型中每个器官组织的中子注量和23Na原子个数,获取单位注量单能中子外照射情况下人体数字模型中每个器官组织的24Na产额。也就是说,计算单位注量单能中子外照射情况下人体各个器官组织的24Na产额。S24. Use the particle transport simulation program to obtain the neutron fluence of monoenergetic neutrons in each organ and tissue in the digital human body model with energy E and different irradiation geometry, and obtain the neutron fluence of each organ and tissue in the digital human body model The neutron fluence and the number of 23 Na atoms are used to obtain the 24 Na production of each organ and tissue in the digital model of the human body under the condition of monoenergetic neutron external irradiation of unit fluence. That is to say, calculate the 24 Na output of various organs and tissues of the human body under the condition of unit fluence monoenergetic neutron external irradiation.

图2为本发明一实施例提供的粒子外照射几何条件原理示意图;如图2所示,中子外照射几何方式G分别设置为左侧向(LLAT)、右侧向(RLAT)、前向(AP)、后向(PA)、各向同性(ISO)照射,即G∈(LLAT,RLAT,AP,PA,ISO)。Fig. 2 is a schematic diagram of the principle of particle external irradiation geometric conditions provided by an embodiment of the present invention; as shown in Fig. (AP), backward (PA), isotropic (ISO) irradiation, that is, G∈(LLAT, RLAT, AP, PA, ISO).

人体数字模型中每个器官组织的中子注量Φn(G,E,ε)通过以下公式获取:The neutron fluence Φ n (G, E, ε) of each organ tissue in the digital human body model is obtained by the following formula:

Φn(G,E,ε)= Ln/( R×Pn)Φ n (G, E, ε) = L n /( R×P n )

即利用粒子输运模拟程序,计算能量为E、不同照射几何方式下的单个中子在人体每个器官组织内的中子注量Φn(G,E,ε);用进入器官组织n的中子的径迹长度除以器官组织n的体积;G表示中子外照射几何方式,G∈(LLAT,RLAT,AP,PA,ISO),E表示入射到人体的初始单能中子能量,ε表示初始单能中子能量在经过其他器官组织慢化作用后进入到器官组织n的中子能量;Ln表示中子在器官组织内运动径迹长度,R表示人体数字模型的分辨率,Pn为器官组织的像素数量。计算Φn(G,E,ε)的主要思想是跟踪并记录中子在人体某个器官组织n内的运动过程,并计算中子在器官组织内运动径迹长度LnThat is to use the particle transport simulation program to calculate the neutron fluence Φ n (G, E, ε) of a single neutron in each organ and tissue of the human body under the energy E and different irradiation geometric modes; The neutron track length divided by the volume of organ tissue n; G represents the geometrical mode of neutron external irradiation, G∈(LLAT, RLAT, AP, PA, ISO), E represents the initial monoenergetic neutron energy incident on the human body, ε represents the neutron energy of the initial monoenergetic neutron energy entering the organ tissue n after being slowed down by other organs and tissues; L n represents the length of the neutron movement track in the organ tissue, R represents the resolution of the digital model of the human body, P n is the number of pixels of the organ tissue. The main idea of calculating Φ n (G, E, ε) is to track and record the movement process of neutrons in a certain organ tissue n of the human body, and calculate the length L n of the neutron movement track in the organ tissue.

也就是说,如果想获取人体数字模型中每个器官组织的中子注量Φn(G,E,ε),需要先计算中子在器官组织内运动径迹长度Ln;具体方法是:当入射中子i进入某个器官组织n的边界时,记录该中子此刻的状态,用Par(i) (v0,t0)表示,其中v0,t0分别表示进入某个器官组织n边界的中子初始速度、初始时刻;当中子离开某个器官组织n边界时,用Par´(i)(v´,t´)表示该中子此刻的状态,v´,t´分别代表该中子的离开速度、离开时刻;中子在器官组织n内部运动任意时刻的状态表示为Par(i) (v,t)。That is to say, if you want to obtain the neutron fluence Φ n (G, E, ε) of each organ and tissue in the digital model of the human body, you need to calculate the neutron movement track length L n in the organ and tissue first; the specific method is: When the incident neutron i enters the boundary of a certain organ tissue n, record the state of the neutron at the moment, denoted by Par(i) (v 0 , t 0 ), where v 0 , t 0 respectively represent entering a certain organ tissue The initial velocity and initial moment of the neutron at the n boundary; when the neutron leaves the n boundary of an organ or tissue, use Par´(i)(v´, t´) to represent the state of the neutron at the moment, and v´ and t´ respectively represent The neutron's departure velocity and departure time; the state of the neutron at any moment in the movement of the organ tissue n is expressed as Par(i) (v, t).

则Ln计算方法为:Then the calculation method of L n is:

Figure DEST_PATH_IMAGE005
Figure DEST_PATH_IMAGE005

在具体的实施过程中,初始单能中子的能量E分别设置为:0.01、0.015、0.02、0.03、0.04、0.05、0.06、0.08、0.1、0.15、0.2、0.3、0.4、0.5、0.6、0.8、1、2、4、6、8 、10MeV、11MeV、12MeV、13MeV、14MeV、15MeV、16MeV、17MeV、18MeV、19MeV、20MeV,以包括常见的中子能量范围。In the specific implementation process, the energy E of the initial monoenergetic neutrons is respectively set as: 0.01, 0.015, 0.02, 0.03, 0.04, 0.05, 0.06, 0.08, 0.1, 0.15, 0.2, 0.3, 0.4, 0.5, 0.6, 0.8 , 1, 2, 4, 6, 8, 10MeV, 11MeV, 12MeV, 13MeV, 14MeV, 15MeV, 16MeV, 17MeV, 18MeV, 19MeV, 20MeV to cover the common neutron energy range.

最后,根据人体数字模型中每个器官组织的中子注量和23Na原子个数,获取单位注量单能中子外照射情况下人体数字模型中每个器官组织的24Na产额,通过以下公式实现,Finally, according to the neutron fluence and the number of 23 Na atoms in each organ and tissue in the digital model of the human body, the 24 Na output of each organ and tissue in the digital model of the human body is obtained under the condition of monoenergetic neutron external irradiation per unit fluence, through The following formula implements,

Pn(G,E)/Φ(G,E)= Φn(G,E,ε)×σ(ε)×Sn×A Pn (G,E)/Φ(G,E)= Φn (G,E,ε)×σ(ε)× Sn ×A

其中,Pn(G,E)/Φ(G,E)表示单位注量单能中子外照射情况下人体数字模型中每个器官组织的24Na产额;即其意义为不同照射几何方式下能量为E的单位注量中子照射情况下各个器官组织的24Na产额。其中, Pn(G,E)表示不同照射几何方式下能量为E的单能中子在各个器官组织产生的24Na原子个数;Φ(G,E)表示不同照射几何方式下能量为E的中子源的注量;Φn(G,E,ε)表示人体数字模型中每个器官组织的中子注量;σ(ε)表示能量为ε的中子与23Na发生俘获反应的截面; Sn 表示人体数字模型中每个器官组织的23Na原子个数; A表示中子源的截面积,单位是cm2Among them, P n (G, E)/Φ (G, E) represents the 24 Na production of each organ and tissue in the digital model of the human body under the condition of unit fluence monoenergetic neutron external irradiation; that is, it means different irradiation geometry The 24 Na production of each organ and tissue under the neutron irradiation with unit fluence of energy E. Among them, P n (G, E) represents the number of 24 Na atoms produced by monoenergetic neutrons with energy E under different irradiation geometries; Φ(G, E) represents the number of 24 Na atoms with energy E under different irradiation geometries The fluence of the neutron source; Φ n (G, E, ε) represents the neutron fluence of each organ and tissue in the digital model of the human body; Cross-section; S n represents the number of 23 Na atoms in each organ and tissue in the digital model of the human body; A represents the cross-sectional area of the neutron source, in cm 2 .

