WO2013189124A1 - Method of determining material-level curve in continuous-type passive nucleonic level gauge - Google Patents

Method of determining material-level curve in continuous-type passive nucleonic level gauge Download PDF

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Publication number
WO2013189124A1
WO2013189124A1 PCT/CN2012/080196 CN2012080196W WO2013189124A1 WO 2013189124 A1 WO2013189124 A1 WO 2013189124A1 CN 2012080196 W CN2012080196 W CN 2012080196W WO 2013189124 A1 WO2013189124 A1 WO 2013189124A1
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Prior art keywords
level
gamma ray
ray intensity
curve
measured
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PCT/CN2012/080196
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French (fr)
Chinese (zh)
Inventor
郭云昌
朱敏娟
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Guo Yunchang
Zhu Minjuan
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Publication of WO2013189124A1 publication Critical patent/WO2013189124A1/en

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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F23/00Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
    • G01F23/22Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
    • G01F23/28Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material
    • G01F23/284Electromagnetic waves
    • G01F23/288X-rays; Gamma rays or other forms of ionising radiation
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F25/00Testing or calibration of apparatus for measuring volume, volume flow or liquid level or for metering by volume
    • G01F25/20Testing or calibration of apparatus for measuring volume, volume flow or liquid level or for metering by volume of apparatus for measuring liquid level

Definitions

  • the present invention relates to the field of passive nuclear material level measurement technology, and in particular, to a method for determining a material level curve in a continuous passive nuclear material level gauge.
  • the passive nuclear material level meter makes it easy to realize the non-contact measurement level without using the radioactive source but only by using the gamma radioactivity of the measured material itself and the gamma radioactivity in the environment of the tested container. Effective and feasible, the field that originally needs to use the nuclear level gauge is replaced by a passive nuclear level gauge, which greatly reduces the number of radioactive sources used, eliminates the high cost of radioactive source management, and reduces the radiation risk.
  • the passive nuclear material level can be divided into two types: switch mode and continuous type.
  • the switch type passive nuclear level gauge is a level meter that can only distinguish whether the material height reaches the set position and outputs a switching signal; and the continuous level meter can distinguish the specific material height and output one or A level meter for a variety of continuous level signals.
  • the material level curve is the corresponding relationship between the material height and the gamma ray intensity. Therefore, the determination of the material level curve plays a very important role in accurately determining the material level.
  • the domestic patent CN200810017274 provides an ideal calculation method which is very inconsistent with reality and is used to calculate the corresponding curve of the level and the measured radioactivity.
  • the method firstly simplifies the bulk radioactive source into a planar radioactive source, and then simplifies the position of the measuring point on the side of the bulk radioactive source to a point above the planar radioactive source, and finally expands the ideal situation above the plane to a point.
  • the trend of the curve thus calculated is opposite to the actual when the measuring point is close to the material interface, so there is no practical value.
  • Another method disclosed in the domestic patent CN03115824 for measuring the level using natural radioactivity is characterized in that, in the case of a known material level, the material is gradually increased, and the gamma ray radiation intensity is continuously measured to obtain the material height and gamma ray emission.
  • the applicable premise of the method is the known material level, and the material level at each moment is known, but in actual cases, the method is difficult to achieve for three reasons: First, the material level cannot usually be accurately known in time; Second, in order to compare Accurate gamma ray intensity values require a certain response time. Third, due to the randomness of gamma rays, the actual measured gamma ray intensity value is a range.
  • the object of the present invention is to make up for the deficiencies of the prior art and to provide a method for accurately determining the material level curve in a continuous passive nuclear level gauge.
  • a method for determining a material level curve in a continuous passive nuclear level gauge which comprises a measuring device and a calculation module, characterized in that the method adopts a direct method and comprises the following steps:
  • the range of the material level is obtained according to the actual measured gamma ray intensity, and the middle value is the measured material level.
  • the method uses a push algorithm instead of the direct method and includes the following steps:
  • the method uses a reference method instead of the direct method and includes the following steps:
  • the push algorithm is applicable to the situation that the two states of the filled container and the complete material empty can be determined, including the case where the specific intermediate material level cannot be determined, and the corresponding relationship between the gamma ray intensity and the material level is obtained.
  • the reference method is applicable to all situations, including the inability to determine the actual level, and the determination of the full and empty state of the container under test.
  • the material level curve in the push algorithm and the reference method is a relatively thick curve, and each material level corresponds to a gamma ray intensity range; each measured gamma ray intensity also corresponds to a material level on the curve.
  • Range the range is the measurement accuracy of the continuous passive nuclear level gauge; the moving positioning method used in the curve fitting in the push algorithm is in a certain level state, from top to bottom or from Moving the continuous passive nuclear level gauge down and up, simultaneously measuring the intensity of the gamma ray, and obtaining a set of changed data.
  • the continuous passive nuclear level corresponding to the largest difference between two adjacent data in the set of data
  • the measured position of the meter is the actual level.
  • the present invention makes up for the gap of the prior art, and provides a method for determining the relationship between the material level and the gamma ray intensity of the continuous passive nuclear level gauge, which provides a solid foundation for accurately determining the material level.
  • the invention proposes a direct method, a fitting push algorithm and a reference method, which can replace each other according to the actual measurement situation, which not only increases the selectivity of the user according to the actual measurement situation, but also can be used as a test method to improve the reliability of the data. degree.
  • FIG. 1 is a schematic diagram showing the internal hardware structure of a passive nuclear level gauge according to the present invention
  • FIG. 2 is a schematic diagram of the application of a passive nuclear level gauge according to the present invention
  • Bit diagram Figure 1. Material 2. Container to be tested 3.
  • Passive nuclear level gauge 4.
  • Passive nuclear level gauge bracket [Detailed Description] The present invention will be further described with reference to the accompanying drawings, which is specialized in the field. The technician is OK To achieve.
  • the method of the present invention is proposed to be applied to a continuous level gauge. It is desirable to continuously output an accurate level signal as the height of the material changes.
  • the basic design of the design is: Continually install a sensitivity point at a determined measurement point.
  • Passive nuclear level gauge measure the intensity of gamma ray in a determined response time, determine the relationship between the measured gamma ray intensity and the level, and output the measured material according to the actual measured gamma ray intensity value. Bit.
  • the implementation of the direct method proposed by the present invention should first determine the material level in combination with other methods.
  • the method is not limited to the moving method and the tapping method.
  • the gamma ray intensity range corresponding to different material positions is repeatedly measured, and the continuous type is recorded.
  • Another point, repeated this way will get a lot of points. By connecting these points together, you can get the range of gamma ray intensity corresponding to different material heights.
  • the passive nuclear level gauge used in the embodiment mainly includes as shown in FIG.
  • gamma ray detection The Nal scintillation detector is used to measure the gamma ray intensity of the environment in which the material to be tested and the container to be tested are located; (2) a signal processing module for processing the collected gamma ray intensity signal, which is pre-set according to software The fixed switch point sends out an alarm signal, cancels the alarm signal, or outputs an electronic circuit of the continuous material level signal according to the relationship between the gamma ray intensity and the material level obtained in advance; (3) the material level signal output module for the signal processing module The output alarm signal, alarm release signal, and output signal electronic circuit can be light, sound, I/O port, relay, analog output circuit, communication interface, etc.; (4) Auxiliary module, including mounting bracket, improvement Signal-to-noise ratio ray shielding device, cable connector, antenna, handheld device for setting switching point or gamma ray intensity and material level relationship parameter, communication device for exchanging information between passive nuclear level gauges (5) software for controlling the gamma detector, processing the
  • step (c) Repeat step (b) until there is sufficient accuracy of the data, usually more than 50 times;
  • each gamma ray intensity value corresponds to a material level range, and the cover range is measured.
  • the current gray level range is obtained based on the measured gamma ray intensity N and the above-described fill level curve. Sometimes, the full value of the material is more difficult to obtain.
  • the reference method is used to measure the full value of the material, and then the algorithm is used. The steps are as follows:
  • the continuous fly ash level gauge is at the installation position, and the ash position 1 is obtained based on the measured gamma ray intensity N and the above relationship formula.
  • the material level curve shown in Fig. 3 is obtained.
  • each material level H corresponds to a gamma ray intensity range (A1, A2).
  • A1, A2 a gamma ray intensity range
  • H1, H2 a range of material levels
  • the direct method, the fitting push algorithm and the reference method can be mutually replaced according to the actual measurement conditions, and can also be used as a test method to improve the reliability of the data.

