CN108363089B - Method and device for rapid determination of radon precipitation rate - Google Patents
Method and device for rapid determination of radon precipitation rate Download PDFInfo
- Publication number
- CN108363089B CN108363089B CN201810123413.7A CN201810123413A CN108363089B CN 108363089 B CN108363089 B CN 108363089B CN 201810123413 A CN201810123413 A CN 201810123413A CN 108363089 B CN108363089 B CN 108363089B
- Authority
- CN
- China
- Prior art keywords
- radon
- chamber
- measurement period
- measuring
- concentration
- 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.)
- Expired - Fee Related
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/16—Measuring radiation intensity
- G01T1/167—Measuring radioactive content of objects, e.g. contamination
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- High Energy & Nuclear Physics (AREA)
- Molecular Biology (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Measurement Of Radiation (AREA)
Abstract
Description
技术领域technical field
本发明涉及核辐射探测技术领域,特别涉及一种氡析出率快速定值方法和装置。The invention relates to the technical field of nuclear radiation detection, in particular to a method and a device for rapid determination of radon precipitation rate.
背景技术Background technique
测量介质表面氡析出率常用的方法是累积法,即用一个集氡室紧扣在介质表面,测量一段时间内析出到集氡室内的氡,就可反推出氡析出率。氡析出率定值过程的快慢主要取决于氡浓度测量过程的快慢。The commonly used method for measuring the radon precipitation rate on the medium surface is the accumulation method, that is, a radon collecting chamber is tightly fastened to the medium surface, and the radon precipitation rate can be deduced by measuring the radon precipitated into the radon collecting chamber within a period of time. The speed of the radon precipitation rate determination process mainly depends on the speed of the radon concentration measurement process.
中国专利文献CN105425267A公开了一种氡析出率的测量方法,该方法在测量氡浓度时,需要先开启取样泵抽取被测环境中含氡空气一段时间,此时仪器测量室内的氡浓度即为初始时刻t=0时集氡室内的氡浓度(环境氡浓度),再将一集氡室扣在被测介质表面上开始集氡,再将密闭测量室通过2根硅胶管与集氡室连接形成一个回路,当收集一定时间后,再开启取样泵将集氡室与测量室内的氡混合一段时间,使得集氡室与测量室内氡浓度达到平衡,此时可以认为测量室内的氡浓度即为集氡室的氡浓度,接着再以T(大于10min)为一个周期反复测量,即可测得一系列等时间间隔的集氡室内氡浓度数据。实际上,当前在采用累积法测氡析出率的过程中,测量氡浓度的方法基本与上述文献中介绍的方式类似,均是采用管子将集氡室与测量室连接成一个回路,测量过程中,先将集氡室与测量室内的空气混合一段时间,以实现集氡室与测量室内氡浓度平衡,再以T为测量周期对氡浓度进行测量,由于测量过程中不断有氡析出,集氡室内氡浓度会逐渐升高,为保证测量结果的准确性,在每次以T为周期进行测量之前都需要将集氡室与测量室内的氡混合平衡一次,频繁的混合平衡过程将导致氡浓度定值过程耗时偏长,从而影响了氡析出率的定值速度。Chinese patent document CN105425267A discloses a method for measuring the radon precipitation rate. When measuring the radon concentration, the method needs to turn on the sampling pump to extract the radon-containing air in the measured environment for a period of time. At this time, the radon concentration in the measuring room of the instrument is the initial At time t=0, the radon concentration in the radon collection chamber (environmental radon concentration) is collected, and then a collection radon chamber is buckled on the surface of the measured medium to start radon collection, and then the closed measurement chamber is connected with the radon collection chamber through two silicone tubes to form In a loop, after collecting for a certain period of time, turn on the sampling pump to mix the radon in the collecting chamber with the radon in the measuring chamber for a period of time, so that the radon concentration in the collecting chamber and the measuring chamber reaches equilibrium. The radon concentration in the radon room is then measured repeatedly with T (greater than 10min) as a cycle, and a series of radon concentration data in the radon room can be measured at equal time intervals. In fact, in the process of measuring the radon precipitation rate by the cumulative method, the method of measuring the radon concentration is basically similar to the method described in the above-mentioned literature, which is to use a pipe to connect the radon collecting chamber and the measuring chamber into a loop. , first mix the air in the collecting room and the measuring room for a period of time to realize the balance of the radon concentration in the collecting room and the measuring room, and then measure the radon concentration with T as the measurement period. The indoor radon concentration will gradually increase. In order to ensure the accuracy of the measurement results, it is necessary to mix and balance the radon in the collecting chamber and the measuring chamber once before each measurement with T as the cycle. The frequent mixing and balancing process will lead to the concentration of radon. The setting process takes a long time, which affects the setting speed of the radon precipitation rate.
发明内容SUMMARY OF THE INVENTION
本发明要解决的技术问题是提供一种氡析出率快速定值方法,该方法在对测量氡浓度时无需混合平衡的过程,对氡析出率的定值速度较快。The technical problem to be solved by the present invention is to provide a rapid method for determining the radon precipitation rate, which does not require a process of mixing and balancing when measuring the radon concentration, and can quickly determine the radon precipitation rate.