S25、利用粒子输运模拟程序,将各个器官组织设置为光子源,将能量为E、不同照射几何方式下的单能中子在人体数字模型中每个器官组织内的24Na产额设置为各个器官组织的光子源的光子抽样概率,建立具有24Na含量分布的人体光子源模型。也就是说,利用粒子输运程序,根据步骤S24计算获得的各个器官组织的24Na产额,将人体各个器官组织设置为光子源,各个器官组织光子源的光子抽样概率分别为Pn(G,E)/Φ(G,E)。S25. Using the particle transport simulation program, set each organ and tissue as a photon source, and set the 24 Na yield in each organ and tissue of the human body digital model for monoenergetic neutrons with energy E and different irradiation geometry as The photon sampling probability of the photon sources of various organs and tissues is used to establish a human photon source model with 24 Na content distribution. That is to say, using the particle transport program, according to the 24 Na yield of each organ and tissue calculated in step S24, each organ and tissue of the human body is set as a photon source, and the photon sampling probabilities of each organ and tissue photon source are respectively P n (G ,E)/Φ(G,E).

将各个器官组织设置为光子源的方法,包括:S251、从人体断层图像数据集的第一张图像的第1个像素开始,遍历所有人体断层图像的每一个像素的颜色值;S252、筛选颜色值为某个器官组织对应的颜色值的像素,并将像素对应的发射的粒子类型设置为光子,将像素对应的发射粒子的概率设置为单位注量单能中子外照射情况下人体数字模型中某个器官组织的24Na产额Pn(G,E)/Φ(G,E);即器官组织设置为光子源;S253、遍历人体断层图像数据集的所有图像的所有像素,完成各个器官组织的光子源设置;其中,各个器官组织光子源中的光子能量设置为1.369MeV与2.754MeV,两个能量的抽样比为1:1。The method for setting each organ tissue as a photon source includes: S251, starting from the first pixel of the first image of the human body tomographic image data set, traversing the color value of each pixel of all human tomographic images; S252, screening the color The value is the pixel corresponding to the color value of a certain organ tissue, and the type of emitted particles corresponding to the pixel is set to photon, and the probability of emitting particles corresponding to the pixel is set to the digital model of the human body in the case of single-energy neutron external irradiation The 24 Na yield Pn(G, E)/Φ(G, E) of a certain organ tissue; that is, the organ tissue is set as the photon source; S253, traverse all the pixels of all the images in the human body tomographic image data set, and complete each organ The photon source setting of the tissue; wherein, the photon energy in each organ tissue photon source is set to 1.369MeV and 2.754MeV, and the sampling ratio of the two energies is 1:1.

S26、基于具有24Na含量分布的人体光子源模型,利用粒子输运模拟程序,获取不同照射几何方式下距离人体数字模型腹部设定距离处的光子注量。S26. Based on the photon source model of the human body with 24 Na content distribution, the particle transport simulation program is used to obtain the photon fluence at a set distance from the abdomen of the digital human body model under different irradiation geometric modes.

首先,计算距离人体数字模型腹部设定距离dcm处的光子注量Φd(G,L),基于步骤S25建立的具有体内24Na含量分布的人体模型,利用粒子输运模拟程序,计算不同照射几何方式下人体模型腹部一定距离d cm处的光子注量,用 Φd(G,L)表示;其意义为人体内24Na衰变产生一个光子在人体模型腹部一定距离d cm处造成的光子注量。其中,G为中子外照射几何方式,G∈(LL,RL,AP,PA,ISO),L表示体内24Na衰变产生的光子出射到体外后的剩余光子能量,L∈(0.01MeV,0.015 MeV,0.02 MeV,0.03 MeV,0.04 MeV,0.05MeV,0.06 MeV,0.08MeV,0.1MeV,0.2MeV,0.3MeV,0.4MeV,0.5MeV,0.6MeV,0.7MeV,0.8MeV,0.9MeV,1MeV,1.5MeV,2MeV,2.5MeV,2.8MeV)。Firstly, calculate the photon fluence Φ d (G, L) at the set distance dcm from the abdomen of the digital human body model, based on the human body model with 24 Na content distribution in the body established in step S25, use the particle transport simulation program to calculate the different irradiation The photon fluence at a certain distance d cm from the abdomen of the mannequin in a geometric manner is represented by Φ d (G, L); its meaning is the photon fluence caused by a photon produced by the decay of 24 Na in the human body at a certain distance d cm from the mannequin abdomen . Among them, G is the geometry of neutron external irradiation, G ∈ (LL, RL, AP, PA, ISO), L represents the remaining photon energy after the photon emitted from the decay of 24 Na in the body, L ∈ (0.01MeV, 0.015 MeV, 0.02 MeV, 0.03 MeV, 0.04 MeV, 0.05MeV, 0.06 MeV, 0.08MeV, 0.1MeV, 0.2MeV, 0.3MeV, 0.4MeV, 0.5MeV, 0.6MeV, 0.7MeV, 0.8MeV, 0.9MeV, 1MeV, 1.5 MeV, 2MeV, 2.5MeV, 2.8MeV).

Φd(G,L)的计算方法为:在腹部一定距离d cm处,设置以d cm为中心点、半径为r的小球体,记录并累加从人体各个方向进入小球体内的光子数Np,则Φd(G,L)= Np/(πr2),r的设置规则为:0.01 cm≤r≤0.05 cm。The calculation method of Φ d (G, L) is: at a certain distance d cm from the abdomen, set a small sphere with d cm as the center point and a radius of r, record and accumulate the number N of photons entering the small sphere from all directions of the human body p , then Φ d (G, L) = N p /(πr 2 ), the setting rule for r is: 0.01 cm≤r≤0.05 cm.

S27、计算人体中子剂量限值对应的中子注量,并根据人体中子剂量限值对应的中子注量和单位注量单能中子外照射情况下人体数字模型中每个器官组织的24Na产额获取人体中子剂量限值相对应各个器官产生的24Na活度。S27. Calculate the neutron fluence corresponding to the neutron dose limit of the human body, and according to the neutron fluence corresponding to the neutron dose limit of the human body and the single-energy neutron external irradiation of the unit fluence, each organ tissue in the digital model of the human body The 24 Na production obtains human neutron dose limits corresponding to the 24 Na activity produced by each organ.

计算人体中子剂量限值H相对应各个器官产生的24Na活度Bn(G,E)。为了快速对大批量人群进行中子受照严重情况进行初步判断和筛查,设置H的范围为:50mSv≤H≤200mSv,此值为中子剂量筛查限值;利用国际放射防护委员会74号(ICRP74)报告提供的单位中子注量-有效剂量转换系数C(G,E),计算中子剂量H对应的中子注量大小,用Φ´(G,E)表示;其中,G∈(LL,RL,AP,PA,ISO),E表示入射到人体的初始单能中子能量;Φ´(G,E)的计算方法为:Φ´(G,E)=H/ C(G,E)。Calculate the human neutron dose limit H corresponding to the 24 Na activity B n (G, E) produced by each organ. In order to quickly conduct preliminary judgment and screening on the severe neutron exposure of a large number of people, the range of H is set to: 50mSv≤H≤200mSv, which is the neutron dose screening limit; (ICRP74) reports the unit neutron fluence-effective dose conversion coefficient C (G, E), calculates the neutron fluence corresponding to the neutron dose H, expressed by Φ´(G, E); where, G∈ (LL, RL, AP, PA, ISO), E represents the initial monoenergetic neutron energy incident on the human body; the calculation method of Φ´(G, E) is: Φ´(G, E)=H/C(G , E).

利用步骤S24计算获得的 24Na产额Pn(G,E)/Φ(G,E),利用以下公式计算H所对应的各个器官的24Na原子数Qn(G,E);Using the 24 Na yield P n (G, E)/Φ (G, E) calculated in step S24, use the following formula to calculate the 24 Na atomic number Q n (G, E) of each organ corresponding to H;

Qn(G,E)= Pn(G,E)/Φ(G,E)×Φ´(G,E)。Qn(G,E)= Pn (G,E)/Φ(G,E)× Φ´ (G,E).

最后,进一步利用以下公式计算人体中子剂量大小H对应的各个器官产生的24Na活度,用Bn(G,E)表示。Finally, further use the following formula to calculate the 24 Na activity produced by each organ corresponding to the neutron dose size H in the human body, expressed by B n (G, E).