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  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Thermal Sciences (AREA)
  • Measurement Of Radiation (AREA)

Abstract

A method of determining the material-level curve in a continuous-type passive nucleonic level gauge (3), said method utilizing a direct method and comprising the following steps: first disposing the continuous-type passive nucleonic level gauge (3) in a designated position; then using other measurement means to determine the material level and, depending on measurement precision requirements, measuring the intensity of gamma rays corresponding to various material levels at points where material levels vary; and, finally, determining the material level on the basis of the actual measurement of the gamma ray intensity. An algorithm method or reference method can also be used instead of a direct method. The present invention fills a gap in the prior art by providing a method to be used with a continuous-type passive nucleonic level gauge (3) to determine the relationship between material levels and gamma ray intensity. The present invention provides a basis for accurately determining material levels by setting forth three alternative methods, i.e. a direct method, an algorithm method and a reference method, to be used depending on actual measurement conditions. The methods provide more measurement options for users depending on actual measurement conditions and, when used as testing methods, improve data reliability.

Description

一种确定连续式无源核子料位计中料位曲线的方法  Method for determining material level curve in continuous passive nuclear material level gauge
[技术领域] 本发明涉及无源核子料位测量技术领域, 具体的说是一种确定连续式无源 核子料位计中料位曲线的方法。 [Technical Field] The present invention relates to the field of passive nuclear material level measurement technology, and in particular, to a method for determining a material level curve in a continuous passive nuclear material level gauge.
[背景技术] [Background technique]
在化工、 冶金、 煤炭、 电力等行业, 在输送物料的过程中, 经常需要测量 料斗、 料仓中的料位。 现有利用伽玛射线测量物位的方法主要有两种: 一种是传统的带放射源的 核子料位计, 如国内专利 CN202230393公开的一种自动料位控制装置, 其实质 是利用左右相互对称的伽马射线柱对料位仓中的料位进行测量; 另一种则是不 带放射源, 利用被测物料和环境的天然的伽玛射线测量物位的无放射源核子料 位计, 简称无源核子料位计, 无源核子料位计使得不用放射源而只是利用被测 物料自身的伽玛放射性和被测容器所在环境中的伽玛放射性实现非接触测量物 位变得简单有效和可行, 使得原本需要使用核子料位计的领域被无源核子料位 计取代, 大大减少了放射源的使用数量, 免去了高昂的放射源管理成本, 降低 了辐射风险。  In the chemical, metallurgical, coal, electric power and other industries, in the process of conveying materials, it is often necessary to measure the material level in the hopper and silo. There are two main methods for measuring the level using gamma ray: one is a conventional nuclear level meter with a radioactive source, such as an automatic level control device disclosed in the domestic patent CN202230393, which essentially utilizes left and right mutual A symmetrical gamma ray column measures the level of the material in the material level bin; the other is a non-radio source nuclear level meter that uses the natural gamma ray to measure the level of the material and the environment without the source. , referred to as the passive nuclear material level meter, the passive nuclear material level meter makes it easy to realize the non-contact measurement level without using the radioactive source but only by using the gamma radioactivity of the measured material itself and the gamma radioactivity in the environment of the tested container. Effective and feasible, the field that originally needs to use the nuclear level gauge is replaced by a passive nuclear level gauge, which greatly reduces the number of radioactive sources used, eliminates the high cost of radioactive source management, and reduces the radiation risk.
根据料位测量的报警模式又可将无源核子料位计分为开关式和连续式两种 形式。 开关式无源核子料位计是只能分辨物料高度是否达到设定位置、 并输出 开关信号的物位计; 而连续式物位计是指能够分辨出具体的物料高度、 并输出 一种或多种连续物位信号的物位计。 对于连续式无源核子料位计来说, 料位曲线即物料高度与伽马射线强度的 对应关系曲线, 因此料位曲线的确定对准确判断料位起到非常关键的作用。 如 国内专利 CN200810017274提供了一种与现实非常不符的理想的计算方法,用来 计算出物位和测量到的放射性强度的对应曲线。 该方法为了计算方便, 首先把 体放射源简化成面状放射源, 其次把体放射源侧面的测量点的位置简化为面状 放射源上空一点, 最后又把平面上空一点的理想情况, 扩大到不符合该理想模 型的实际应用中, 由此计算出的曲线的变化趋势在测量点靠近物料分界面时, 与实际是相反的, 所以没有实用价值。 又如国内专利 CN03115824公开的一种利用天然放射性测量物位的方法, 其 方法在于已知料位的情况下, 逐渐增加物料, 同时连续测量伽玛射线放射强度, 得到物料高度和伽玛射线放射强度一一对应的点, 连接所有测量点得到一条连 续曲线即料位曲线。 该方法的适用前提为已知料位, 并且知道每个时刻的料位, 但在实际情况下, 该方法难以实现原因有三: 第一, 通常不能及时准确知道料 位; 第二、 为了得到比较准确的伽玛射线强度值, 需要一定的响应时间; 第三, 由于伽玛射线的随机性, 实际测量到的伽玛射线强度值是一个范围。 According to the alarm mode of the material level measurement, the passive nuclear material level can be divided into two types: switch mode and continuous type. The switch type passive nuclear level gauge is a level meter that can only distinguish whether the material height reaches the set position and outputs a switching signal; and the continuous level meter can distinguish the specific material height and output one or A level meter for a variety of continuous level signals. For the continuous passive nuclear level gauge, the material level curve is the corresponding relationship between the material height and the gamma ray intensity. Therefore, the determination of the material level curve plays a very important role in accurately determining the material level. Such as The domestic patent CN200810017274 provides an ideal calculation method