为了解决上述技术问题,本发明采用如下技术方案:一种氡析出率快速定值方法,包括以下步骤:In order to solve the above-mentioned technical problems, the present invention adopts the following technical solutions: a method for rapidly setting a radon precipitation rate, comprising the following steps:
步骤一、快速跟踪测量变化的氡浓度;Step 1. Quickly track and measure the changing radon concentration;
利用插值法对变化的氡浓度进行等效:先对环境本底进行测量,得到环境氡浓度C0,完成环境本底测量后开始集氡,集氡过程中以T为测量周期,在第n个测量周期结束时的氡浓度为:Use the interpolation method to equivalence the changing radon concentration: first measure the environmental background to obtain the environmental radon concentration C 0 , and start collecting radon after completing the environmental background measurement. The radon concentration at the end of each measurement period is:
Cn=C0+ΔC1+ΔC2+....+ΔCn=K0,(n+1)N0,(n+1)+K1,(n+1)N1,(n+1)+K2,(n+1)N2,(n+1)+…+2Kn,(n+1)Nn,(n+1) (1);C n =C 0 +ΔC 1 +ΔC 2 +....+ΔC n =K 0,(n+1) N 0,(n+1) +K 1,(n+1) N 1,(n +1) +K 2,(n+1) N 2,(n+1) +…+2K n,(n+1) N n,(n+1) (1);
其中,…,Nn,(n+1)=Nn+1-N0,(n+1)-N1,(n+1)....-N(n-1),(n+1);in, …,N n,(n+1) =N n+1 -N 0,(n+1) -N 1,(n+1) ....-N (n-1),(n+1) ;
上式中,K0,(n+1)为氡浓度恒定条件下,从开始测量到第n+1个测量周期开始这段时间的刻度因子;K1,(n+1)为氡浓度恒定条件下,从第1个测量周期开始到第n+1个测量周期开始这段时间的刻度因子;K2,(n+1)为氡浓度恒定条件下,从第2个测量周期开始到第n+1个测量周期开始这段时间的刻度因子;Kn,(n+1)为氡浓度恒定条件下,从第n个测量周期开始到第n+1个测量周期开始这段时间的刻度因子;K0,n为氡浓度恒定条件下,从开始测量到第n个测量周期开始这段时间的刻度因子;K1,n为氡浓度恒定条件下,从第1个测量周期开始到第n个测量周期开始这段时间的刻度因子;N0,(n+1)为开始测量时析出的氡到第n+1个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;N1,(n+1)为从第1个测量周期开始时析出的氡到第n+1个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;N2,(n+1)为从第2个测量周期开始时析出的氡到第n+1个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;Nn,(n+1)为从第n个测量周期开始时析出的氡到第n+1个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;Nn+1为在第n+1个测量周期开始时,探测器收集到的α粒子总计数值;In the above formula, K 0,(n+1) is the scale factor from the start of measurement to the beginning of the n+1th measurement cycle under the condition of constant radon concentration; K 1,(n+1) is the constant radon concentration Under conditions, the scale factor from the start of the first measurement period to the start of the n+1th measurement period; K 2,(n+1) is the constant radon concentration condition, from the start of the second measurement period to the first The scale factor of the period from the start of n+1 measurement periods; K n,(n+1) is the scale from the start of the nth measurement period to the start of the n+1th measurement period under the condition of constant radon concentration factor; K 0,n is the scale factor of the period from the start of measurement to the start of the nth measurement cycle under the condition of constant radon concentration; K 1,n is the condition of constant radon concentration, from the first measurement cycle to the first The scale factor at the beginning of n measurement cycles; N 0,(n+1) is the alpha particles generated by decay and collected by the detector during the period from the start of the measurement to the start of the n+1th measurement cycle number; N 1,(n+1) is the number of alpha particles produced by decay and collected by the detector during the period from the radon precipitated at the beginning of the first measurement cycle to the beginning of the n+1th measurement cycle; N 2, (n+1) is the number of alpha particles produced by decay and collected by the detector from the radon precipitated at the beginning of the second measurement period to the beginning of the n+1th measurement period; N n,(n+1) is the number of alpha particles produced by decay and collected by the detector from the radon precipitated at the beginning of the nth measurement period to the start of the n+1th measurement period; N n+1 is the n+1th measurement period At the beginning, the total number of alpha particles collected by the detector;
式(1)中的刻度因子值均通过以下式(2)计算得到;The scale factor values in formula (1) are all calculated by the following formula (2);
其中,K标=C标/ΔNP Among them, K standard = C standard / ΔNP
Ki,j为从第i个测量周期开始到第j个测量周期开始这段时间的刻度因子;T标为在标准氡室氡浓度恒定条件下对氡析出率测量仪器进行定值的测量周期时长,K标为测量周期T标的刻度因子;C标为测量周期T标结束时的氡浓度;ΔNP为在测量周期T标结束时,探测器收集的α粒子计数值;T为测量周期T标之外其它每个测量周期的时长,λR、λP分别为氡、218Po的衰变常量,其中λR=2.1×10-6s-1,λP=3.7×10-3s-1;K i,j is the scale factor from the start of the i-th measurement period to the start of the j-th measurement period; T is the measurement period of the radon precipitation rate measuring instrument under the condition of constant radon concentration in the standard radon room Duration, K is the scale factor of the measurement period T; C is the radon concentration at the end of the measurement period T ; ΔNP is the alpha particle count value collected by the detector at the end of the measurement period T; T is the measurement period The duration of each measurement period other than the T standard , λ R and λ P are the decay constants of radon and 218 Po, respectively, where λ R =2.1×10 -6 s -1 , λ P =3.7×10 -3 s - 1 ;
步骤二、氡析出率快速定值;Step 2, rapid setting of radon precipitation rate;
根据公式(1)、(2)计算出集氡过程中各测量周期结束时的氡浓度值,再根据所述氡浓度值计算氡析出率。Calculate the radon concentration value at the end of each measurement period in the radon collection process according to formulas (1) and (2), and then calculate the radon precipitation rate according to the radon concentration value.
优选的,先按照式(1)、(2)计算出集氡至第一个测量周期结束时的氡浓度C1以及第i个测量周期结束时的氡浓度Ci,i≥3;Preferably, first calculate the radon concentration C 1 from the collection to the end of the first measurement period and the radon concentration Ci at the end of the i-th measurement period according to formulas (1) and (2), i≥3;
再按下式计算氡析出率;Then calculate the radon precipitation rate according to the following formula;
V为集氡室有效体积与氡析出率测量仪器的测量室体积之和;V is the sum of the effective volume of the radon collecting chamber and the measuring chamber volume of the radon extraction rate measuring instrument;
S为集氡室的底面积;S is the bottom area of the radon collection chamber;
n为测量次数。n is the number of measurements.