Bn(G,E)=0.693/T×Qn(G,E)B n (G, E)=0.693/T×Q n (G, E)

其中,T为24Na的半衰期。Among them, T is the half-life of 24 Na.

S28、根据不同照射几何方式下距离人体数字模型腹部设定距离处的光子注量以及人体中子剂量限值相对应各个器官产生的24Na活度,获取中子照射结束时刻的距离人体数字模型腹部设定距离处的周围剂量当量率。S28. According to the photon fluence at the set distance from the abdomen of the digital model of the human body under different irradiation geometric modes and the neutron dose limit of the human body corresponding to the 24 Na activity produced by each organ, obtain the distance from the digital model of the human body at the end of neutron irradiation Peripheral dose equivalent rate at a set distance from the abdomen.

中子照射结束时刻的距离人体数字模型腹部设定距离处的周围剂量当量率H´(G,E)通过以下公式获取:The surrounding dose equivalent rate H´(G,E) at the set distance from the abdomen of the digital human body model at the end of neutron irradiation is obtained by the following formula:

Figure 350105DEST_PATH_IMAGE002
Figure 350105DEST_PATH_IMAGE002

其中,Φd(G,L)表示不同照射几何方式下距离人体数字模型腹部设定距离dcm处 的光子注量,

Figure 100002_DEST_PATH_IMAGE006
表示人体中子剂量限值相对应各个器官产生的24Na活度,
Figure DEST_PATH_IMAGE007
表示对所有器官的24Na活度累加后获得的人体24Na总活度;F(G,E)表示单 能光子单位注量-周围剂量当量转换系数,该系数取自ICRP74号报告。需要说明的是,由于24Na一次衰变放出2个光子,因此,
Figure 100002_DEST_PATH_IMAGE008
要乘以系数2。 Among them, Φ d (G, L) represents the photon fluence at the set distance dcm from the abdomen of the digital model of the human body under different irradiation geometries,
Figure 100002_DEST_PATH_IMAGE006
Indicates that the human neutron dose limit corresponds to the 24 Na activity produced by each organ,
Figure DEST_PATH_IMAGE007
Indicates the total 24 Na activity of the human body obtained after summing up the 24 Na activities of all organs; F(G, E) indicates the monoenergetic photon unit fluence-surrounding dose equivalent conversion coefficient, which is taken from ICRP74 report. It should be noted that, since 24 Na decays once and emits 2 photons, therefore,
Figure 100002_DEST_PATH_IMAGE008
To be multiplied by a factor of 2.

S3、根据间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率和距离人体腹部设定距离处的实际测量的周围剂量当量率,判定待检测人员的中子剂量是否大于中子剂量限制值;其中,当距离人体腹部设定距离处的实际测量的周围剂量当量率大于间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率时,判定待检测人员的中子剂量大于中子剂量限制值。S3. According to the surrounding dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time and the actually measured surrounding dose equivalent rate at the set distance from the abdomen of the human body, determine whether the neutron dose of the person to be detected is greater than the neutron dose Dose limit value; wherein, when the actual measured ambient dose equivalent rate at the set distance from the abdomen of the human body is greater than the ambient dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time, it is determined that the neutron dose of the person to be detected The dose is greater than the neutron dose limit.

图3为本发明一实施例提供利用辐射巡测仪测量人体腹部周围剂量当量率的场景示意图;如图3所示,利用辐射测量仪测量待检测人员的距离人体腹部设定距离处的周围剂量当量率。距离人体腹部设定距离为辐射测量仪垂直于腹部表面检测时辐射测量仪与待检测人员的腹部的距离d,5 cm≤d≤30 cm。距离。Fig. 3 is a schematic diagram of a scene where a radiation survey instrument is used to measure the dose equivalent rate around the abdomen of a human body according to an embodiment of the present invention; Equivalent rate. The set distance from the abdomen of the human body is the distance d between the radiation measuring instrument and the abdomen of the person to be detected when the radiation measuring instrument is perpendicular to the abdominal surface, and 5 cm≤d≤30 cm. distance.

也就是说,根据待检测人员受中子照射结束时间至接受辐射测量仪测量时间的间隔时间t和距离人体数字模型腹部d cm处的周围剂量当量率H´(G,E),获取间隔时间对应的距离人体数字模型腹部d cm处的周围剂量当量率H*(G,E);根据所述间隔时间对应的距离人体数字模型腹部d cm处的周围剂量当量率H*(G,E)和距离人体腹部d cm 处的实际测量的周围剂量当量率M(G,E),判定所述待检测人员的中子剂量是否大于中子剂量限制值H;其中,当距离人体腹部d cm 处的周围剂量当量率M(G,E)大于间隔时间对应的距离人体数字模型腹部d cm处的周围剂量当量率H*(G,E)时,判定待检测人员的中子剂量大于中子剂量限制值H。That is to say, according to the interval time t from the end of neutron irradiation to the measurement time of the radiation measuring instrument and the surrounding dose equivalent rate H´(G, E) at a distance d cm from the abdomen of the digital model of the human body, the interval time is obtained The corresponding surrounding dose equivalent rate H*(G, E) at the distance d cm from the abdomen of the digital human model; the corresponding surrounding dose equivalent rate H*(G, E) at the distance d cm from the abdomen of the digital human model according to the interval time and the actual measured ambient dose equivalent rate M(G, E) at a distance d cm from the abdomen of the human body, to determine whether the neutron dose of the person to be detected is greater than the neutron dose limit value H; where, when the distance d cm from the abdomen of the human body When the surrounding dose equivalent rate M(G, E) of the corresponding interval time is greater than the surrounding dose equivalent rate H*(G, E) corresponding to the distance d cm from the abdomen of the digital model of the human body, it is determined that the neutron dose of the person to be detected is greater than the neutron dose Limit value H.

假设人员在受中子照射结束后的t秒后进行测量,间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率通过以下公式获取:Assuming that the personnel are measured after t seconds after the end of the neutron irradiation, the surrounding dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time is obtained by the following formula:

Figure DEST_PATH_IMAGE009
Figure DEST_PATH_IMAGE009

其中,H*(G,E)表示间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率,H´(G,E)表示中子照射结束时刻的距离人体数字模型腹部设定距离处的周围剂量当量率,e为常数,其值为2.7183,T为24Na的半衰期。Among them, H * (G, E) represents the surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model corresponding to the interval time, and H´(G, E) represents the distance from the abdomen setting of the digital human body model at the end of neutron irradiation The surrounding dose equivalent rate at distance, e is a constant, its value is 2.7183, T is the half-life of 24 Na.

当M(G,E)≤H*(G,E)时,表示该人员中子剂量≤中子剂量限值H,判断该人员不需要进行医学处置;当M(G,E)>H*(G,E),表示该人员中子剂量>中子剂量限值H,则该人员需要进一步医学处置;由此实现对人员进行快速中子剂量评估与筛查。When M(G,E)≤H*(G,E), it means that the neutron dose of the person is ≤neutron dose limit H, and it is judged that the person does not need medical treatment; when M(G,E)>H* (G, E), indicating that the neutron dose of the person is greater than the neutron dose limit value H, and the person needs further medical treatment; thus, rapid neutron dose assessment and screening of the person can be realized.

需要说明的是,在具体的实施过程中当不能确定受测量人员的中子照射几何方式时,采用ISO照射几何方式。It should be noted that, in the specific implementation process, when the neutron irradiation geometry of the measured person cannot be determined, the ISO irradiation geometry is adopted.