which is very inconsistent with reality and is used to calculate the corresponding curve of the level and the measured radioactivity. For the convenience of calculation, the method firstly simplifies the bulk radioactive source into a planar radioactive source, and then simplifies the position of the measuring point on the side of the bulk radioactive source to a point above the planar radioactive source, and finally expands the ideal situation above the plane to a point. In the actual application that does not conform to the ideal model, the trend of the curve thus calculated is opposite to the actual when the measuring point is close to the material interface, so there is no practical value. Another method disclosed in the domestic patent CN03115824 for measuring the level using natural radioactivity is characterized in that, in the case of a known material level, the material is gradually increased, and the gamma ray radiation intensity is continuously measured to obtain the material height and gamma ray emission. A point where the intensity corresponds one-to-one, connecting all the measurement points to obtain a continuous curve, that is, the material level curve. The applicable premise of the method is the known material level, and the material level at each moment is known, but in actual cases, the method is difficult to achieve for three reasons: First, the material level cannot usually be accurately known in time; Second, in order to compare Accurate gamma ray intensity values require a certain response time. Third, due to the randomness of gamma rays, the actual measured gamma ray intensity value is a range.
[发明内容] [Summary of the Invention]
本发明的目的在于弥补现有技术的不足, 提供一种可精准确定连续式无源 核子料位计中料位曲线的方法。  The object of the present invention is to make up for the deficiencies of the prior art and to provide a method for accurately determining the material level curve in a continuous passive nuclear level gauge.
为实现上述目的, 设计一种确定连续式无源核子料位计中料位曲线的方法, 包括测量装置和计算模块, 其特征在于该方法采用直接法, 包含以下步骤: In order to achieve the above object, a method for determining a material level curve in a continuous passive nuclear level gauge is designed, which comprises a measuring device and a calculation module, characterized in that the method adopts a direct method and comprises the following steps:
(a)将连续式无源核子料位计安装在选定位置, 使其安装高度符合报警的 高度要求, 安装方向要使得其中的伽玛马射线探测器能探测被测物料和被测容 器的伽玛射线强度; (a) Install the continuous passive nuclear level gauge at the selected position so that the installation height meets the height requirements of the alarm. The installation direction is such that the gamma ray detector can detect the material to be tested and the container to be tested. Gamma ray intensity;
(b )在测量范围内任意的一个可知的料位处, 记录连续式无源核子料位计 测量到的伽马射线强度及其变化范围, 得到料位与伽马射线强度平面上的一个 线段; (c ) 按照所需测量精度, 改变料位, 记录连续式无源核子料位计测量到的 伽马射线强度及其变化范围, 得到料位与伽马射线强度平面上的另一个线段;(b) Record the intensity of the gamma ray measured by the continuous passive nuclear level gauge and its range of variation at any known level within the measurement range, and obtain a line segment on the level of the level and the gamma ray intensity plane. ; (c) Change the material level according to the required measurement accuracy, record the intensity of the gamma ray measured by the continuous passive nuclear level gauge and its variation range, and obtain another line segment on the level of the level and the gamma ray intensity plane;
( d ) 重复步骤 (C ) ; ( d ) repeat step (C) ;
(e ) 连接得到的线段的最大点, 再连接得到的线段的最小点, 得到不同料 位对应的伽马射线强度的变化趋势, 即比较粗的一条料位曲线;  (e) connecting the maximum point of the obtained line segment, and then connecting the minimum point of the obtained line segment, to obtain the change trend of the gamma ray intensity corresponding to different material positions, that is, a relatively thick material level curve;
( f )根据该料位曲线, 依实际测量的伽玛射线强度得到料位的范围, 其中 间值就是被测料位。  (f) According to the material level curve, the range of the material level is obtained according to the actual measured gamma ray intensity, and the middle value is the measured material level.
该方法采用推算法替代直接法, 包含以下步骤:  The method uses a push algorithm instead of the direct method and includes the following steps:
(a) 线性拟合推算, 在料满 (料位为 H) 时, 测量伽玛射线强度 Nh; 在料 空 (料位为 L) 时, 测出伽玛射线强度 Nl, 实际测量时, 当测到的伽玛射线强 度为 N, 则此时的料位依计算公式 h=L+ (H-L) * (N-Nl) I (Nh-Nl)计算得出。  (a) Linear fitting calculation, measuring the gamma ray intensity Nh when the material is full (the material level is H); and measuring the gamma ray intensity Nl when the material space is empty (the material level is L), when actually measuring The measured gamma ray intensity is N, and the material level at this time is calculated according to the calculation formula h=L+ (HL) * (N-Nl) I (Nh-Nl).
(b ) 曲线拟合推算, 测出料满和料空两个伽玛射线强度值, 再多次改变料 位, 利用移动定位法确定该料位值, 同时测出对应该料位的伽玛射线强度, 得 到包括料满和料空在内的多个料位和伽玛射线强度的对应点, 再利用三次曲线 拟合这些点, 得到伽玛射线强度和料位的关系曲线, 实际测量时, 用测量到的 伽玛射线强度值和该关系曲线, 计算对应的料位。  (b) Calculate the curve fitting, measure the two gamma ray intensity values of the material full and the material empty, change the material level multiple times, determine the material level value by the mobile positioning method, and measure the gamma corresponding to the material level. The intensity of the ray is obtained, and the corresponding points of the plurality of material levels and the gamma ray intensity including the full material and the material empty are obtained, and the three curves are used to fit the points, and the relationship between the gamma ray intensity and the material level is obtained, and the actual measurement time is obtained. Calculate the corresponding level by using the measured gamma ray intensity value and the relationship curve.