基于与上述定值方法同样的发明构思,本发明还提供一种氡析出率快速定值装置,其包括绝缘外壳、测量室、高压模块、信号与数据处理模块,所述测量室设于绝缘外壳内,所述测量室的侧壁和底壁上设有导电材料制成的导电层,所述绝缘外壳的底壁上开设有多个贯穿导电层将测量室与外界连通的第一进气孔,在所述测量室的顶壁上安装有半导体探测器,所述高压模块与导电层电性连接,从而在所述测量室与半导体探测器之间形成静电场,使得氡衰变产生的第一代子体218Po在所述静电场的作用下被吸附到所述半导体探测器表面,所述半导体探测器与信号与数据处理模块连接,所述信号与数据处理模块用于对半导体探测器形成的电信号进行处理并结合前面所述的氡析出率快速定值方法计算相应的氡析出率值。Based on the same inventive concept as the above-mentioned setting method, the present invention also provides a rapid setting device for radon precipitation rate, which includes an insulating casing, a measuring chamber, a high-voltage module, a signal and data processing module, and the measuring chamber is provided in the insulating casing. Inside, the side walls and bottom walls of the measurement chamber are provided with conductive layers made of conductive materials, and the bottom wall of the insulating housing is provided with a plurality of first air inlet holes that penetrate the conductive layers to communicate the measurement chamber with the outside world , a semiconductor detector is installed on the top wall of the measurement chamber, and the high-voltage module is electrically connected to the conductive layer, so that an electrostatic field is formed between the measurement chamber and the semiconductor detector, so that the first The progeny 218 Po is adsorbed to the surface of the semiconductor detector under the action of the electrostatic field, and the semiconductor detector is connected to the signal and data processing module, which is used to form the semiconductor detector. The electrical signal of the radon is processed and the corresponding radon precipitation rate value is calculated in combination with the fast setting method of the radon precipitation rate described above.
进一步地,前述氡析出率快速定值装置还包括顶部开设有连接孔的集氡室,所述连接孔的孔壁上攻有第一内螺纹,所述绝缘外壳的外周面上攻有与第一内螺纹相匹配的外螺纹,所述绝缘外壳的下端可从连接孔伸入集氡室的内腔中并与集氡室螺纹连接。Further, the aforementioned radon precipitation rate rapid setting device also includes a radon collecting chamber with a connecting hole at the top, the hole wall of the connecting hole is tapped with a first internal thread, and the outer peripheral surface of the insulating shell is tapped with a first internal thread. An external thread matched with an internal thread, the lower end of the insulating shell can extend into the inner cavity of the radon collecting chamber from the connecting hole and be screwed with the radon collecting chamber.
优选的,所述导电层采用金属材料制成。Preferably, the conductive layer is made of metal material.
更进一步地,所述绝缘外壳的上段大、下段小,在所述上段与下段相接的部位形成台阶面,所述外螺纹设置在下段的外周面上,所述绝缘外壳的下端穿过连接孔与集氡室螺纹连接后,所述台阶面抵靠住集氡室的顶端面。Further, the upper section of the insulating shell is large and the lower section is small, a step surface is formed at the part where the upper section and the lower section are connected, the outer thread is arranged on the outer peripheral surface of the lower section, and the lower end of the insulating shell passes through the connection. After the hole is threadedly connected to the radon collecting chamber, the step surface abuts the top surface of the radon collecting chamber.
其中,在所述绝缘外壳的侧壁上还开设有多个贯穿导电层将测量室与外界连通的第二进气孔。Wherein, the side wall of the insulating shell is also provided with a plurality of second air inlet holes penetrating the conductive layer to communicate the measurement chamber with the outside world.
优选的,所述集氡室的数量为多个,每个集氡室的底面积与其体积的比值均不相同。Preferably, the number of the radon collecting chambers is multiple, and the ratio of the bottom area to the volume of each radon collecting chamber is different.
进一步地,前述氡析出率快速定值装置还包括底罩,所述底罩顶端敞口,在所述底罩的敞口端内壁上攻有与绝缘外壳上外螺纹相匹配的第二内螺纹,所述底罩的底部设有用于外接导气管路的进气端口和出气端口,所述底罩可从绝缘外壳下端往上套于绝缘外壳外部并与绝缘外壳螺纹连接。Further, the aforementioned radon precipitation rate rapid setting device also includes a bottom cover, the top of the bottom cover is open, and the inner wall of the open end of the bottom cover is tapped with a second inner thread that matches the outer thread on the insulating housing. The bottom of the bottom cover is provided with an air inlet port and an air outlet port for externally connecting the air guide pipeline, and the bottom cover can be sleeved on the outside of the insulating case from the lower end of the insulating case upwards and be connected with the insulating case by threads.
本发明采用差值法对变化的氡浓度进行等效(Cn=Cn-1+ΔCn=C0+ΔC1+ΔC2+…+ΔCn),通过相应的刻度因子值以及测量过程中探测器收集的α粒子计数数据再结合前一测量周期的氡浓度计算后一测量周期的氡浓度值,该方法在测量氡浓度时无需混合平衡的过程,大幅提高了氡析出率定值速度。The present invention adopts the difference method to equivalence the changing radon concentration (C n =C n-1 +ΔC n =C 0 +ΔC 1 +ΔC 2 +...+ΔC n ), through the corresponding scale factor value and measurement process The alpha particle count data collected by the detector in the middle of the year is combined with the radon concentration of the previous measurement period to calculate the radon concentration value of the next measurement period. This method does not require the process of mixing and equilibrium when measuring the radon concentration, which greatly improves the speed of radon precipitation rate determination. .
附图说明Description of drawings
图1为利用差值法对变化氡浓度进行等效的示意图;Fig. 1 is the schematic diagram that utilizes difference method to carry out equivalence to changing radon concentration;
图2为本发明所涉氡析出率快速定值装置主体部分的结构示意图;Fig. 2 is the structural schematic diagram of the main part of the radon precipitation rate fast setting device according to the present invention;
图3为图2所示氡析出率快速定值装置主体部分连接集氡室后的结构示意图;Fig. 3 is the structural schematic diagram after the main part of the radon precipitation rate fast setting device shown in Fig. 2 is connected to the radon collecting chamber;
图4为图3中集氡室的剖视图;Fig. 4 is a sectional view of the radon concentration chamber in Fig. 3;
图5为图2所示氡析出率快速定值装置主体部分连接底罩后的结构示意图;FIG. 5 is a schematic structural diagram of the main part of the radon precipitation rate rapid setting device shown in FIG. 2 after the bottom cover is connected;
图6为图3中底罩的剖视图;6 is a cross-sectional view of the bottom cover in FIG. 3;
图7为图3所示主体部分连接集氡室再扣置于待测介质表面测量氡析出率时的示意图;Fig. 7 is a schematic diagram when the main body part shown in Fig. 3 is connected to the radon collecting chamber and is then placed on the surface of the medium to be measured to measure the radon precipitation rate;
图8为图5所示主体部分连接底罩再连接氡室进行刻度时的结构示意图;Fig. 8 is the structural representation when the main body part shown in Fig. 5 is connected to the bottom cover and then connected to the radon chamber for calibration;
图中:In the picture:
1——绝缘外壳 2——测量室 3——高压模块1——Insulating shell 2——Measuring room 3——High voltage module
4——信号与数据处理模块 5——半导体探测器 6——集氡室4 - Signal and data processing module 5 - Semiconductor detector 6 - Radon collection chamber
7——底罩 1a——外螺纹 1b——台阶面7 - Bottom cover 1a - External thread 1b - Step surface
2a——导电层 2b——第一进气孔 2c——第二进气孔2a——conductive layer 2b——first air inlet 2c——second air inlet
6a——连接孔 6b——第一内螺纹 7a——第二内螺纹6a——connecting hole 6b——first internal thread 7a——second internal thread
7b——进气端口 7c——出气端口 8——氡子体过滤器7b - Inlet port 7c - Outlet port 8 - Radon daughter filter
9——取样泵 10——氡室。9 - Sampling pump 10 - Radon chamber.