本发明的高通量中子剂量评估方法,由于提前进行了中子剂量到周围剂量当量率的转换计算,在评估人体受照中子剂量时,不需要利用能谱仪对人体24Na的比活度进行测量,而只需利用辐射巡测仪在几秒钟时间内测量人体腹部位置的周围剂量当量率,就能实现对一个人员中子剂量的初步判断和评估;相比传统方法,本发明极大地节省了中子剂量评估的时间,尤其适用于核灾难后大批量人员需要进行中子剂量评估与筛查的场景;本发明的中子剂量评估方法快捷方便,表现在辐射巡测仪功能简单,可以由非专业人士进行操作,因此可以配置大量人员进行中子剂量评估和筛查工作,相比传统方法需要专业人士操作的掣肘,该方法实现了高通量筛查,大幅提高了中子剂量评估效率,具有非常重要的社会和经济效益。相较于现有技术中使用能谱仪进行中子剂量评估,本发明采用的是价格便宜的便携式辐射巡测仪,可以大量配置,进而在降低检测成本的基础上大大提高了检测效率。In the high-throughput neutron dose evaluation method of the present invention, since the conversion calculation of the neutron dose to the surrounding dose equivalent rate is carried out in advance, when evaluating the neutron dose of the human body, it is not necessary to use the ratio of 24 Na to the human body by an energy spectrometer. The neutron dose of a person can be initially judged and evaluated by using a radiation survey instrument to measure the surrounding dose equivalent rate at the abdomen of the human body within a few seconds; compared with the traditional method, this The invention greatly saves the time for neutron dose assessment, and is especially suitable for scenarios where a large number of personnel need to conduct neutron dose assessment and screening after a nuclear disaster; The function is simple and can be operated by non-professionals, so a large number of personnel can be allocated for neutron dose assessment and screening. Compared with traditional methods that require professionals to operate, this method achieves high-throughput screening and greatly improves The efficiency of neutron dose assessment has very important social and economic benefits. Compared with the neutron dose assessment using the energy spectrometer in the prior art, the present invention uses a cheap portable radiation survey instrument, which can be configured in large quantities, thereby greatly improving the detection efficiency on the basis of reducing the detection cost.

如图4所示,本发明提供一种高通量中子剂量评估装置400,本发明可以安装于电子设备中。根据实现的功能,该高通量中子剂量评估装置400可以所述装置包括辐射测量仪测量模块410、判定阈值获取模块420以及判定模块430。本发明所述模块也可以称之为单元,是指一种能够被电子设备处理器所执行,并且能够完成固定功能的一系列计算机程序段,其存储在电子设备的存储器中。As shown in FIG. 4 , the present invention provides a high-throughput neutron dose assessment device 400 , which can be installed in electronic equipment. According to the functions realized, the high-throughput neutron dose assessment device 400 may include a radiometer measurement module 410 , a decision threshold acquisition module 420 and a decision module 430 . The module in the present invention can also be called a unit, which refers to a series of computer program segments that can be executed by the processor of the electronic device and can complete fixed functions, and are stored in the memory of the electronic device.

在本实施例中,关于各模块/单元的功能如下:In this embodiment, the functions of each module/unit are as follows:

辐射测量仪测量模块410,用于利用辐射测量仪测量待检测人员的距离人体腹部设定距离处的周围剂量当量率;The radiation measuring instrument measurement module 410 is used to measure the surrounding dose equivalent rate of the person to be detected at a set distance from the abdomen of the human body by using the radiation measuring instrument;

判定阈值获取模块420,用于根据待检测人员受中子照射结束时间至接受辐射测量仪测量时间的间隔时间和预获取的中子照射结束时刻距离人体数字模型腹部设定距离处的周围剂量当量率,获取间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率;Judgment threshold acquisition module 420, which is used to obtain the surrounding dose equivalent at a set distance from the abdomen of the digital model of the human body according to the interval time between the end time of the neutron irradiation of the person to be detected and the measurement time of the radiation measuring instrument and the pre-acquired neutron irradiation end time Rate, obtain the surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model corresponding to the interval time;

判定模块430,用于根据间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率和距离人体腹部设定距离处的实际测量的周围剂量当量率,判定待检测人员的中子剂量是否大于中子剂量限制值;其中,The determination module 430 is used to determine the neutron dose of the person to be detected according to the surrounding dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time and the actually measured surrounding dose equivalent rate at the set distance from the abdomen of the human body Is it greater than the neutron dose limit value; where,

当距离人体腹部设定距离处的实际测量的周围剂量当量率大于间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率时,判定待检测人员的中子剂量大于中子剂量限制值。When the actual measured ambient dose equivalent rate at the set distance from the abdomen of the human body is greater than the ambient dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time, it is determined that the neutron dose of the person to be detected is greater than the neutron dose limit value.

本发明的高通量中子剂量评估装置400由于提前进行了中子剂量到周围剂量当量率的转换计算,在评估人体受照中子剂量时,不需要利用能谱仪对人体24Na的比活度进行测量,而只需利用辐射巡测仪在几秒钟时间内测量人体腹部位置的周围剂量当量率,就能实现对一个人员中子剂量的初步判断和评估;相比传统方法,本发明极大地节省了中子剂量评估的时间,尤其适用于核灾难后大批量人员需要进行中子剂量评估与筛查的场景;本发明的中子剂量评估方法快捷方便,表现在辐射巡测仪功能简单,可以由非专业人士进行操作,因此可以配置大量人员进行中子剂量评估和筛查工作,相比传统方法需要专业人士操作的掣肘,该方法实现了高通量筛查,大幅提高了中子剂量评估效率,具有非常重要的社会和经济效益。相较于现有技术中使用能谱仪进行中子剂量评估,本发明采用的是价格便宜的便携式辐射巡测仪,可以大量配置,进而在降低检测成本的基础上大大提高了检测效率。Since the high-throughput neutron dose evaluation device 400 of the present invention has carried out the conversion calculation from the neutron dose to the surrounding dose equivalent rate in advance, when evaluating the neutron dose to the human body, it is not necessary to use the ratio of the energy spectrometer to the human body 24 Na The neutron dose of a person can be initially judged and evaluated by using a radiation survey instrument to measure the surrounding dose equivalent rate at the abdomen of the human body within a few seconds; compared with the traditional method, this The invention greatly saves the time for neutron dose assessment, and is especially suitable for scenarios where a large number of personnel need to conduct neutron dose assessment and screening after a nuclear disaster; The function is simple and can be operated by non-professionals, so a large number of personnel can be allocated for neutron dose assessment and screening. Compared with traditional methods that require professionals to operate, this method achieves high-throughput screening and greatly improves The efficiency of neutron dose assessment has very important social and economic benefits. Compared with the neutron dose assessment using the energy spectrometer in the prior art, the present invention uses a cheap portable radiation survey instrument, which can be configured in large quantities, thereby greatly improving the detection efficiency on the basis of reducing the detection cost.

如图5所示,本发明提供一种高通量中子剂量评估方法的电子设备5。As shown in FIG. 5 , the present invention provides an electronic device 5 for a high-throughput neutron dose assessment method.

该电子设备5可以包括处理器50、存储器51和总线,还可以包括存储在存储器51中并可在所述处理器50上运行的计算机程序,如高通量中子剂量评估程序52。The electronic device 5 may include a processor 50 , a memory 51 and a bus, and may also include a computer program stored in the memory 51 and operable on the processor 50 , such as a high-throughput neutron dose assessment program 52 .

其中,所述存储器51至少包括一种类型的可读存储介质,所述可读存储介质包括闪存、移动硬盘、多媒体卡、卡型存储器(例如:SD或DX存储器等)、磁性存储器、磁盘、光盘等。所述存储器51在一些实施例中可以是电子设备3的内部存储单元,例如该电子设备5的移动硬盘。所述存储器31在另一些实施例中也可以是电子设备5的外部存储设备,例如电子设备3上配备的插接式移动硬盘、智能存储卡(Smart Media Card, SMC)、安全数字(SecureDigital, SD)卡、闪存卡(Flash Card)等。进一步地,所述存储器51还可以既包括电子设备5的内部存储单元也包括外部存储设备。所述存储器51不仅可以用于存储安装于电子设备5的应用软件及各类数据,例如高通量中子剂量评估程序的代码等,还可以用于暂时地存储已经输出或者将要输出的数据。Wherein, the memory 51 includes at least one type of readable storage medium, and the readable storage medium includes flash memory, mobile hard disk, multimedia card, card-type memory (for example: SD or DX memory, etc.), magnetic memory, magnetic disk, CD etc. The memory 51 may be an internal storage unit of the electronic device 3 in some embodiments, such as a mobile hard disk of the electronic device 5 . The memory 31 can also be an external storage device of the electronic device 5 in other embodiments, such as a plug-in mobile hard disk equipped on the electronic device 3, a smart memory card (Smart Media Card, SMC), a secure digital (SecureDigital, SD) card, flash memory card (Flash Card), etc. Further, the memory 51 may also include both an internal storage unit of the electronic device 5 and an external storage device. The memory 51 can not only be used to store application software and various data installed in the electronic device 5, such as the code of the high-throughput neutron dose assessment program, but also can be used to temporarily store the data that has been output or will be output.