该方法采用参考法替代直接法, 包含以下步骤:  The method uses a reference method instead of the direct method and includes the following steps:
(a)在被测容器附近环境辐射相似处, 选择可以确定料位的、 装同一种被 测物料的、 相似容器, 并将连续式无源核子料位计安装在与被测容器的测量位 置相似的位置;  (a) In the vicinity of the environmental radiation near the container to be tested, select a similar container that can be used to determine the material level, and install the continuous passive nuclear level gauge in the measurement position with the container to be tested. Similar location
(b) 测量料满和料空时的伽玛射线强度 Nh和 Nl, 做为实际被测容器处的 料满和料空时的伽玛射线强度 Nh和 Nl。  (b) Measure the gamma ray intensities Nh and Nl at the full and empty, as the gamma ray intensities Nh and Nl at the actual container and at the material empty.
(c )将连续式无源核子料位计安装回被测容器的选定位置, 实际测量伽玛 射线强度 N, 并用刚才确定的料空、 料满射线强度 Nh和 Nl, 按照推算法得到实 际料位 h=L+ (H-L) * (N-Nl) I (Nh-Nl)。  (c) Install the continuous passive nuclear level gauge back to the selected position of the container to be tested, actually measure the gamma ray intensity N, and use the material space and material full ray intensity Nh and Nl just determined, according to the algorithm Level h = L + (HL) * (N-Nl) I (Nh-Nl).
所述推算法适用于能确定被测容器内满料和完全料空两种状态的情况, 包 括不能确定具体中间料位的情况, 得到伽玛射线强度和料位的对应关系。 所述参考法适用于所有情况, 包括不能确定实际的料位, 也不能确定被测 容器内料满、 料空状态的情况。 The push algorithm is applicable to the situation that the two states of the filled container and the complete material empty can be determined, including the case where the specific intermediate material level cannot be determined, and the corresponding relationship between the gamma ray intensity and the material level is obtained. The reference method is applicable to all situations, including the inability to determine the actual level, and the determination of the full and empty state of the container under test.
所述推算法和参考法中的料位曲线是一条比较粗的曲线, 每个料位对应一 个伽玛射线强度范围; 每一个测量到的伽玛射线强度在这条曲线上也对应一个 料位范围, 该范围就是该连续式无源核子料位计的测量精度; 所述的推算法中的曲线拟合中用的移动定位法, 是在某一料位状态下, 从 上向下或从下向上移动连续式无源核子料位计, 同时测量伽玛射线强度, 得到 一组变化的数据, 该组数据中相邻两个数据的差最大的数所对应的连续式无源 核子料位计的测量位置就是实际料位。 本发明与现有技术相比, 弥补了现有技术的空白, 提供了适用于连续式无 源核子料位计的确定料位与伽马射线强度关系的方法, 为准确测定料位提供坚 实基础, 本发明提出直接法、 拟合推算法及参考法三种可依实际测量情况相互 替换的方法, 既增加了用户测量时依实际测量情况的选择性, 又可作为检验方 法提高数据的可信度。  The material level curve in the push algorithm and the reference method is a relatively thick curve, and each material level corresponds to a gamma ray intensity range; each measured gamma ray intensity also corresponds to a material level on the curve. Range, the range is the measurement accuracy of the continuous passive nuclear level gauge; the moving positioning method used in the curve fitting in the push algorithm is in a certain level state, from top to bottom or from Moving the continuous passive nuclear level gauge down and up, simultaneously measuring the intensity of the gamma ray, and obtaining a set of changed data. The continuous passive nuclear level corresponding to the largest difference between two adjacent data in the set of data The measured position of the meter is the actual level. Compared with the prior art, the present invention makes up for the gap of the prior art, and provides a method for determining the relationship between the material level and the gamma ray intensity of the continuous passive nuclear level gauge, which provides a solid foundation for accurately determining the material level. The invention proposes a direct method, a fitting push algorithm and a reference method, which can replace each other according to the actual measurement situation, which not only increases the selectivity of the user according to the actual measurement situation, but also can be used as a test method to improve the reliability of the data. degree.
[附图说明] 图 1是本发明涉及的无源核子料位计内部硬件结构示意图; 图 2是本发明涉及的无源核子料位计应用示意图; 图 3是本发明实施例测量到的料位曲线图; 图中 1.物料 2.被测容器 3. 无源核子料位计 4.无源核子料位计支架 [具体实施方式] 结合附图对本发明做进一步说明, 该方法对本领域专业技术人员来说是可 以实现的。 本发明方法的提出是为了适用于连续式料位计, 希望随着物料高度的变化、 连续输出精确的物位信号, 设计的基本方案为: 在确定好的测量点位置安装符 合灵敏度要求的连续式无源核子料位计, 在确定的响应时间内测量伽玛射线强 度, 确定测量到的伽玛射线强度和物位的关系曲线, 依实际测量到的伽玛射线 强度值, 输出被测料位。 BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a schematic diagram showing the internal hardware structure of a passive nuclear level gauge according to the present invention; FIG. 2 is a schematic diagram of the application of a passive nuclear level gauge according to the present invention; Bit diagram; Figure 1. Material 2. Container to be tested 3. Passive nuclear level gauge 4. Passive nuclear level gauge bracket [Detailed Description] The present invention will be further described with reference to the accompanying drawings, which is specialized in the field. The technician is OK To achieve. The method of the present invention is proposed to be applied to a continuous level gauge. It is desirable to continuously output an accurate level signal as the height of the material changes. The basic design of the design is: Continually install a sensitivity point at a determined measurement point. Passive nuclear level gauge, measure the intensity of gamma ray in a determined response time, determine the relationship between the measured gamma ray intensity and the level, and output the measured material according to the actual measured gamma ray intensity value. Bit.