具体实施方式Detailed ways
为了便于本领域技术人员更好地理解本发明相对于现有技术的改进之处,下面结合附图和实施例对本发明作进一步的描述。In order to facilitate those skilled in the art to better understand the improvements of the present invention relative to the prior art, the present invention will be further described below with reference to the accompanying drawings and embodiments.
需要提前说明的是,在本发明中,Ki,j表示在氡浓度恒定条件下,从第i个测量周期开始到第j个测量周期开始这段时间的刻度因子,Ni,j表示从第i个测量周期开始时析出的氡到第j个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;Nj为在第j个测量周期开始时,探测器收集的α粒子总计数值。上述i、j仅是一个一个代号,用于表示任意自然数。It should be noted in advance that, in the present invention, K i,j represents the scale factor from the start of the i-th measurement cycle to the start of the j-th measurement cycle under the condition of constant radon concentration, and Ni ,j represents the time from The number of alpha particles generated by the decay of radon at the beginning of the i-th measurement period to the start of the j-th measurement period and collected by the detector; N j is the α particle collected by the detector at the beginning of the j-th measurement period The particle total value. The above i and j are just a code, used to represent any natural number.
本发明涉及的氡析出率快速定值方法包括以下步骤:The rapid determination method of radon precipitation rate involved in the present invention comprises the following steps:
步骤一、快速跟踪测量变化的氡浓度;Step 1. Quickly track and measure the changing radon concentration;
利用插值法对变化的氡浓度进行等效:先对环境本底进行测量,得到环境氡浓度C0,完成环境本底测量后开始集氡,集氡过程中以T为测量周期,在第n个测量周期结束时的氡浓度为:Use the interpolation method to equivalence the changing radon concentration: first measure the environmental background to obtain the environmental radon concentration C 0 , and start collecting radon after completing the environmental background measurement. The radon concentration at the end of each measurement period is:
Cn=C0+ΔC1+ΔC2+....+ΔCn=K0,(n+1)N0,(n+1)+K1,(n+1)N1,(n+1)+K2,(n+1)N2,(n+1)+…+2Kn,(n+1)Nn,(n+1) (1);C n =C 0 +ΔC 1 +ΔC 2 +....+ΔC n =K 0,(n+1) N 0,(n+1) +K 1,(n+1) N 1,(n +1) +K 2,(n+1) N 2,(n+1) +…+2K n,(n+1) N n,(n+1) (1);
其中,…,Nn,(n+1)=Nn+1-N0,(n+1)-N1,(n+1)....-N(n-1),(n+1);in, …,N n,(n+1) =N n+1 -N 0,(n+1) -N 1,(n+1) ....-N (n-1),(n+1) ;
上式中,K0,(n+1)为氡浓度恒定条件下,从开始测量到第n+1个测量周期开始这段时间的刻度因子;K1,(n+1)为氡浓度恒定条件下,从第1个测量周期开始到第n+1个测量周期开始这段时间的刻度因子;K2,(n+1)为氡浓度恒定条件下,从第2个测量周期开始到第n+1个测量周期开始这段时间的刻度因子;Kn,(n+1)为氡浓度恒定条件下,从第n个测量周期开始到第n+1个测量周期开始这段时间的刻度因子;K0,n为氡浓度恒定条件下,从开始测量到第n个测量周期开始这段时间的刻度因子;K1,n为氡浓度恒定条件下,从第1个测量周期开始到第n个测量周期开始这段时间的刻度因子;N0,(n+1)为开始测量时析出的氡到第n+1个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;N1,(n+1)为从第1个测量周期开始时析出的氡到第n+1个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;N2,(n+1)为从第2个测量周期开始时析出的氡到第n+1个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;Nn,(n+1)为从第n个测量周期开始时析出的氡到第n+1个测量周期开始这段时间衰变产生且被探测器收集到的α粒子数;Nn+1为在第n+1个测量周期开始时,探测器收集到的α粒子总计数值;In the above formula, K 0,(n+1) is the scale factor from the start of measurement to the beginning of the n+1th measurement cycle under the condition of constant radon concentration; K 1,(n+1) is the constant radon concentration Under conditions, the scale factor from the start of the first measurement period to the start of the n+1th measurement period; K 2,(n+1) is the constant radon concentration condition, from the start of the second measurement period to the first The scale factor of the period from the start of n+1 measurement periods; K n,(n+1) is the scale from the start of the nth measurement period to the start of the n+1th measurement period under the condition of constant radon concentration factor; K 0,n is the scale factor of the period from the start of measurement to the start of the nth measurement cycle under the condition of constant radon concentration; K 1,n is the condition of constant radon concentration, from the first measurement cycle to the first The scale factor at the beginning of n measurement cycles; N 0,(n+1) is the alpha particles generated by decay and collected by the detector during the period from the start of the measurement to the start of the n+1th measurement cycle number; N 1,(n+1) is the number of alpha particles produced by decay and collected by the detector during the period from the radon precipitated at the beginning of the first measurement cycle to the beginning of the n+1th measurement cycle; N 2, (n+1) is the number of alpha particles produced by decay and collected by the detector from the radon precipitated at the beginning of the second measurement period to the beginning of the n+1th measurement period; N n,(n+1) is the number of alpha particles produced by decay and collected by the detector from the radon precipitated at the beginning of the nth measurement period to the start of the n+1th measurement period; N n+1 is the n+1th measurement period At the beginning, the total number of alpha particles collected by the detector;
式(1)中的刻度因子值均通过以下式(2)计算得到;The scale factor values in formula (1) are all calculated by the following formula (2);
其中,K标=C标/ΔNP Among them, K standard = C standard / ΔNP
Ki,j为从第i个测量周期开始到第j个测量周期开始这段时间的刻度因子;T标为在标准氡室氡浓度恒定条件下对氡析出率测量仪器进行定值的测量周期时长,K标为测量周期T标的刻度因子;C标为测量周期T标结束时的氡浓度;ΔNP为在测量周期T标结束时,探测器收集的α粒子计数值;T为测量周期T标之外其它每个测量周期的时长,λR、λP分别为氡、218Po的衰变常量,其中λR=2.1×10-6s-1,λP=3.7×10-3s-1;K i,j is the scale factor from the start of the i-th measurement period to the start of the j-th measurement period; T is the measurement period of the radon precipitation rate measuring instrument under the condition of constant radon concentration in the standard radon room Duration, K is the scale factor of the measurement period T; C is the radon concentration at the end of the measurement period T ; ΔNP is the alpha particle count value collected by the detector at the end of the measurement period T; T is the measurement period The duration of each measurement period other than the T standard , λ R and λ P are the decay constants of radon and 218 Po, respectively, where λ R =2.1×10 -6 s -1 , λ P =3.7×10 -3 s - 1 ;
步骤二、氡析出率快速定值;Step 2, rapid setting of radon precipitation rate;
根据公式(1)、(2)计算出集氡过程中各测量周期结束时的氡浓度值,再根据所述氡浓度值计算氡析出率。Calculate the radon concentration value at the end of each measurement period in the radon collection process according to formulas (1) and (2), and then calculate the radon precipitation rate according to the radon concentration value.