所述处理器50在一些实施例中可以由集成电路组成,例如可以由单个封装的集成电路所组成,也可以是由多个相同功能或不同功能封装的集成电路所组成,包括一个或者多个中央处理器(Central Processing unit,CPU)、微处理器、数字处理芯片、图形处理器及各种控制芯片的组合等。所述处理器50是所述电子设备的控制核心(Control Unit),利用各种接口和线路连接整个电子设备的各个部件,通过运行或执行存储在所述存储器51内的程序或者模块(例如高通量中子剂量评估程序等),以及调用存储在所述存储器51内的数据,以执行电子设备5的各种功能和处理数据。In some embodiments, the processor 50 may be composed of an integrated circuit, for example, may be composed of a single packaged integrated circuit, or may be composed of multiple integrated circuits with the same function or different functions, including one or more Combination of central processing unit (Central Processing unit, CPU), microprocessor, digital processing chip, graphics processor and various control chips, etc. The processor 50 is the control core (Control Unit) of the electronic device, and uses various interfaces and lines to connect various components of the entire electronic device, and runs or executes programs or modules stored in the memory 51 (such as high Flux neutron dose assessment program, etc.), and call the data stored in the memory 51 to execute various functions of the electronic device 5 and process data.

所述总线可以是外设部件互连标准(peripheral component interconnect,简称PCI)总线或扩展工业标准结构(extended industry standard architecture,简称EISA)总线等。该总线可以分为地址总线、数据总线、控制总线等。所述总线被设置为实现所述存储器51以及至少一个处理器50等之间的连接通信。The bus may be a peripheral component interconnect (PCI for short) bus or an extended industry standard architecture (EISA for short) bus or the like. The bus can be divided into address bus, data bus, control bus and so on. The bus is configured to realize connection and communication between the memory 51 and at least one processor 50 and the like.

图5仅示出了具有部件的电子设备,本领域技术人员可以理解的是,图5示出的结构并不构成对所述电子设备5的限定,可以包括比图示更少或者更多的部件,或者组合某些部件,或者不同的部件布置。Figure 5 only shows an electronic device with components, and those skilled in the art can understand that the structure shown in Figure 5 does not constitute a limitation to the electronic device 5, and may include fewer or more components than those shown in the illustration. components, or combinations of certain components, or different arrangements of components.

例如,尽管未示出,所述电子设备5还可以包括给各个部件供电的电源(比如电池),优选地,电源可以通过电源管理装置与所述至少一个处理器50逻辑相连,从而通过电源管理装置实现充电管理、放电管理、以及功耗管理等功能。电源还可以包括一个或一个以上的直流或交流电源、再充电装置、电源故障检测电路、电源转换器或者逆变器、电源状态指示器等任意组件。所述电子设备3还可以包括多种传感器、蓝牙模块、Wi-Fi模块等,在此不再赘述。For example, although not shown, the electronic device 5 may also include a power supply (such as a battery) for supplying power to various components. Preferably, the power supply may be logically connected to the at least one processor 50 through a power management device, so that through power management The device implements functions such as charge management, discharge management, and power consumption management. The power supply may also include one or more DC or AC power supplies, recharging devices, power failure detection circuits, power converters or inverters, power status indicators and other arbitrary components. The electronic device 3 may also include various sensors, Bluetooth modules, Wi-Fi modules, etc., which will not be repeated here.

进一步地,所述电子设备5还可以包括网络接口,可选地,所述网络接口可以包括有线接口和/或无线接口(如WI-FI接口、蓝牙接口等),通常用于在该电子设备3与其他电子设备之间建立通信连接。Further, the electronic device 5 may also include a network interface. Optionally, the network interface may include a wired interface and/or a wireless interface (such as a WI-FI interface, a Bluetooth interface, etc.), which are usually used in the electronic device 3 Establish a communication connection with other electronic devices.

可选地,该电子设备5还可以包括用户接口,用户接口可以是显示器(Display)、输入单元(比如键盘(Keyboard)),可选地,用户接口还可以是标准的有线接口、无线接口。可选地,在一些实施例中,显示器可以是LED显示器、液晶显示器、触控式液晶显示器以及OLED(Organic Light-Emitting Diode,有机发光二极管)触摸器等。其中,显示器也可以适当的称为显示屏或显示单元,用于显示在电子设备5中处理的信息以及用于显示可视化的用户界面。Optionally, the electronic device 5 may further include a user interface. The user interface may be a display (Display) or an input unit (such as a keyboard (Keyboard)). Optionally, the user interface may also be a standard wired interface or a wireless interface. Optionally, in some embodiments, the display may be an LED display, a liquid crystal display, a touch-sensitive liquid crystal display, an OLED (Organic Light-Emitting Diode, organic light-emitting diode) touch device, and the like. Wherein, the display may also be appropriately referred to as a display screen or a display unit, and is used for displaying information processed in the electronic device 5 and for displaying a visualized user interface.

应该了解,所述实施例仅为说明之用,在专利申请范围上并不受此结构的限制。It should be understood that the embodiments are only for illustration, and are not limited by the structure in terms of the scope of the patent application.

所述电子设备5中的所述存储器51存储的高通量中子剂量评估程序52是多个指令的组合,在所述处理器50中运行时,可以实现:利用辐射测量仪测量待检测人员的距离人体腹部设定距离处的周围剂量当量率;根据待检测人员受中子照射结束时间至接受辐射测量仪测量时间的间隔时间和预获取的距离人体数字模型腹部设定距离处的周围剂量当量率,获取间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率;根据间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率和距离人体腹部设定距离处的实际测量的周围剂量当量率,判定待检测人员的中子剂量是否大于中子剂量限制值;其中,当距离人体腹部设定距离处的实际测量的周围剂量当量率大于间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率时,判定待检测人员的中子剂量大于中子剂量限制值。The high-throughput neutron dose assessment program 52 stored in the memory 51 in the electronic device 5 is a combination of multiple instructions. When running in the processor 50, it can be realized: use a radiation measuring instrument to measure the dose of the person to be detected The surrounding dose equivalent rate at the set distance from the abdomen of the human body; the interval time from the end of neutron irradiation to the measurement time of the radiation measuring instrument and the pre-acquired surrounding dose at the set distance from the abdomen of the digital model of the human body Equivalent rate, obtain the surrounding dose equivalent rate at the set distance from the abdomen of the digital model of the human body corresponding to the interval time; according to the surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model corresponding to the interval time and the set distance from the abdomen of the human body The actual measured ambient dose equivalent rate, to determine whether the neutron dose of the person to be detected is greater than the neutron dose limit value; wherein, when the actual measured ambient dose equivalent rate at the set distance from the abdomen of the human body is greater than the distance corresponding to the interval time When the surrounding dose equivalent rate at the set distance from the abdomen of the digital model is determined, it is determined that the neutron dose of the person to be detected is greater than the neutron dose limit value.

具体地,所述处理器50对上述指令的具体实现方法可参考图1对应实施例中相关步骤的描述,在此不赘述。需要强调的是,为进一步保证上述高通量中子剂量评估程序的私密和安全性,上述数据库可用处理数据存储于本服务器集群所处区块链的节点中。Specifically, for the specific implementation method of the above instructions by the processor 50, reference may be made to the description of relevant steps in the embodiment corresponding to FIG. 1 , and details are not repeated here. It should be emphasized that, in order to further ensure the privacy and security of the above-mentioned high-throughput neutron dose assessment program, the above-mentioned database can store the processed data in the nodes of the blockchain where the server cluster is located.

进一步地,所述电子设备5集成的模块/单元如果以软件功能单元的形式实现并作为独立的产品销售或使用时,可以存储在一个计算机可读取存储介质中。所述计算机可读介质可以包括:能够携带所述计算机程序代码的任何实体或装置、记录介质、U盘、移动硬盘、磁碟、光盘、计算机存储器、只读存储器(ROM,Read-Only Memory)。Further, if the integrated modules/units of the electronic device 5 are realized in the form of software function units and sold or used as independent products, they can be stored in a computer-readable storage medium. The computer readable medium may include: any entity or device capable of carrying the computer program code, recording medium, U disk, removable hard disk, magnetic disk, optical disk, computer memory, read-only memory (ROM, Read-Only Memory) .