本发明提出的直接法的实现要结合其他方法先确定料位, 方法不局限于移 动法和敲击法, 按照测量精度要求, 反复测量不同料位对应的伽玛射线强度范 围, 记录连续式无源核子料位计测量到的伽玛射线强度及其变化范围, 由此得 到料位曲线上的一个点, 然后再用各种方法, 改变料位, 重复上述步骤, 又会 得到料位曲线上的另外一个点, 如此反复重复, 会得到许多点, 把这些点连起 来, 就能得到不同料位高度对应的伽玛射线强度的变化范围。 实际上这样得到 的是一条比较 "粗" 的、 每个料位对应一个伽玛射线强度范围、 每一个伽玛射 线强度值也对应一个料位范围的料位曲线。 尽量找到足够多的点使得连起来的 曲线平滑, 由测量到的伽玛射线强度值对应的料位范围符合连续式无源核子料 位计的精度要求。 然后依据实际测量的伽玛射线强度判定料位范围。 将本发明提供的方法应用于连续式飞灰料位计中, 测量电除尘器或布袋除 尘器灰斗的料位, 所用的电除尘器或布袋除尘器灰斗如图 2所示为倒四棱锥形 钢板结构、 高度 5-8米、 倾角 60度、 外部设有 20-40cm厚的保温材料和保护保 温材料的彩钢板, 内部被测物料是煤粉燃烧后形成的温度在 135-45CTC的飞灰, 鉴于飞灰的温度、 黏性和落灰的冲击力及其较强的伽玛放射性, 在灰斗灰位监 测上采用本发明所述的方法是非常理想的。 实施例中使用的无源核子料位计如图 1所示主要包括: (1 ) 伽玛射线探测 器, 选用 Nal闪烁探测器, 用于测量被测物料和被测容器所在环境的伽玛射线 强度; (2 ) 信号处理模块, 用于处理所收集的伽玛射线强度信号, 结合软件根 据预先设定的开关点发出报警信号、 解除报警信号, 或根据预先取得的伽玛射 线强度与料位的关系输出连续料位信号的电子线路; (3 ) 料位信号输出模块, 用于把信号处理模块输出的报警信号、 报警解除信号、 料位信号输出的电子线 路, 可以是灯光、 声音、 I/O口、 继电器、 模拟量输出电路、 通信接口等; (4) 辅助模块, 包括安装支架、 改善信噪比的射线屏蔽装置、 电缆接头、 天线、 用 于设定开关点或伽玛射线强度与料位的关系曲线参数的手持设备、 用于无源核 子料位计之间交换信息的通信设备等; (5 ) 软件, 用于控制伽玛探测器, 处理 伽玛信号并输出报警信号、 解除报警信号、 或连续料位信号, 实现通信或人机 对话等等功能的所有相关代码的集合。 采用直接法测量步骤如下: The implementation of the direct method proposed by the present invention should first determine the material level in combination with other methods. The method is not limited to the moving method and the tapping method. According to the measurement accuracy requirement, the gamma ray intensity range corresponding to different material positions is repeatedly measured, and the continuous type is recorded. The intensity of the gamma ray measured by the source nuclear level gauge and its range of variation, thereby obtaining a point on the level curve, and then using various methods to change the level, repeating the above steps, and then obtaining the level curve. Another point, repeated this way, will get a lot of points. By connecting these points together, you can get the range of gamma ray intensity corresponding to different material heights. In fact, what is obtained is a relatively "coarse" material level curve corresponding to one gamma ray intensity range for each material level and one gamma ray intensity value corresponding to one material level range. Try to find enough points to make the connected curve smooth. The measured range of the gamma ray intensity corresponds to the accuracy requirement of the continuous passive nuclear level gauge. The fill level is then determined based on the actual measured gamma ray intensity. The method provided by the invention is applied to a continuous fly ash level gauge, and the level of the ash hopper of the electrostatic precipitator or the bag filter is measured. The hopper of the electric precipitator or the bag filter is used as shown in FIG. 2 Pyramid steel plate structure, height 5-8 meters, inclination angle 60 degrees, externally provided with 20-40cm thick insulation material and color steel plate for protection of thermal insulation material, the internal measured material is the temperature formed after pulverized coal combustion is 135-45CTC Fly ash, in view of the temperature, viscosity and ash impact of fly ash and its strong gamma radioactivity, it is highly desirable to employ the method described herein for ash ash monitoring. The passive nuclear level gauge used in the embodiment mainly includes as shown in FIG. 1 : (1) gamma ray detection The Nal scintillation detector is used to measure the gamma ray intensity of the environment in which the material to be tested and the container to be tested are located; (2) a signal processing module for processing the collected gamma ray intensity signal, which is pre-set according to software The fixed switch point sends out an alarm signal, cancels the alarm signal, or outputs an electronic circuit of the continuous material level signal according to the relationship between the gamma ray intensity and the material level obtained in advance; (3) the material level signal output module for the signal processing module The output alarm signal, alarm release signal, and output signal electronic circuit can be light, sound, I/O port, relay, analog output circuit, communication interface, etc.; (4) Auxiliary module, including mounting bracket, improvement Signal-to-noise ratio ray shielding device, cable connector, antenna, handheld device for setting switching point or gamma ray intensity and material level relationship parameter, communication device for exchanging information between passive nuclear level gauges (5) software for controlling the gamma detector, processing the gamma signal and outputting the alarm signal, releasing the alarm signal , Or a continuous set of all relevant material code signal, or interactive communication to achieve like functionality. The direct measurement method is as follows:
(a)将连续式飞灰料位计安装在灰斗高度的 3/4位置处, 使得连续式飞灰 料位计的探测方向对准灰斗, 并开始测量伽马射线强度;  (a) Install a continuous fly ash level gauge at 3/4 of the hopper height so that the direction of detection of the continuous fly ash level gauge is aligned with the hopper and begins to measure gamma ray intensity;
(b ) 改变料位, 用其他料位测量设备测量并确认料位, 记录连续式无源核 子料位计测量到的伽马射线强度及其在可信度为 99%时的变化范围,得到料位曲 线上的一个线段;  (b) Change the material level, measure and confirm the material level with other material level measuring equipment, record the gamma ray intensity measured by the continuous passive nuclear level meter and its variation range when the reliability is 99%. a line segment on the level curve;
(c ) 重复步骤 (b), 直到有足够精度的数据, 通常要 50次以上;  (c) Repeat step (b) until there is sufficient accuracy of the data, usually more than 50 times;
(d) 连接得到的线段, 得到不同料位对应的伽马射线强度的变化趋势, 即 料位曲线, 依据该料位曲线, 每个伽玛射线强度值对应一个料位范围, 盖范围 就是测量精度;  (d) Connect the obtained line segments to obtain the change trend of the gamma ray intensity corresponding to different material levels, that is, the material level curve. According to the material level curve, each gamma ray intensity value corresponds to a material level range, and the cover range is measured. Accuracy
(e ) 根据实测的伽玛射线强度 N和上述的料位曲线, 得到当前灰位范围。 由于确认料位比较困难, 但是可以确认料满和料空这两个状态, 就采用推 (a)将连续式飞灰料位计安装在灰斗高度的 3/4位置处, 使得连续式飞灰 料位计的探测方向对准灰斗, 并开始测量伽马射线强度; (e) The current gray level range is obtained based on the measured gamma ray intensity N and the above-described fill level curve. Since it is difficult to confirm the material level, but it can be confirmed that the two states of the material and the material are empty, the push is adopted. (a) Install the continuous fly ash level gauge at the 3/4 position of the hopper height so that the detection direction of the continuous fly ash level gauge is aligned with the hopper and begins to measure the gamma ray intensity;
(b) 在灰斗全空时 (灰位为 L), 测得料空伽玛射线强度 N1;  (b) When the hopper is completely empty (gray is L), the measured gamma ray intensity N1 is measured;
(c) 在根据经验确认灰斗全满时 (灰位为 H), 测得料空伽玛射线强度 Nh; (c) When it is empirically confirmed that the hopper is full (gray position H), the gamma ray intensity Nh is measured;
( d ) 在实际测量时, 测到的伽玛射线强度 N与此时的灰位 h的关系: h=L+ (H-L) * (N-Nl) I (Nh-Nl), 并输入连续式飞灰料位计; (d) In the actual measurement, the relationship between the measured gamma ray intensity N and the gray position h at this time: h=L+ (HL) * (N-Nl) I (Nh-Nl), and input continuous flight Ash level gauge;
(e ) 根据实测的伽玛射线强度 N和上述的料位曲线, 得到当前灰位范围。 有时, 料满值也比较难获得, 用参考法测量料满值, 再用推算法, 步骤如 下:  (e) The current gray level range is obtained based on the measured gamma ray intensity N and the above-described fill level curve. Sometimes, the full value of the material is more difficult to obtain. The reference method is used to measure the full value of the material, and then the algorithm is used. The steps are as follows:
(a)将连续式飞灰料位计安装在灰斗高度的 3/4位置处, 使得连续式飞灰 料位计的探测方向对准灰斗;  (a) Install the continuous fly ash level gauge at the 3/4 position of the hopper height so that the detection direction of the continuous fly ash level gauge is aligned with the ash hopper;
(b) 在灰斗全空时 (料位为 L), 测得料空伽玛射线强度 N1;  (b) When the hopper is completely empty (level L), the measured gamma ray intensity N1;
(c )将连续式飞灰料位计拿下来, 在安装位置的下面不同高度处, 与灰斗 保持相同距离, 对着灰斗测量。 用移动定位法判断灰位, 确认灰位到一半以上 后, 在灰斗下半部分, 找到伽玛射线强度最强的区域, 以此最强伽玛射线强度 近似为料满伽玛射线强度 Nh; (c) Take the continuous fly ash level gauge down, at the same height below the installation location, at the same distance from the hopper, against the ash bucket. The gray position is judged by the moving positioning method, and after confirming that the gray level is more than half, the area with the strongest gamma ray intensity is found in the lower half of the ash bucket, and the strongest gamma ray intensity is approximated as the full gamma ray intensity Nh. ;
(d)将连续式飞灰料位计安装回安装位置, 测到的伽玛射线强度 N与此时 的灰位 h的关系: h=L+ (H-L) * (N-N1) / (Nh-Nl), 并输入连续式飞灰料位计; (d) Install the continuous fly ash level gauge back to the installation position, and measure the relationship between the measured gamma ray intensity N and the ash h at this time: h=L+ (HL) * (N-N1) / (Nh- Nl), and input continuous fly ash level gauge;
(e )连续式飞灰料位计在安装位置, 根据实测的伽玛射线强度 N和上述的 关系公式, 得到灰位1。 依据上述方法得到如图 3所示的料位曲线, 随着料位高度的增加, 伽马射 线放射强度呈上升趋势, 每一个料位 H对应一个伽玛射线强度范围 (A1,A2), 实 际测量时, 每测量到一个伽玛射线强度值 A, 它所对应的也是一个料位的范围 (H1,H2), 亦即测量精度。 直接法、 拟合推算法及参考法三种方法可依据实际测 量工况相互替换, 亦可作为检验方法, 提高数据的可信度。 (e) The continuous fly ash level gauge is at the installation position, and the ash position 1 is obtained based on the measured gamma ray intensity N and the above relationship formula. According to the above method, the material level curve shown in Fig. 3 is obtained. As the height of the material level increases, the gamma ray radiation intensity increases, and each material level H corresponds to a gamma ray intensity range (A1, A2). When measuring, each time a gamma ray intensity value A is measured, it corresponds to a range of material levels (H1, H2), which is the measurement accuracy. The direct method, the fitting push algorithm and the reference method can be mutually replaced according to the actual measurement conditions, and can also be used as a test method to improve the reliability of the data.

Claims

1. 一种确定连续式无源核子料位计中料位曲线的方法,包括测量装置和计算模 块, 其特征在于该方法采用直接法, 包含以下步骤: A method for determining a fill level curve in a continuous passive nuclear level gauge, comprising a measuring device and a computing module, characterized in that the method employs a direct method comprising the steps of:
(a) 将连续式无源核子料位计安装在选定位置, 使其安装高度符合报警的高 度要求, 安装方向要使得其中的伽玛马射线探测器能探测被测物料和被测容器 的伽玛射线强度; (a) Install the continuous passive nuclear level gauge at the selected position so that the installation height meets the height requirements of the alarm. The installation direction is such that the gamma ray detector can detect the material to be tested and the container to be tested. Gamma ray intensity;
(b ) 在测量范围内任意的一个可知的料位处, 记录连续式无源核子料位计测 量到的伽马射线强度及其变化范围,得到料位与伽马射线强度平面上的一个线 段;  (b) Record the intensity of the gamma ray measured by the continuous passive nuclear level gauge and its range of variation at any known level within the measurement range to obtain a line segment on the level of the fill level and the gamma ray intensity ;
(c ) 按照所需测量精度, 改变料位, 记录连续式无源核子料位计测量到的伽 马射线强度及其变化范围, 得到料位与伽马射线强度平面上的另一个线段; (c) Change the level of the material according to the required measurement accuracy, record the intensity of the gamma ray measured by the continuous passive nuclear level gauge and its range of variation, and obtain another line segment on the level of the level and the gamma ray intensity plane;
(d) 重复步骤 (c); (d) repeat step (c);
( e ) 连接得到的线段的最大点, 再连接得到的线段的最小点, 得到不同料位 对应的伽马射线强度的变化趋势, 即比较粗的一条料位曲线;  (e) connecting the maximum point of the obtained line segment, and then connecting the minimum point of the obtained line segment to obtain a change trend of the gamma ray intensity corresponding to different material levels, that is, a relatively thick material level curve;
(f ) 根据该料位曲线, 依实际测量的伽玛射线强度得到料位的范围, 其中间 值就是被测料位。  (f) According to the material level curve, the range of the material level is obtained according to the actual measured gamma ray intensity, and the middle value is the measured material level.
2.如权利要求 1所述的一种确定连续式无源核子料位计中料位曲线的方法,其 特征在于该方法采用推算法替代直接法, 包含以下步骤:  2. A method of determining a fill level curve in a continuous passive nuclear level gauge according to claim 1 wherein the method employs a push algorithm instead of a direct method comprising the following steps:
(a) 线性拟合推算, 在料满 (料位为 H) 时, 测量伽玛射线强度 Nh; 在料空 (料位为 L) 时, 测出伽玛射线强度 Nl, 实际测量时, 当测到的伽玛射线强度 为 N, 则此时的料位依计算公式 h=L+ (H-L) * (N-Nl) I (Nh-Nl)计算得出; (a) Linear fitting estimation, measuring the gamma ray intensity Nh when the material is full (feed level H) ; when the material space is empty (level L), the gamma ray intensity Nl is measured, when actually measuring The measured gamma ray intensity is N, and the material level at this time is calculated according to the calculation formula h=L+ (HL) * (N-Nl) I (Nh-Nl);
(b) 曲线拟合推算, 测出料满和料空两个伽玛射线强度值, 再多次改变料位, 利用移动定位法确定该料位值, 同时测出对应该料位的伽玛射线强度, 得到包 括料满和料空在内的多个料位和伽玛射线强度的对应点,再利用三次曲线拟合 这些点, 得到伽玛射线强度和料位的关系曲线, 实际测量时, 用测量到的伽玛 射线强度值和该关系曲线, 计算对应的料位。  (b) Calculate the curve fitting, measure the two gamma ray intensity values of the material full and the material empty, change the material level multiple times, determine the material level value by the mobile positioning method, and measure the gamma corresponding to the material level. The ray intensity is obtained, and the corresponding points of the plurality of material levels and the gamma ray intensity including the full material and the material empty are obtained, and the three curves are used to fit the points, and the relationship between the gamma ray intensity and the material level is obtained, and the actual measurement time is obtained. Calculate the corresponding level by using the measured gamma ray intensity value and the relationship curve.
3. 如权利要求 1所述的一种确定连续式无源核子料位计中料位曲线的方法, 其特征在于该方法采用参考法替代直接法, 包含以下步骤: (a) 在被测容器附近环境辐射相似处, 选择可以确定料位的、 装同一种被测 物料的、 相似容器, 并将连续式无源核子料位计安装在与被测容器的测量位置 相似的位置; 3. A method of determining a fill level curve in a continuous passive nuclear level gauge according to claim 1, wherein the method uses a reference method instead of the direct method, comprising the steps of: (a) In the vicinity of the environmental radiation near the container to be tested, select a similar container that can be used to determine the material level, and install the continuous passive nuclear level gauge in the measurement position with the container to be tested. Similar location
(b)测量料满和料空时的伽玛射线强度 Nh和 Nl,做为实际被测容器处的料满 和料空时的伽玛射线强度 Nh和 N1; (b) Measure the gamma ray intensities Nh and Nl when the material is full and empty, as the gamma ray intensities Nh and N1 when the material is actually filled and empty;
(c) 将连续式无源核子料位计安装回被测容器的选定位置, 实际测量伽玛射 线强度 N, 并用刚才确定的料空、 料满射线强度 Nh和 Nl, 按照推算法得到实 际料位 h=L+ (H-L) * (N-Nl) I (Nh-Nl)。 (c) Install the continuous passive nuclear level gauge back to the selected position of the container under test, actually measure the gamma ray intensity N, and use the material space and material full ray intensity Nh and Nl just determined, according to the algorithm Level h = L + (HL) * (N-Nl) I (Nh-Nl).
4.如权利要求 1或 2所述的一种确定连续式无源核子料位计中料位曲线的方 法,其特征在于所述推算法适用于能确定被测容器内满料和完全料空两种状态 的情况, 包括不能确定具体中间料位的情况, 得到伽玛射线强度和料位的对应 关系。 4. A method for determining a fill level curve in a continuous passive nuclear level gauge according to claim 1 or 2, wherein the push algorithm is adapted to determine that the measured container is full and completely empty. In the case of two states, including the case where the specific intermediate level cannot be determined, the correspondence between the gamma ray intensity and the material level is obtained.
5.如权利要求 1或 3所述的一种确定连续式无源核子料位计中料位曲线的方 法, 其特征在于所述参考法适用于所有情况, 包括不能确定实际的料位, 也不 能确定被测容器内料满、 料空状态的情况。 5. A method of determining a fill level curve in a continuous passive nuclear level gauge according to claim 1 or 3, wherein said reference method is applicable to all situations, including the inability to determine the actual fill level, It is not possible to determine the condition in which the measured container is full and empty.
6.如权利要求 1或 2或 3所述的一种确定连续式无源核子料位计中料位曲线的 方法, 其特征在于: 6. A method of determining a fill level curve in a continuous passive nuclear level gauge according to claim 1 or 2 or 3, wherein:
(a) 料位曲线是一条比较粗的曲线, 每个料位对应一个伽玛射线强度范围; (a) The fill level curve is a relatively thick curve, each level corresponding to a gamma ray intensity range;
(b ) 每一个测量到的伽玛射线强度在这条曲线上也对应一个料位范围, 该范 (b) Each measured gamma ray intensity also corresponds to a fill level on this curve, the range
7.如权利要求 2所述的一种确定连续式无源核子料位计中料位曲线的方法中的 曲线拟合推算中用移动定位法, 其特征在于: (a) 在某一料位状态下, 从上向下或从下向上移动连续式无源核子料位计, 同时测量伽玛射线强度, 得到一组变化的数据; 7 . The mobile positioning method used in the curve fitting estimation method for determining a material level curve in a continuous passive nuclear material level meter according to claim 2 , wherein: (a) moving the continuous passive nuclear level gauge from top to bottom or from bottom to top at a certain level, and simultaneously measuring the intensity of the gamma ray to obtain a set of varying data;
(b) 该组数据中相邻两个数据的差最大的数所对应的连续式无源核子料位计 的测量位置就是实际料位。  (b) The measurement position of the continuous passive nuclear level gauge corresponding to the largest difference between two adjacent data in the set of data is the actual level.
PCT/CN2012/080196 2012-06-19 2012-08-16 Method of determining material-level curve in continuous-type passive nucleonic level gauge WO2013189124A1 (en)