需要说明的是,本发明相对于现有技术的改进之处主要在于采用差值法对变化的氡浓度进行等效计算,在得出集氡过程中各测量周期的氡浓度值后可以采用现有技术中的方案来计算相应的氡析出率。在现有技术中,集氡室内的氡浓度变化通常用下式表示:It should be noted that the improvement of the present invention relative to the prior art is mainly in that the difference method is used to perform equivalent calculation on the changed radon concentration, and the existing radon concentration value in each measurement period in the radon collection process can be obtained. There are solutions in the art to calculate the corresponding radon release rate. In the prior art, the radon concentration change in the radon collection chamber is usually expressed by the following formula:
式中:C为集氡室内的氡浓度;V为集氡室体积;J为氡析出率;S为集氡室底面积;λ为氡的衰变常量;R为泄露和反扩散常量;t为集氡时间。where C is the radon concentration in the radon collecting chamber; V is the volume of the radon collecting chamber; J is the radon precipitation rate; S is the bottom area of the radon collecting chamber; λ is the decay constant of radon; R is the leakage and anti-diffusion constant; t is the Set radon time.
令λe=λ+R,Let λ e =λ+R,
令则有: make Then there are:
Ci+1=a+bCi C i+1 =a+bC i
为提高测量精度,进行多次测量,用最小二乘法采用线性拟合来计算a、b,最后求出λe和J,即可得到氡析出率值。In order to improve the measurement accuracy, carry out multiple measurements, use the least squares method to calculate a and b by linear fitting, and finally obtain λ e and J, and then the radon precipitation rate value can be obtained.
当然,也可以采用文献CN105425267A中的氡析出率计算方式,具体来说,先按照式(1)、(2)计算出集氡至第一个测量周期结束时的氡浓度C1以及第i个测量周期结束时的氡浓度Ci(i≥3)后,再按下式计算氡析出率;Of course, the radon precipitation rate calculation method in the document CN105425267A can also be used. Specifically, first calculate the radon concentration C1 and the i-th radon concentration from the collection of radon to the end of the first measurement cycle according to formulas (1) and (2). After measuring the radon concentration Ci (i≥3) at the end of the measurement period, calculate the radon precipitation rate as follows;
V为集氡室有效体积与氡析出率测量仪器的测量室体积之和;V is the sum of the effective volume of the radon collecting chamber and the measuring chamber volume of the radon extraction rate measuring instrument;
S为集氡室的底面积;S is the bottom area of the radon collection chamber;
n为测量次数。n is the number of measurements.
上述氡析出率快速定值方法采用差值法对变化的氡浓度进行等效(Cn=Cn-1+ΔCn=C0+ΔC1+ΔC2+…+ΔCn),通过相应的刻度因子值以及测量过程中探测器收集的α粒子计数数据再结合前一测量周期的氡浓度计算后一测量周期的氡浓度值,该方法在进行氡浓度测量时无需混合平衡的过程,可以大幅提高氡析出率定值速度。The above - mentioned rapid determination method of radon precipitation rate adopts the difference method to equiv- The scale factor value and the alpha particle count data collected by the detector during the measurement process are combined with the radon concentration of the previous measurement period to calculate the radon concentration value of the next measurement period. Improve the speed of setting value of radon precipitation rate.
作为本发明的另一方面,本申请还提供一种利用前述方法对氡析出率快速定值的装置,图2-6示出了该氡析出率快速定值装置的一种具体结构,其包括绝缘外壳1、测量室2、高压模块3(可以选择常用的3KV高压模块)、信号与数据处理模块4,测量室2设于绝缘外壳1内,测量室2的侧壁和底壁上设有导电材料制成的导电层2a(导电层2a可以选用金属材料制成),绝缘外壳1的底壁上开设有多个贯穿导电层2a将测量室2与外界连通的第一进气孔2b,在测量室2的顶壁上安装有半导体探测器5,高压模块3与导电层2a电性连接,从而在测量室2与半导体探测器5之间形成静电场,使得氡衰变产生的第一代子体218Po在静电场的作用下被吸附到所述半导体探测器5表面,半导体探测器5与信号与数据处理模块4连接,信号与数据处理模块4用于对半导体探测器5形成的电信号进行处理并结合前面所述的氡析出率快速定值方法计算相应的氡析出率值。As another aspect of the present invention, the present application also provides a device for rapidly setting the radon precipitation rate by using the aforementioned method. Figures 2-6 show a specific structure of the device for rapidly setting the radon precipitation rate, which includes: Insulation shell 1, measurement room 2, high-voltage module 3 (commonly used 3KV high-voltage module can be selected), signal and data processing module 4, the measurement room 2 is set in the insulation shell 1, and the side walls and bottom walls of the measurement room 2 are provided with The conductive layer 2a made of conductive material (the conductive layer 2a can be made of metal material), the bottom wall of the insulating housing 1 is provided with a plurality of first air inlet holes 2b that pass through the conductive layer 2a to communicate the measurement chamber 2 with the outside world, A semiconductor detector 5 is installed on the top wall of the measurement chamber 2, and the high-voltage module 3 is electrically connected to the conductive layer 2a, so that an electrostatic field is formed between the measurement chamber 2 and the semiconductor detector 5, so that the first generation of radon decay produces The sub-body 218 Po is adsorbed to the surface of the semiconductor detector 5 under the action of the electrostatic field. The semiconductor detector 5 is connected to the signal and data processing module 4 , and the signal and data processing module 4 is used to detect the electrical signals formed by the semiconductor detector 5 . The signal is processed and the corresponding radon leaching rate value is calculated in combination with the radon leaching rate fast setting method described above.
需要强调的是,本发明所涉氡析出率快速定值装置并不涉及对信号与数据处理模块4(即信号处理与数据处理硬件电路部分)的改进,本领域技术人员应当明白,本发明主要的改进之处在于测算方法方面,而非装置的电路部分。对于上述氡析出率快速定值装置来说,其完全可以采用文献CN105425267A中的电路结构(包括前置放大电路、放大成形电路、脉冲幅度甄别电路、单片机、能谱峰自动调节电路、TFT显示屏,电路结构框图见文献CN105425267A中图2所示)来实现对半导体探测器5形成的电信号进行处理并根据前面所述方法中的步骤来计算氡浓度值,再根据得到的氡浓度值计算相应的氡析出率值。It should be emphasized that the device for rapid determination of the radon precipitation rate involved in the present invention does not involve the improvement of the signal and data processing module 4 (ie, the signal processing and data processing hardware circuit part). Those skilled in the art should understand that the present invention mainly The improvement is in the measurement method, not the circuit part of the device. For the above-mentioned radon precipitation rate fast setting device, it can completely adopt the circuit structure in the document CN105425267A (including preamplifier circuit, amplification and shaping circuit, pulse amplitude discrimination circuit, single chip microcomputer, energy spectrum peak automatic adjustment circuit, TFT display screen) , the circuit structure block diagram is shown in Figure 2 in the document CN105425267A) to realize the processing of the electrical signal formed by the semiconductor detector 5 and calculate the radon concentration value according to the steps in the aforementioned method, and then calculate the corresponding radon concentration value according to the obtained radon concentration value. The radon extraction rate value.
在图3-4中,上述氡析出率快速定值装置还包括顶部开设有连接孔6a的集氡室6,连接孔6a的孔壁上攻有第一内螺纹6b,绝缘外壳1的外周面上攻有与第一内螺纹6b相匹配的外螺纹1a,绝缘外壳1的下端可从连接孔6a伸入集氡室6的内腔中并与集氡室6螺纹连接。具体来说,绝缘外壳1为上段大、下段小的结构,在上段与下段相接的部位形成台阶面1b,外螺纹1a设置在下段的外周面上,当绝缘外壳1的下端穿过连接孔6a与集氡室6螺纹连接后,台阶面1b可以抵靠住集氡室6的顶端面。此外,在绝缘外壳1的侧壁上还开设有多个贯穿导电层2a将测量室2与外界连通的第二进气孔2c。优选的,前述集氡室6的数量为多个,每个集氡室6的底面积与其体积的比值均不相同。在测量待测介质氡析出率时,如图7所示,先对环境本底进行测量,得到环境氡浓度C0,然后将集氡室6与图2所示氡析出率快速定值装置的主体部分连接,并将集氡室6扣置到待测介质表面进行集氡,氡及其子体扩散方向见图7中箭头所示,集氡过程中,信号与数据处理模块4对半导体探测器5形成的电信号进行处理并结合前面所述的氡析出率快速定值方法(将前述方法编成程序植入到信号与数据处理模块4中)即可计算得到相应的氡析出率值。值得一提的是,配置多个底面积与其体积比值均不相同的集氡室6后,可以通过选择底面积与体积比值更大的集氡室6来在相同时间内获得相对更高的氡浓度,由于在氡析出率、氡的衰变常量、泄露和反扩散常量及集氡时间相同的条件下,改变集氡室底面积与其体积的比值显然可相应地改变氡浓度。In Fig. 3-4, the above-mentioned radon precipitation rate rapid setting device also includes a radon collecting chamber 6 with a connecting hole 6a at the top, the hole wall of the connecting hole 6a is tapped with a first internal thread 6b, and the outer peripheral surface of the insulating housing 1 There is an external thread 1a matched with the first internal thread 6b, and the lower end of the insulating housing 1 can extend into the inner cavity of the radon collecting chamber 6 from the connecting hole 6a and be screwed with the radon collecting chamber 6 . Specifically, the insulating shell 1 has a structure with a large upper section and a small lower section, a stepped surface 1b is formed at the part where the upper section and the lower section meet, and the external thread 1a is arranged on the outer peripheral surface of the lower section. When the lower end of the insulating shell 1 passes through the connecting hole After 6a is screwed with the radon collecting chamber 6 , the step surface 1b can abut against the top surface of the radon collecting chamber 6 . In addition, a plurality of second air inlet holes 2c penetrating the conductive layer 2a to communicate the measurement chamber 2 with the outside are also opened on the side wall of the insulating housing 1 . Preferably, the number of the aforementioned radon collecting chambers 6 is multiple, and the ratio of the bottom area to the volume of each radon collecting chamber 6 is different. When measuring the radon precipitation rate of the medium to be measured, as shown in FIG. 7 , first measure the environmental background to obtain the environmental radon concentration C 0 , and then connect the radon collecting chamber 6 with the radon precipitation rate rapid setting device shown in FIG. 2 . The main part is connected, and the radon collecting chamber 6 is buckled to the surface of the medium to be measured for radon collection. The diffusion direction of radon and its daughters is shown by the arrow in Figure 7. During the radon collection process, the signal and data processing module 4 detects the semiconductor. The electrical signal formed by the device 5 is processed and the corresponding radon leaching rate value can be calculated by combining with the aforementioned rapid radon extraction rate setting method (programming the aforementioned method into the signal and data processing module 4). It is worth mentioning that, after configuring a plurality of radon collecting chambers 6 with different bottom area to volume ratios, a relatively higher radon concentration can be obtained in the same time by selecting a radon collecting chamber 6 with a larger bottom area to volume ratio. concentration, due to Under the same conditions of radon precipitation rate, radon decay constant, leakage and anti-diffusion constant and radon collecting time, changing the ratio of the bottom area of the radon collecting chamber to its volume can obviously change the radon concentration accordingly.
此外,上述氡析出率快速定值装置还可以包括图5-6中的底罩7,底罩7顶端敞口,在底罩7的敞口端内壁上攻有与绝缘外壳1上外螺纹1a相匹配的第二内螺纹7a,底罩7的底部设有用于外接导气管路的进气端口7b和出气端口7c,底罩7可从绝缘外壳1下端往上套于绝缘外壳1外部并与绝缘外壳1螺纹连接。底罩7主要是在确定刻度因子时使用,如图8所示,对氡析出率快速定值装置刻度时,将底罩7的进气端口7b通过管道依次连接氡子体过滤器8、取样泵9及氡室10,再将底罩7的出气端口7c通过另一条管道也与氡室10连接即可利用氡室10对氡析出率快速定值装置进行刻度(气流方向参考图中箭头方向所示)。In addition, the above-mentioned radon precipitation rate rapid setting device may also include the bottom cover 7 in FIGS. 5-6 , the top of the bottom cover 7 is open, and the inner wall of the open end of the bottom cover 7 is tapped with an external thread 1a on the insulating casing 1 The matching second internal thread 7a, the bottom of the bottom cover 7 is provided with an air inlet port 7b and an air outlet port 7c for externally connecting the air guide pipeline, and the bottom cover 7 can be sleeved from the lower end of the insulating case 1 to the outside of the insulating case 1 and connected to the outside of the insulating case 1. Insulation housing 1 screw connection. The bottom cover 7 is mainly used when determining the scale factor. As shown in FIG. 8 , when the radon precipitation rate rapid setting device is scaled, the air inlet port 7b of the bottom cover 7 is connected to the radon daughter filter 8 through the pipeline in turn, and the sampling is performed. The pump 9 and the radon chamber 10, and then the air outlet 7c of the bottom cover 7 is also connected to the radon chamber 10 through another pipeline, and the radon chamber 10 can be used to calibrate the radon precipitation rate rapid setting device (refer to the direction of the arrow in the figure for the airflow direction. shown).
需要说明的是,上述集氡室6和底罩7实际上是氡析出率快速定值装置的附件,在实际应用时可以利用现有技术中已有的集氡室和底罩来替代或改造,集氡室6和底罩7也不是必须通过螺纹与图2所示的氡析出率快速定值装置主体部分可拆卸连接,实际生产销售时,图2所示氡析出率快速定值装置主体部分是可以单独出售的。另外,可应用于本发明所涉氡析出率快速定值装置的集氡室6和底罩7并不限于附图中所示的结构,在了解本发明的技术构思之后,本领域技术人员应当明白,集氡室6和底罩7还可以采用其它结构,只要其能够实现本申请的发明目的即可。上述对集氡室6和底罩7结构的描述只是用于举例说明,以便于本领域技术人员更好地理解本发明的技术构思,图中所示集氡室6和底罩7的结构仅是优选,而非唯一结构方案。It should be noted that the above-mentioned radon collecting chamber 6 and the bottom cover 7 are actually accessories of the radon precipitation rate rapid setting device, and the existing radon collecting chamber and bottom cover in the prior art can be used to replace or transform in practical application. , the radon collecting chamber 6 and the bottom cover 7 do not have to be detachably connected to the main body of the radon precipitation rate rapid setting device shown in Figure 2 through threads. Parts can be sold separately. In addition, the radon collecting chamber 6 and the bottom cover 7 that can be applied to the radon precipitation rate rapid setting device of the present invention are not limited to the structures shown in the drawings. After understanding the technical concept of the present invention, those skilled in the art should It is understood that the radon collecting chamber 6 and the bottom cover 7 can also adopt other structures, as long as they can achieve the purpose of the invention of the present application. The above description of the structure of the radon collecting chamber 6 and the bottom cover 7 is only used for illustration, so that those skilled in the art can better understand the technical concept of the present invention, and the structures of the radon collecting chamber 6 and the bottom cover 7 shown in the figures are only is the preferred, not the only structural solution.
上述实施例为本发明较佳的实现方案,除此之外,本发明还可以其它方式实现,在不脱离本技术方案构思的前提下任何显而易见的替换均在本发明的保护范围之内。The above-mentioned embodiment is a preferred implementation scheme of the present invention. In addition, the present invention can also be implemented in other ways, and any obvious replacements are within the protection scope of the present invention without departing from the concept of the technical solution.
为了让本领域普通技术人员更方便地理解本发明相对于现有技术的改进之处,本发明的一些附图和描述已经被简化,并且为了清楚起见,本申请文件还省略了一些其它元素,本领域普通技术人员应该意识到这些省略的元素也可构成本发明的内容。In order to make it easier for those skilled in the art to understand the improvements of the present invention relative to the prior art, some drawings and descriptions of the present invention have been simplified, and for the sake of clarity, some other elements are also omitted in this application document, One of ordinary skill in the art would realize that these omitted elements may also constitute the subject matter of the present invention.
Claims (9)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201810123413.7A CN108363089B (en) | 2018-02-07 | 2018-02-07 | Method and device for rapid determination of radon precipitation rate |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201810123413.7A CN108363089B (en) | 2018-02-07 | 2018-02-07 | Method and device for rapid determination of radon precipitation rate |
Publications (2)
Publication Number | Publication Date |
---|---|
CN108363089A CN108363089A (en) | 2018-08-03 |
CN108363089B true CN108363089B (en) | 2019-02-22 |
Family
ID=63004737
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201810123413.7A Expired - Fee Related CN108363089B (en) | 2018-02-07 | 2018-02-07 | Method and device for rapid determination of radon precipitation rate |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN108363089B (en) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN112946717B (en) * | 2021-01-28 | 2023-01-17 | 衡阳师范学院 | Portable radon exhalation rate and radon concentration reference device and reference determination method |
CN112946718B (en) * | 2021-01-28 | 2022-12-06 | 衡阳师范学院 | Radon exhalation rate reference determination method and portable radon exhalation rate reference determination device |
DE102022100066A1 (en) | 2022-01-03 | 2023-07-06 | SafeRadon GmbH | Determination device for determining an exhalation rate of a surface of a building and determination method |
CN115236719A (en) * | 2022-07-27 | 2022-10-25 | 核工业北京化工冶金研究院 | A measuring device and method for surface radon precipitation rate based on electret radon measurement |
Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DD276538A1 (en) * | 1988-10-27 | 1990-02-28 | Freiberg Bergakademie | COMPRESSOR CHAMBER FOR GAS EXHAUST MEASUREMENT |
CN2924527Y (en) * | 2006-05-12 | 2007-07-18 | 核工业北京地质研究院 | On-site multi-channel α energy spectrum measuring instrument for radon exhalation rate and radon concentration |
CN101071108A (en) * | 2006-05-12 | 2007-11-14 | 核工业北京地质研究院 | Radon exhalation rate and radon concentration field multi-channel alpha energy spectrum measuring instrument |
CN101609154A (en) * | 2009-07-01 | 2009-12-23 | 衡阳师范学院 | Method for measuring radon exhalation rate |
CN101782655A (en) * | 2010-03-19 | 2010-07-21 | 南华大学 | Method and device for measuring radon exhalation rate in open loop way |
CN102830417A (en) * | 2012-08-30 | 2012-12-19 | 衡阳师范学院 | Method for closed-loop measurement of radon exhalation rate by utilizing total count of 218Po and 214Po |
CN104765060A (en) * | 2015-03-26 | 2015-07-08 | 南华大学 | Radon monitor scale factor valuing method |
CN105425267A (en) * | 2015-11-06 | 2016-03-23 | 南华大学 | System and method for measuring evolution rate of radon |
CN106959464A (en) * | 2017-03-29 | 2017-07-18 | 南华大学 | The measurement apparatus and measuring method of a kind of precipitation rate of radon |
-
2018
- 2018-02-07 CN CN201810123413.7A patent/CN108363089B/en not_active Expired - Fee Related
Patent Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DD276538A1 (en) * | 1988-10-27 | 1990-02-28 | Freiberg Bergakademie | COMPRESSOR CHAMBER FOR GAS EXHAUST MEASUREMENT |
CN2924527Y (en) * | 2006-05-12 | 2007-07-18 | 核工业北京地质研究院 | On-site multi-channel α energy spectrum measuring instrument for radon exhalation rate and radon concentration |
CN101071108A (en) * | 2006-05-12 | 2007-11-14 | 核工业北京地质研究院 | Radon exhalation rate and radon concentration field multi-channel alpha energy spectrum measuring instrument |
CN101609154A (en) * | 2009-07-01 | 2009-12-23 | 衡阳师范学院 | Method for measuring radon exhalation rate |
CN101782655A (en) * | 2010-03-19 | 2010-07-21 | 南华大学 | Method and device for measuring radon exhalation rate in open loop way |
CN102830417A (en) * | 2012-08-30 | 2012-12-19 | 衡阳师范学院 | Method for closed-loop measurement of radon exhalation rate by utilizing total count of 218Po and 214Po |
CN104765060A (en) * | 2015-03-26 | 2015-07-08 | 南华大学 | Radon monitor scale factor valuing method |
CN105425267A (en) * | 2015-11-06 | 2016-03-23 | 南华大学 | System and method for measuring evolution rate of radon |
CN106959464A (en) * | 2017-03-29 | 2017-07-18 | 南华大学 | The measurement apparatus and measuring method of a kind of precipitation rate of radon |
Non-Patent Citations (4)
Title |
---|
基于ERS2S测氡仪的氡析出率准确测量研究;张叶等;《核电子学与探测技术》;20150228;第35卷(第2期);第150-153页 |
氡析出率快速测量的不确定度评定;李志强等;《核技术》;20170430;第40卷(第4期);第1-6页 |
氡析出率标准装置快速定值方法的研究与应用;李志强;《中国博士学位论文全文数据库(电子期刊)工程科技Ⅱ辑》;20170215;第1-86页 |
泄露和反扩散对氡析出率测量的影响研究;李志强等;《核电子学与探测技术》;20151231;第35卷(第12期);第1255-1258页 |
Also Published As
Publication number | Publication date |
---|---|
CN108363089A (en) | 2018-08-03 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN108363089B (en) | Method and device for rapid determination of radon precipitation rate | |
CA2244342C (en) | A method and apparatus for measuring well characteristics and formation properties | |
CN104820230B (en) | A kind of Low background α, β activity analysis instrument | |
Sirkar et al. | The limiting behaviour of the turbulent transverse velocity component close to a wall | |
CN106707325B (en) | For measuring the method and system of dielectric surface radon release total amount in certain period of time | |
CN111625750B (en) | Identification method for tight sandstone reservoir gas layer and gas-water same layer | |
CN110108658A (en) | A kind of infrared spectra of pollutant gas recognition methods and system | |
CN108646286B (en) | A reference device and method for continuously and reliably controlling radon exhalation rate | |
CN108614289A (en) | Radon Exhalation Rate Measuring Apparatus synchronizes gauge device and method | |
CN207965115U (en) | A kind of impulse phase detection error caliberating device of PD meter | |
Bowen et al. | The influence of the Earth's magnetic field on cosmic-ray intensities up to the top of the atmosphere | |
CN105181782B (en) | The detecting system and detection method of a kind of array detection plate for ionic migration spectrometer | |
CN111963162B (en) | Lithology and water-based dual-parameter fluid property identification method | |
CN109031388A (en) | Radon consistence absolute measuring system and method in a kind of water | |
CN109630091B (en) | Method for optimizing numerical simulation energy spectrum in carbon-oxygen ratio logging | |
CN109470311B (en) | A multi-parameter RF online detection device and detection method for double-concealed probe-type grain silos | |
CN115628783B (en) | Gas-liquid two-phase flow metering system based on multiple sensors | |
CN112946717B (en) | Portable radon exhalation rate and radon concentration reference device and reference determination method | |
Giesel et al. | Water flow calculations by means of gamma absorption and tensiometer field measurements in the unsaturated soil profile | |
CN112946718A (en) | Radon exhalation rate reference constant value method and portable radon exhalation rate reference constant value device | |
CN109085082A (en) | A kind of pressurization capillary water absorption height and water absorption measuring device and measuring method | |
CN106646579B (en) | Simplified phantom for whole body counter calibration and calibration method | |
CN109696701A (en) | Based on radon itself the decay quick detection device and method for inhibiting radon daughter | |
Ludwig et al. | Proton Polarization in the Sr 88 (d, p) Sr 8 9*(1.05-MeV) Reaction | |
Fulbright et al. | A comparison of the C12 (He3, p) and (He3, n) reactions leading to analogue states in N14 and O14 |
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 | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20190222 |
|
CF01 | Termination of patent right due to non-payment of annual fee |