本发明实施例还提供一种计算机可读存储介质,所述存储介质可以是非易失性的,也可以是易失性的,所述存储介质存储有计算机程序,所述计算机程序被处理器执行时实现:利用辐射测量仪测量待检测人员的距离人体腹部设定距离处的周围剂量当量率;根据待检测人员受中子照射结束时间至接受辐射测量仪测量时间的间隔时间和预获取的距离人体数字模型腹部设定距离处的周围剂量当量率,获取间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率;根据间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率和距离人体腹部设定距离处的实际测量的周围剂量当量率,判定待检测人员的中子剂量是否大于中子剂量限制值;其中,当距离人体腹部设定距离处的实际测量的周围剂量当量率大于间隔时间对应的距离人体数字模型腹部设定距离处的周围剂量当量率时,判定待检测人员的中子剂量大于中子剂量限制值。An embodiment of the present invention also provides a computer-readable storage medium, the storage medium may be non-volatile or volatile, the storage medium stores a computer program, and the computer program is executed by a processor Timely implementation: use radiation measuring instrument to measure the surrounding dose equivalent rate of the person to be detected at a set distance from the abdomen of the human body; according to the interval time between the end time of the person to be detected being exposed to neutrons and the time of receiving the measurement of the radiation measuring instrument and the pre-acquired distance The surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model is obtained, and the surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model corresponding to the interval time is obtained; the surrounding dose equivalent rate at the set distance from the abdomen of the digital human body model corresponding to the interval time The dose equivalent rate and the actual measured surrounding dose equivalent rate at the set distance from the abdomen of the human body are used to determine whether the neutron dose of the person to be detected is greater than the neutron dose limit value; When the ambient dose equivalent rate is greater than the ambient dose equivalent rate at the set distance from the abdomen of the digital human body model corresponding to the interval, it is determined that the neutron dose of the person to be detected is greater than the neutron dose limit value.

具体地,所述计算机程序被处理器执行时具体实现方法可参考实施例高通量中子剂量评估方法中相关步骤的描述,在此不赘述。Specifically, for the specific implementation method when the computer program is executed by the processor, reference may be made to the description of relevant steps in the high-throughput neutron dose assessment method in the embodiment, and details are not repeated here.

在本发明所提供的几个实施例中,应该理解到,所揭露的设备,装置和方法,可以通过其它的方式实现。例如,以上所描述的装置实施例仅仅是示意性的,例如,所述模块的划分,仅仅为一种逻辑功能划分,实际实现时可以有另外的划分方式。In the several embodiments provided by the present invention, it should be understood that the disclosed devices, devices and methods can be implemented in other ways. For example, the device embodiments described above are only illustrative. For example, the division of the modules is only a logical function division, and there may be other division methods in actual implementation.

所述作为分离部件说明的模块可以是或者也可以不是物理上分开的,作为模块显示的部件可以是或者也可以不是物理单元,即可以位于一个地方,或者也可以分布到多个网络单元上。可以根据实际的需要选择其中的部分或者全部模块来实现本实施例方案的目的。The modules described as separate components may or may not be physically separated, and the components shown as modules may or may not be physical units, that is, they may be located in one place, or may be distributed to multiple network units. Part or all of the modules can be selected according to actual needs to achieve the purpose of the solution of this embodiment.

另外,在本发明各个实施例中的各功能模块可以集成在一个处理单元中,也可以是各个单元单独物理存在,也可以两个或两个以上单元集成在一个单元中。上述集成的单元既可以采用硬件的形式实现,也可以采用硬件加软件功能模块的形式实现。In addition, each functional module in each embodiment of the present invention may be integrated into one processing unit, or each unit may physically exist separately, or two or more units may be integrated into one unit. The above-mentioned integrated units can be implemented in the form of hardware, or in the form of hardware plus software function modules.

对于本领域技术人员而言,显然本发明不限于上述示范性实施例的细节,而且在不背离本发明的精神或基本特征的情况下,能够以其他的具体形式实现本发明。It will be apparent to those skilled in the art that the invention is not limited to the details of the above-described exemplary embodiments, but that the invention can be embodied in other specific forms without departing from the spirit or essential characteristics of the invention.

因此,无论从哪一点来看,均应将实施例看作是示范性的,而且是非限制性的,本发明的范围由所附权利要求而不是上述说明限定,因此旨在将落在权利要求的等同要件的含义和范围内的所有变化涵括在本发明内。不应将权利要求中的任何附关联图标记视为限制所涉及的权利要求。Accordingly, the embodiments should be regarded in all points of view as exemplary and not restrictive, the scope of the invention being defined by the appended claims rather than the foregoing description, and it is therefore intended that the scope of the invention be defined by the appended claims rather than by the foregoing description. All changes within the meaning and range of equivalents of the elements are embraced in the present invention. Any reference sign in a claim should not be construed as limiting the claim concerned.

本发明所指区块链是分布式数据存储、点对点传输、共识机制、加密算法等计算机技术的新型应用模式。区块链(Blockchain),本质上是一个去中心化的数据库,是一串使用密码学方法相关联产生的数据块,每一个数据块中包含了一批次网络交易的信息,用于验证其信息的有效性(防伪)和生成下一个区块。区块链可以包括区块链底层平台、平台产品服务层以及应用服务层等。The block chain referred to in the present invention is a new application mode of computer technologies such as distributed data storage, point-to-point transmission, consensus mechanism, and encryption algorithm. Blockchain (Blockchain), essentially a decentralized database, is a series of data blocks associated with each other using cryptographic methods. Each data block contains a batch of network transaction information, which is used to verify its Validity of information (anti-counterfeiting) and generation of the next block. The blockchain can include the underlying platform of the blockchain, the platform product service layer, and the application service layer.

此外,显然“包括”一词不排除其他单元或步骤,单数不排除复数。装置权利要求中陈述的多个单元或装置也可以由一个单元或装置通过软件或者硬件来实现。第二等词语用来表示名称,而并不表示任何特定的顺序。In addition, it is obvious that the word "comprising" does not exclude other elements or steps, and the singular does not exclude the plural. A plurality of units or means stated in the device claims may also be realized by one unit or device through software or hardware. Secondary terms are used to denote names without implying any particular order.

最后应说明的是,以上实施例仅用以说明本发明的技术方案而非限制,尽管参照较佳实施例对本发明进行了详细说明,本领域的普通技术人员应当理解,可以对本发明的技术方案进行修改或等同替换,而不脱离本发明技术方案的精神和范围。Finally, it should be noted that the above embodiments are only used to illustrate the technical solutions of the present invention without limitation. Although the present invention has been described in detail with reference to the preferred embodiments, those of ordinary skill in the art should understand that the technical solutions of the present invention can be Modifications or equivalent replacements can be made without departing from the spirit and scope of the technical solutions of the present invention.