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Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104089681A (en) * 2014-07-03 2014-10-08 胡桂标 Portable level gage
CN104390677B (en) * 2014-11-08 2018-03-13 胡桂标 The background radiation amendment measuring method and its system of passive nuclear level sensing device
CN104482996B (en) * 2014-12-24 2019-03-15 胡桂标 The material kind of passive nuclear level sensing device corrects measuring system
CN104568061A (en) * 2015-01-14 2015-04-29 上海沃纳机电科技有限公司 Multi-probe passive nuclear level meter
CN108387293A (en) * 2018-06-05 2018-08-10 上海云鱼智能科技有限公司 The passive nuclear level sensing device of combined type mechanically and its measurement method
CN113375757B (en) * 2020-03-27 2022-12-02 洛森自动化科技(上海)有限公司 Method for measuring material level by applying curve simulation and nuclear radiation principle
CN114166157B (en) * 2021-12-08 2023-10-20 国能锅炉压力容器检验有限公司 Intelligent quantitative method for oxide skin in tube according to ray intensity curve
CN115178339B (en) * 2022-04-11 2023-04-25 北京智冶互联科技有限公司 Automatic control method and device for rolling operation, electronic equipment and medium

Citations (17)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3594575A (en) * 1968-08-30 1971-07-20 Industrial Nucleonics Corp Linearization of radiation gauges for measuring the quantity of fluidic materials in containers
CN87106698A (en) * 1986-09-03 1988-03-23 卡尔斯鲁厄核子研究中心股份公司 Apparatus for measuring charge level
SU1506282A1 (en) * 1985-02-01 1989-09-07 Специализированное конструкторско-технологическое бюро с опытным производством Института электроники им.У.А.Арифова Device for measuring liquid level
JPH0274827A (en) * 1988-09-10 1990-03-14 Aasunikusu Kk Gamma-ray level gage
CN1193103A (en) * 1998-01-21 1998-09-16 太原理工大学 Passive liquid-level sensor
CN2337541Y (en) * 1997-11-27 1999-09-08 唐山冀油东大技术开发有限公司 Marker type floating-roof raw oil tank liquid level meter apparatus
WO2003052396A2 (en) * 2001-12-19 2003-06-26 Endress + Hauser Gmbh + Co. Kg Methods and devices for erasing errors and compensating interference signals caused by gammagraphy in radiometric measuring systems
CN1466674A (en) * 2000-09-27 2004-01-07 ������˹�ͺ�ɪ�����Ϲ�˾ Method for detecting the limit state of a material and device thereof
CN2869804Y (en) * 2005-10-10 2007-02-14 中国石油天然气股份有限公司 Large coke tower material level continuous measuring device
CN1995928A (en) * 2006-11-29 2007-07-11 上海辉博自动化仪表有限公司 Non-contact type article position measuring method using auxiliary materials for replacement of radioactive source
US20070278404A1 (en) * 2004-02-16 2007-12-06 Endress + Co. Kg Radiometric Measuring Device
CN101629840A (en) * 2009-06-23 2010-01-20 丹东东方测控技术有限公司 Mobile measuring instrument and measuring method of material level in storage warehouse
CN101644595A (en) * 2009-09-01 2010-02-10 南京大学 Fitting method of complex water level process
CN101782417A (en) * 2010-02-01 2010-07-21 河海大学 Method and device for automatically measuring water-level variation
CN101855524A (en) * 2007-11-09 2010-10-06 恩德莱斯和豪瑟尔两合公司 Radiometric two-wire measuring device for measurement of a fill level
CN101910806A (en) * 2008-01-10 2010-12-08 罗伯特·博世有限公司 Capacitive fill level sensor and method for estimating a fill level
CN101936923A (en) * 2010-09-29 2011-01-05 上海辉博自动化仪表有限公司 Non-contact material level measuring device

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN2788151Y (en) * 2005-01-06 2006-06-14 黑龙江省中贝技术有限公司 Multi-passage principal and subordinate type nucleus substance position monitoring device
GB0705449D0 (en) * 2007-03-22 2007-05-02 Siemens Milltronics Proc Instr A high frequency radar system
CN101246033B (en) * 2008-01-11 2010-07-07 陈群英 Method for measuring coal ash material position using nuclear radiation field theory

Patent Citations (17)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3594575A (en) * 1968-08-30 1971-07-20 Industrial Nucleonics Corp Linearization of radiation gauges for measuring the quantity of fluidic materials in containers
SU1506282A1 (en) * 1985-02-01 1989-09-07 Специализированное конструкторско-технологическое бюро с опытным производством Института электроники им.У.А.Арифова Device for measuring liquid level
CN87106698A (en) * 1986-09-03 1988-03-23 卡尔斯鲁厄核子研究中心股份公司 Apparatus for measuring charge level
JPH0274827A (en) * 1988-09-10 1990-03-14 Aasunikusu Kk Gamma-ray level gage
CN2337541Y (en) * 1997-11-27 1999-09-08 唐山冀油东大技术开发有限公司 Marker type floating-roof raw oil tank liquid level meter apparatus
CN1193103A (en) * 1998-01-21 1998-09-16 太原理工大学 Passive liquid-level sensor
CN1466674A (en) * 2000-09-27 2004-01-07 ������˹�ͺ�ɪ�����Ϲ�˾ Method for detecting the limit state of a material and device thereof
WO2003052396A2 (en) * 2001-12-19 2003-06-26 Endress + Hauser Gmbh + Co. Kg Methods and devices for erasing errors and compensating interference signals caused by gammagraphy in radiometric measuring systems
US20070278404A1 (en) * 2004-02-16 2007-12-06 Endress + Co. Kg Radiometric Measuring Device
CN2869804Y (en) * 2005-10-10 2007-02-14 中国石油天然气股份有限公司 Large coke tower material level continuous measuring device
CN1995928A (en) * 2006-11-29 2007-07-11 上海辉博自动化仪表有限公司 Non-contact type article position measuring method using auxiliary materials for replacement of radioactive source
CN101855524A (en) * 2007-11-09 2010-10-06 恩德莱斯和豪瑟尔两合公司 Radiometric two-wire measuring device for measurement of a fill level
CN101910806A (en) * 2008-01-10 2010-12-08 罗伯特·博世有限公司 Capacitive fill level sensor and method for estimating a fill level
CN101629840A (en) * 2009-06-23 2010-01-20 丹东东方测控技术有限公司 Mobile measuring instrument and measuring method of material level in storage warehouse
CN101644595A (en) * 2009-09-01 2010-02-10 南京大学 Fitting method of complex water level process
CN101782417A (en) * 2010-02-01 2010-07-21 河海大学 Method and device for automatically measuring water-level variation
CN101936923A (en) * 2010-09-29 2011-01-05 上海辉博自动化仪表有限公司 Non-contact material level measuring device

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