Claims (9)

1. A high-throughput neutron dose assessment method, characterized in that the method comprises:
measuring the peripheral dose equivalent rate of a person to be detected at a set distance from the abdomen of the human body by using a radiation survey meter;
according to the interval time from the neutron irradiation ending time to the radiation inspection instrument measuring time of a person to be detected and the pre-acquired peripheral dose equivalent rate at the set distance from the neutron irradiation ending time to the human digital model abdomen, acquiring the peripheral dose equivalent rate at the set distance from the human digital model abdomen corresponding to the interval time;
judging whether the neutron dose of the person to be detected is greater than a neutron dose limit value or not according to the peripheral dose equivalent rate at the set distance from the human digital model abdomen corresponding to the interval time and the actually measured peripheral dose equivalent rate at the set distance from the human abdomen; wherein,
when the actually measured peripheral dose equivalent rate at the set distance from the human abdomen is greater than the peripheral dose equivalent rate at the set distance from the human digital model abdomen corresponding to the interval time, determining that the neutron dose of the person to be detected is greater than the neutron dose limit value;
the method for acquiring the peripheral dose equivalent rate at the set distance from the neutron irradiation ending time to the human digital model abdomen comprises the following steps,
establishing a human body digital model by using a preset human body tomography image data set, and acquiring the pixel number of each organ tissue;
assigning corresponding element compositions and density values to the organ tissues of the human digital model, and determining the mass of each organ tissue according to the density values;
obtaining tissue of each organ 23 Na by mass percent, further according to each organ tissue 23 Obtaining Na mass percentage, organ tissue mass and Avogastron constant of each organ tissue in human digital model 23 The number of Na atoms;
obtaining neutron fluence of monoenergetic neutrons under different irradiation geometric modes in each organ tissue in the human digital model with energy of E by using a particle transport simulation program, and obtaining the neutron fluence of the monoenergetic neutrons in each organ tissue in the human digital model according to the neutron fluence sum of each organ tissue in the human digital model 23 The number of Na atoms is obtained, and the number of each organ tissue in the human body digital model under the condition of external irradiation of unit-fluence single-energy neutrons is obtained 24 Na yield;
setting each organ tissue as photon source by utilizing particle transport simulation program, and arranging monoenergetic neutrons with energy of E and different irradiation geometric modes in each organ tissue in human digital model 24 Na yield is set as the photon sampling probability of photon source of each organ tissue, and the Na yield is set to have 24 A human photon source model with Na content distribution;
based on the fact that 24 A human body photon source model with distributed Na content obtains photon fluence at a set distance from the abdomen of the human body digital model in different irradiation geometric modes by utilizing a particle transport simulation program;
calculating neutron fluence corresponding to the neutron dose limit value of the human body, and according to the neutron fluence corresponding to the neutron dose limit value of the human body and the neutron of unit fluence under the condition of external irradiation of single-energy neutrons, determining the neutron fluence of each organ tissue in the human body digital model 24 Obtained by Na yield from each organ corresponding to neutron dose limit in human body 24 Activity of Na;
according to photon fluence at a set distance from the abdomen of the digital phantom under different irradiation geometries and the neutron dose limit value generated by each organ corresponding to the neutron dose limit value 24 And Na activity, namely obtaining the peripheral dose equivalent rate at the set distance from the human digital model abdomen at the neutron irradiation end moment.
2. The high-throughput neutron dose evaluation method of claim 1,
a method for establishing a digital model of a human body using a preset tomographic image data set of the human body and obtaining the number of pixels per organ tissue, comprising,
starting from the 1 st pixel of the first image of the human body tomography image data set, traversing and acquiring the color value of each pixel of all human body tomography images;
color values C corresponding to respective organ tissues n (a, b, c) obtaining the total number of pixels of each organ tissue; wherein a, B and c respectively represent integer component values of red R, green G and blue B in an RGB color space, and a is more than or equal to 0 and less than or equal to 255,0 and less than or equal to B and less than or equal to 255,0 and less than or equal to c and less than or equal to 255; the organ tissue includes skin, bone, brain, heart, lung, liver, kidney, spleen, stomach, large intestine, small intestine, and muscle;
accumulating all the pixel numbers of each organ tissue to obtain the pixel number P of each organ tissue n
3. The high-throughput neutron dose evaluation method of claim 1,
according to the tissue of each organ 23 Obtaining the mass percentage of Na, the mass of the organ tissues and the Avgalois constant of each organ tissue in the human digital model 23 The number of Na atoms is realized by the following formula:
S n =M n ×Y n (N a ,p)/23×N A
wherein S is n Representing each organ tissue in a digital model of the human body 23 Number of Na atoms, N A Denotes the Avogastron constant, Y n (N a P) of organ tissue 23 Na in percentage by mass; m is a group of n Representing organ tissue mass; in addition, the air conditioner is provided with a fan,
the organ tissue mass is obtained by the following formula: m n = R◊P n ◊ρ n N is the number of organ tissues (1,2,3 … T), T is the resolution of the human digital model, and P is the number of organ tissues n Number of pixels of organ tissue, p n Is the density of each organ tissue.
4. The high-throughput neutron dose evaluation method of claim 1,
according to the neutron fluence sum of each organ tissue in the human body digital model 23 The number of Na atoms is obtained, and the number of each organ tissue in the human body digital model under the condition of external irradiation of unit-fluence single-energy neutrons is obtained 24 The Na yield is realized by the following formula,
P n (G,E)/Φ(G,E)= Φ n (G,E,ε)×σ(ε)×S n ×A
wherein, P n (G, E)/phi (G, E) represents the tissue of each organ in the digital human body model under the condition of external irradiation of unit fluence monoenergetic neutrons 24 Na yield; p n (G, E) represents the generation of monoenergetic neutrons with energy E in various organ tissues under different irradiation geometries 24 The number of Na atoms, phi (G, E) represents the fluence of a neutron source with the energy of E under different irradiation geometric modes; phi n (G, E, ε) represents the neutron fluence of each organ tissue in the human digital model; σ (ε) represents the energy of a neutron with ε 23 Cross section where Na capture reaction occurs; s n Representing each organ tissue in a digital model of the human body 23 The number of Na atoms; a represents the cross-sectional area of the neutron source; in addition, the air conditioner is provided with a fan,
neutron fluence phi of each organ tissue in the digital phantom n (G, E, ε) is obtained by the following formula:
Φ n (G,E,ε)= L n /( R×P n )
g represents the out-of-neutron irradiation geometry, G ∈ (LLAT, RLAT, AP, PA, ISO), wherein LLAT represents left lateral irradiation, RLAT represents right lateral irradiation, AP represents forward irradiation, PA represents backward irradiation, and ISO represents isotropic irradiation; e represents the initial monoenergetic neutron energy incident to the human body, and epsilon represents the neutron energy of the initial monoenergetic neutron energy entering the organ tissue n after the moderation of other organ tissues; l is a radical of an alcohol n Representing the length of a neutron's motion track in organ tissue, R representing the digital model of the bodyResolution of type P n The number of pixels of the organ tissue.
5. The high-throughput neutron dose evaluation method of claim 1,
a method of providing individual organ tissues as a photon source, comprising,
starting from the 1 st pixel of the first image of the human body tomography image data set, traversing and acquiring the color value of each pixel of all human body tomography images;
screening pixels with color values corresponding to certain organ tissues, setting the types of emitted particles corresponding to the pixels as photons, and setting the probability of the emitted particles corresponding to the pixels as the probability of certain organ tissues in a human digital model under the condition of unit fluence single energy neutron external irradiation 24 Na yield P n (G,E)/Φ(G,E);
Traversing all pixels of all images of the human body tomographic image data set to complete the photon source setting of each organ tissue; wherein the photon energy in each organ tissue photon source is set to be 1.369MeV and 2.754MeV.
6. The high-throughput neutron dose evaluation method of claim 1,
the distance from the human digital model abdomen is set to be d between the radiation patrol instrument and the abdomen of a person to be detected when the radiation patrol instrument is perpendicular to the abdomen surface for detection, and d is not less than 5 cm and not more than 30 cm.
7. The high-throughput neutron dose evaluation method of claim 1,
the peripheral dose equivalent rate at a set distance from the abdomen of the digital phantom at the interval time is obtained by the following formula,
Figure DEST_PATH_IMAGE002
wherein,H * (G, E) represents the peripheral dose equivalent rate at a set distance from the abdomen of the digital human body model corresponding to the interval time, H ´ (G, E) represents the peripheral dose equivalent rate at a set distance from the abdomen of the digital human body model at the end time of neutron irradiation, E is a constant, and T is a constant 24 Half-life of Na; in addition, the air conditioner is provided with a fan,
the peripheral dose equivalent rate H ´ (G, E) at a set distance from the abdomen of the digital phantom at the end of neutron irradiation is obtained by the following equation,
Figure DEST_PATH_IMAGE004
Φ d (G, L) represents the photon fluence at a set distance from the abdomen of the digital phantom of the human body in different irradiation geometric modes,
Figure DEST_PATH_IMAGE006
indicating production of neutron dose limits in humans for respective organs 24 The activity of the Na is high,
Figure DEST_PATH_IMAGE008
representing for all organs 24 Human body obtained after Na activity accumulation 24 Total activity of Na; f (G, E) represents the conversion coefficient of unit fluence of monoenergetic photons to the surrounding dose equivalent.
8. A high-flux neutron dose evaluation device, characterized in that the device comprises,
the radiation patrol instrument measuring module is used for measuring the peripheral dose equivalent rate of a person to be detected at a set distance from the abdomen of the human body by using the radiation patrol instrument;
the judgment threshold value obtaining module is used for obtaining the peripheral dose equivalent rate at the set distance from the human digital model abdomen corresponding to the interval time according to the interval time from the neutron irradiation ending time of the person to be detected to the radiation inspection instrument measuring time and the pre-obtained peripheral dose equivalent rate at the set distance from the neutron irradiation ending time to the human digital model abdomen; the method for acquiring the peripheral dose equivalent rate at the set distance from the neutron irradiation ending time to the human digital model abdomen comprises the following steps,
establishing a human body digital model by using a preset human body tomography image data set, and acquiring the pixel number of each organ tissue;
assigning corresponding element compositions and density values to the organ tissues of the human digital model, and determining the mass of each organ tissue according to the density values;
obtaining tissue of each organ 23 Percentage by mass of Na, further according to the tissue of each organ 23 Obtaining the mass percentage of Na, the mass of the organ tissues and the Avgalois constant of each organ tissue in the human digital model 23 The number of Na atoms;
obtaining the neutron fluence of the monoenergetic neutrons in each organ tissue in the human digital model under different irradiation geometric modes with the energy of E by utilizing a particle transport simulation program, and obtaining the neutron fluence sum of each organ tissue in the human digital model according to the neutron fluence sum of each organ tissue in the human digital model 23 The number of Na atoms is obtained, and the number of each organ tissue in the human body digital model under the condition of external irradiation of unit-fluence single-energy neutrons is obtained 24 Na yield;
setting each organ tissue as photon source by using particle transport simulation program, and arranging the monoenergetic neutrons with energy of E and different irradiation geometries in each organ tissue in the human digital model 24 Na yield is set as photon sampling probability of photon source of each organ tissue, and Na yield is set to be 24 A human photon source model with Na content distribution;
the judgment module is used for judging whether the neutron dose of the person to be detected is larger than the neutron dose limit value or not according to the peripheral dose equivalent rate at the set distance from the human body digital model abdomen corresponding to the interval time and the actually measured peripheral dose equivalent rate at the set distance from the human body abdomen; wherein,
and when the actually measured peripheral dose equivalent rate at the set distance from the human abdomen is greater than the peripheral dose equivalent rate at the set distance from the human digital model abdomen corresponding to the interval time, judging that the neutron dose of the person to be detected is greater than the neutron dose limit value.
9. An electronic device, characterized in that the electronic device comprises:
at least one processor; and (c) a second step of,
a memory communicatively coupled to the at least one processor; wherein,
the memory stores instructions executable by the at least one processor to enable the at least one processor to perform the steps in the high-throughput neutron dose evaluation method of any of claims 1 to 7.
CN202211077060.4A 2022-09-05 2022-09-05 High-throughput neutron dose assessment method and device Active CN115144886B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202211077060.4A CN115144886B (en) 2022-09-05 2022-09-05 High-throughput neutron dose assessment method and device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202211077060.4A CN115144886B (en) 2022-09-05 2022-09-05 High-throughput neutron dose assessment method and device

Publications (2)

Publication Number Publication Date
CN115144886A CN115144886A (en) 2022-10-04
CN115144886B true CN115144886B (en) 2023-01-06

Family

ID=83416252

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202211077060.4A Active CN115144886B (en) 2022-09-05 2022-09-05 High-throughput neutron dose assessment method and device

Country Status (1)

Country Link
CN (1) CN115144886B (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2017009393A (en) * 2015-06-19 2017-01-12 株式会社東芝 Neutron measurement device, neutron measurement method, and treatment apparatus for boron neutron capture therapy
CN108121005A (en) * 2017-12-05 2018-06-05 清华大学 Utilize the method and neutron dose rate instrument of bromination cerium detector measurement neutron dose rate

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
IT201900009741A1 (en) * 2019-06-21 2020-12-21 Istituto Naz Fisica Nucleare Personal wearable dosimeter for neutrons
CN112882082B (en) * 2021-01-12 2022-03-29 中国人民解放军海军工程大学 Measurement Method of Neutron-γ Surrounding Dose Equivalent Rate Meter Based on Pulse Shape Discrimination
CN113420491B (en) * 2021-08-24 2021-12-17 中国人民解放军军事科学院军事医学研究院 Evaluation method of radiation dose to organs of experimental animals under external particle irradiation

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2017009393A (en) * 2015-06-19 2017-01-12 株式会社東芝 Neutron measurement device, neutron measurement method, and treatment apparatus for boron neutron capture therapy
CN108121005A (en) * 2017-12-05 2018-06-05 清华大学 Utilize the method and neutron dose rate instrument of bromination cerium detector measurement neutron dose rate

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
Activation analysis of patients and establishment of release criteria following boron neutron capture therapy at Tsing Hua Open-Pool Reactor;Chien-Hsuan Chan 等;《Radiation Physics and Chemistry》;20220814;第198卷;第110226页 *
中子周围剂量当量(率)监测方法的研究;李桃生;《中国优秀博硕士学位论文全文数据库 (博士)工程科技Ⅱ辑》;20050615(第02期);C040-11 *

Also Published As

Publication number Publication date
CN115144886A (en) 2022-10-04

Similar Documents

Publication Publication Date Title
Fattibene et al. The 4th international comparison on EPR dosimetry with tooth enamel: Part 1: Report on the results
CN113420491B (en) Evaluation method of radiation dose to organs of experimental animals under external particle irradiation
Koshkareva et al. Predictive accuracy of first post‐treatment PET/CT in HPV‐related oropharyngeal squamous cell carcinoma
Khatonabadi et al. A comparison of methods to estimate organ doses in CT when utilizing approximations to the tube current modulation function
Fedon et al. Internal breast dosimetry in mammography: Monte Carlo validation in homogeneous and anthropomorphic breast phantoms with a clinical mammography system
Qiu et al. Reproducibility of radiomic features with GrowCut and GraphCut semiautomatic tumor segmentation in hepatocellular carcinoma
Rafat Motavalli et al. Pulmonary embolism in pregnant patients: assessing organ dose to pregnant phantom and its fetus during lung imaging
Son et al. Proof‐of‐concept prototype time‐of‐flight PET system based on high‐quantum‐efficiency multianode PMT s
CN114707416A (en) A kind of human body radiation dose detection method, device, system and computer equipment
CN115144886B (en) High-throughput neutron dose assessment method and device
Vrba et al. EURADOS intercomparison exercise on MC modelling for the in-vivo monitoring of AM-241 in skull phantoms (Part II and III).
Li et al. Current pediatric administered activity guidelines for 99mTc‐DMSA SPECT based on patient weight do not provide the same task‐based image quality
Bolch et al. Guidance on the use of handheld survey meters for radiological triage: time-dependent detector count rates corresponding to 50, 250, and 500 mSv effective dose for adult males and adult females
Rault et al. Fast simulation of yttrium‐90 bremsstrahlung photons with GATE
Stone Measurement of f
Kundel et al. Reliability of soft-copy versus hard-copy interpretation of emergency department radiographs: a prototype study
CN114966797A (en) Human Neutron Dose Assessment Method and System
Chen et al. Interpretation of diagnosis of occupational radiation skin diseases
Hardy et al. Reference dataset for benchmarking fetal doses derived from Monte Carlo simulations of CT exams
CN117930322B (en) Neutron dose assessment method and device based on blood sodium 24 specific activity
CN116051954A (en) Image detection model training method, image detection method, device and medium
Chen et al. Enhancing positronium lifetime imaging through two-component reconstruction in time-of-flight positron emission tomography
Mathieu et al. Precision of dosimetry‐related measurements obtained on current multidetector computed tomography scanners
Abadi et al. AAPM Truth‐based CT (TrueCT) reconstruction grand challenge
Staton et al. Organ and effective doses in infants undergoing upper gastrointestinal (UGI) fluoroscopic examination

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant