CN101819140A - Continuous monitoring device and method of gaseous elemental mercury concentration - Google Patents

Continuous monitoring device and method of gaseous elemental mercury concentration Download PDF

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CN101819140A
CN101819140A CN 201010171418 CN201010171418A CN101819140A CN 101819140 A CN101819140 A CN 101819140A CN 201010171418 CN201010171418 CN 201010171418 CN 201010171418 A CN201010171418 A CN 201010171418A CN 101819140 A CN101819140 A CN 101819140A
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mercury
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CN101819140B (en
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娄秀涛
王鹏
王华山
张云刚
陈斌
瑞小川
张治国
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Harbin Institute of Technology Shenzhen
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Abstract

气态单质汞浓度的连续监测装置和方法,涉及气体浓度的测量领域,解决了现有的气态单质汞监测技术灵敏度低、系统复杂和成本过高的问题。本发明的装置,汞元素灯置于磁铁的磁场中,输出光经准直透镜透射得到平行光,平行光经过样品池后入射至分光镜,透射光经过参考池后入射至第一凸透镜,聚焦至第一探测器,反射光入射至第二凸透镜,聚焦至第二探测器,第一探测器和第二探测器与数据采集分析器连接。本发明的方法,具体如下:一、确定光强对比度M为零所对应的常数A;二、描绘光强对比度M与气态单质汞介质浓度的对应关系曲线;三、测量待测气态单质汞介质的光强对比度M,并与对应关系曲线对照,得到待测气态单质汞介质的浓度。用于监测气态汞浓度。

The device and method for continuous monitoring of gaseous elemental mercury concentration relate to the field of gas concentration measurement, and solve the problems of low sensitivity, system complexity and high cost of the existing gaseous elemental mercury monitoring technology. In the device of the present invention, the mercury element lamp is placed in the magnetic field of the magnet, the output light is transmitted through the collimator lens to obtain parallel light, the parallel light enters the beam splitter after passing through the sample cell, and the transmitted light enters the first convex lens after passing through the reference cell, focusing to the first detector, the reflected light is incident on the second convex lens, and focused to the second detector, and the first detector and the second detector are connected with a data acquisition analyzer. The method of the present invention is specifically as follows: one, determine that the light intensity contrast M is the constant A corresponding to zero; two, depict the corresponding relationship curve between the light intensity contrast M and the concentration of the gaseous elemental mercury medium; three, measure the gaseous elemental mercury medium to be measured The contrast M of the light intensity is compared with the corresponding relationship curve to obtain the concentration of the gaseous elemental mercury medium to be measured. For monitoring gaseous mercury concentrations.

Description

气态单质汞浓度的连续监测装置和方法 Device and method for continuous monitoring of gaseous elemental mercury concentration

技术领域technical field

本发明涉及气体浓度的测量领域,具体涉及的是一种用于连续监测气态单质汞浓度的装置和方法。The invention relates to the field of gas concentration measurement, in particular to a device and method for continuously monitoring the concentration of gaseous elemental mercury.

背景技术Background technique

燃烧烟气中的汞有三种存在形式:气态单质汞,气态二价氧化态汞和颗粒态汞。其中气态汞为主要形式。总汞的含量是通过热催化或化学转化的方式将其它形态的汞转化为气态单质汞来测得的。在目前已有应用的汞排放连续监测系统中,最常被采用的气态单质汞测量技术是基于光谱学检测原理的冷蒸汽原子吸收光谱(CVAAS)和冷蒸汽原子荧光光谱(CVAFS)技术。前者可对烟气中的气态单质汞浓度实施直接测量而无需像后者那样需要载气,因而被绝大多数的汞排放连续监测系统所采用。在大部分基于CVAAS的系统中,烟气流中的汞在引入光学检测系统分析前需经预富集和解吸附两个步骤来提高测量灵敏度以及去除干扰气体,这两个步骤大大降低了汞排放监测的实时性,使得汞监测只能处于半连续状态。Mercury in combustion flue gas exists in three forms: gaseous elemental mercury, gaseous divalent oxidized mercury and particulate mercury. Among them, gaseous mercury is the main form. The total mercury content is measured by thermocatalytic or chemical conversion of other forms of mercury into gaseous elemental mercury. Among the currently applied continuous monitoring systems for mercury emissions, the most commonly used gaseous elemental mercury measurement techniques are cold vapor atomic absorption spectroscopy (CVAAS) and cold vapor atomic fluorescence spectroscopy (CVAFS) techniques based on the principle of spectroscopic detection. The former can directly measure the concentration of gaseous elemental mercury in the flue gas without the need for a carrier gas like the latter, so it is adopted by most continuous monitoring systems for mercury emissions. In most CVAAS-based systems, the mercury in the flue gas stream needs to be pre-concentrated and desorbed before being introduced into the optical detection system for analysis to improve measurement sensitivity and remove interfering gases. These two steps greatly reduce mercury emissions. The real-time nature of monitoring makes mercury monitoring only in a semi-continuous state.

目前可以做到气态单质汞连续监测的技术主要有两种:紫外差分吸收光谱(UV-DOAS)和塞曼原子吸收光谱(ZAAS)技术。此两种技术均是基于吸收光谱学原理,在汞具有最大吸收截面的253.7nm处对其实施测量,响应速度可达到秒量级,做到真正意义上的实时测量。前者采用的是覆盖紫外到可见波段的宽带发射光源,但由于汞是单原子分子,其吸收线宽很窄,即使采用滤光片也难以获得大的光强吸收比率,从而难以获得较高的测量灵敏度。后者是CVAAS中的一个特例,采用窄带发射的汞元素灯作为光源,通过应用塞曼背景校正技术来排除干扰且无需进行汞的预富集和解吸附,但其对检偏系统的要求很高,增加了系统的复杂性和成本而得不到更广泛的应用。At present, there are two main technologies that can continuously monitor gaseous elemental mercury: ultraviolet differential absorption spectroscopy (UV-DOAS) and Zeeman atomic absorption spectroscopy (ZAAS). Both of these technologies are based on the principle of absorption spectroscopy. Mercury is measured at 253.7nm, where mercury has the largest absorption cross-section. The response speed can reach the order of seconds, achieving real-time measurement in the true sense. The former uses a broadband emitting light source covering the ultraviolet to visible bands, but because mercury is a monatomic molecule, its absorption line width is very narrow, and it is difficult to obtain a large light intensity absorption ratio even with a filter, so it is difficult to obtain a higher Measurement sensitivity. The latter is a special case in CVAAS, which uses a narrow-band emitting mercury element lamp as a light source, and uses Zeeman background correction technology to eliminate interference and does not require pre-enrichment and desorption of mercury, but it has high requirements for the analysis system , which increases the complexity and cost of the system and cannot be widely used.

发明内容Contents of the invention

本发明是为了解决现有的气态单质汞监测技术灵敏度低、系统复杂和成本过高的问题,从而提供一种气态单质汞浓度的连续监测装置和方法。The invention aims to solve the problems of low sensitivity, complex system and high cost of the existing gaseous elemental mercury monitoring technology, thereby providing a continuous monitoring device and method for gaseous elemental mercury concentration.

气态单质汞浓度的连续监测装置,它由汞元素灯、磁铁、准直透镜、样品池、分光镜、参考池、第一凸透镜、第一探测器、第二凸透镜、第二探测器、数据采集分析器组成,汞元素灯置于磁铁的磁场中,并且设置在准直透镜的焦点处,第一探测器的探测面与第一凸透镜的焦平面重合,第二探测器的探测面与第二凸透镜的焦平面重合,汞元素灯的输出光入射至准直透镜,经准直透镜透射得到平行光,所述平行光经过样品池后入射至分光镜,所述平行光经分光镜分成反射光和透射光,其中透射光经过参考池后入射至第一凸透镜,再经第一凸透镜聚焦至第一探测器,反射光入射至第二凸透镜,再经第二凸透镜聚焦至第二探测器,所述第一探测器的输出端和第二探测器的输出端分别连接数据采集分析器的两个接入端,参考池中的介质为饱和浓度的单质汞气体。A continuous monitoring device for the concentration of gaseous elemental mercury, which consists of a mercury element lamp, a magnet, a collimating lens, a sample cell, a beam splitter, a reference cell, a first convex lens, a first detector, a second convex lens, a second detector, and data acquisition The analyzer is composed of the mercury element lamp placed in the magnetic field of the magnet and set at the focal point of the collimating lens. The detection surface of the first detector coincides with the focal plane of the first convex lens, and the detection surface of the second detector coincides with the focal plane of the second convex lens. The focal planes of the convex lenses coincide, the output light of the mercury element lamp is incident on the collimator lens, and the parallel light is transmitted through the collimator lens. The parallel light is incident on the beam splitter after passing through the sample cell, and the parallel light is divided into reflected light by the beam splitter and the transmitted light, wherein the transmitted light enters the first convex lens after passing through the reference cell, and then focuses to the first detector through the first convex lens, and the reflected light enters the second convex lens, and then focuses to the second detector through the second convex lens, so The output end of the first detector and the output end of the second detector are respectively connected to the two access ends of the data acquisition analyzer, and the medium in the reference pool is elemental mercury gas with a saturated concentration.

气态单质汞浓度的连续监测方法,具体过程如下:The continuous monitoring method of gaseous elemental mercury concentration, the specific process is as follows:

步骤一、样品池充满待测气态单质汞介质时,数据采集分析器测量第一探测器探测的透射光强I R 和第二探测器探测的反射光强I S Step 1. When the sample cell is filled with the gaseous elemental mercury medium to be measured, the data acquisition analyzer measures the transmitted light intensity I R detected by the first detector and the reflected light intensity I S detected by the second detector;

步骤二、根据如下公式计算步骤一所述的透射光和反射光的光强对比度MStep 2, calculate the light intensity contrast M of transmitted light and reflected light described in step 1 according to the following formula;

Figure 2010101714180100002DEST_PATH_IMAGE001
Figure 2010101714180100002DEST_PATH_IMAGE001

其中,A是样品池中仅含有空气时光强对比度M为零所对应的常数;Wherein, A is the constant corresponding to the light intensity contrast M being zero when only air is contained in the sample cell;

步骤三、将步骤二得到的光强对比度M与光强对比度M与气态单质汞介质浓度的对应关系曲线对照,得到待测气态单质汞介质的浓度。Step 3: compare the light intensity contrast M obtained in step 2 with the corresponding relationship curve between the light intensity contrast M and the concentration of the gaseous elemental mercury medium to obtain the concentration of the gaseous elemental mercury medium to be measured.

本发明利用塞曼关联光谱技术实现了对单质汞气浓度的连续有效监测,用参考气体本身的光谱信息实现了对气态单质汞的选择性探测,排除了二氧化硫和二氧化氮等气体带来的干扰。系统组成简单,无需使用光谱仪等色散设备和复杂的检偏设备,成本较低。本发明可以达到的最低检测限低于1μg/m3,充分满足了工业废气排放中汞含量监测的要求。适用于要求灵敏度高气态单质汞浓度监测领域。The invention realizes the continuous and effective monitoring of the concentration of elemental mercury gas by using the Zeeman correlation spectrum technology, realizes the selective detection of gaseous elemental mercury by using the spectral information of the reference gas itself, and eliminates the pollution caused by gases such as sulfur dioxide and nitrogen dioxide. interference. The system is simple in composition, without the use of dispersion equipment such as spectrometers and complex polarization analysis equipment, and the cost is low. The minimum detection limit that can be achieved by the invention is lower than 1 μg/m 3 , which fully meets the requirements for monitoring mercury content in industrial waste gas emissions. It is suitable for the monitoring field of gaseous elemental mercury concentration requiring high sensitivity.

附图说明Description of drawings

图1为气态单质汞浓度的连续监测装置的结构示意图。图2为气态单质汞浓度的连续监测方法的流程图。图3为具体实施方式十中光强对比度与待测量气体浓度的对应关系图。Figure 1 is a schematic structural diagram of a continuous monitoring device for gaseous elemental mercury concentration. Fig. 2 is a flowchart of a continuous monitoring method for gaseous elemental mercury concentration. Fig. 3 is a graph showing the corresponding relationship between light intensity contrast and gas concentration to be measured in Embodiment 10.

具体实施方式Detailed ways

具体实施方式一、结合图1说明本实施方式,气态单质汞浓度的连续监测装置,它由汞元素灯1、磁铁2、准直透镜3、样品池4、分光镜5、参考池6、第一凸透镜7、第一探测器8、第二凸透镜9、第二探测器10、数据采集分析器11组成,汞元素灯1置于磁铁2的磁场中,并且设置在准直透镜3的焦点处,第一探测器8的探测面与第一凸透镜7的焦平面重合,第二探测器10的探测面与第二凸透镜9的焦平面重合,汞元素灯1的输出光入射至准直透镜3,经准直透镜3透射得到平行光,所述平行光经过样品池4后入射至分光镜5,所述平行光经分光镜5分成反射光和透射光,其中透射光经过参考池6后入射至第一凸透镜7,再经第一凸透镜7聚焦至第一探测器8,反射光入射至第二凸透镜9,再经第二凸透镜9聚焦至第二探测器10,所述第一探测器8的输出端和第二探测器10的输出端分别连接数据采集分析器11的两个接入端,参考池6中的介质为饱和浓度的单质汞气体。 The specific embodiment one, present embodiment is described in conjunction with Fig. 1, the continuous monitoring device of gaseous elemental mercury concentration, it is made of mercury element lamp 1, magnet 2, collimating lens 3, sample cell 4, beam splitter 5, reference cell 6, the first Composed of a convex lens 7, a first detector 8, a second convex lens 9, a second detector 10, and a data acquisition analyzer 11, the mercury element lamp 1 is placed in the magnetic field of the magnet 2, and is arranged at the focal point of the collimating lens 3 , the detection surface of the first detector 8 coincides with the focal plane of the first convex lens 7, the detection surface of the second detector 10 coincides with the focal plane of the second convex lens 9, and the output light of the mercury element lamp 1 is incident on the collimator lens 3 , the parallel light is transmitted through the collimator lens 3, and the parallel light is incident on the beam splitter 5 after passing through the sample cell 4, and the parallel light is divided into reflected light and transmitted light by the beam splitter 5, wherein the transmitted light is incident after passing through the reference cell 6 to the first convex lens 7, then focus to the first detector 8 through the first convex lens 7, the reflected light is incident on the second convex lens 9, and then focus to the second detector 10 through the second convex lens 9, the first detector 8 The output end of the second detector 10 and the output end of the second detector 10 are respectively connected to the two access ends of the data acquisition analyzer 11, and the medium in the reference pool 6 is elemental mercury gas with a saturated concentration.

样品池4中的介质是待测气态单质汞介质。参考池6中饱和浓度的单质汞气体能够使处于波长为253.7nm附近的光被最大程度的吸收。The medium in the sample cell 4 is the gaseous elemental mercury medium to be measured. The saturated concentration of elemental mercury gas in the reference cell 6 can make the light with a wavelength near 253.7nm be absorbed to the maximum extent.

工作原理:汞元素灯1发出紫外光,在磁铁2产生的磁场作用下其253.7nm处的发射谱线劈裂为一系列具有不同波长的塞曼分量,波长劈裂后的紫外光经准直透镜3后变为平行光,在经过装有待测气体的样品池4后被分光镜5分为透射光和反射光,透射光经过装有饱和浓度气态单质汞的参考池6后,处于253.7nm附近的塞曼分量被最大程度的吸收,剩余的塞曼分量作为参考光再经第一凸透镜7聚焦后被第一探测器8接收,反射光为样品光,反射光直接经第二凸透镜9聚焦后被第二探测器10接收,第一探测器8和第二探测器10的产生的信号输入到数据采集分析器11中进行模/数转换和数据分析,采集透射光和反射光的光强信息。当样品池4中不存在气态单质汞时,两路光的光强对比度为零,当样品池4中出现气态单质汞时,两路光的光强对比度随着汞含量的增加而增加,且光强对比度与汞含量呈一一对应的关系。Working principle: Mercury element lamp 1 emits ultraviolet light. Under the action of the magnetic field generated by magnet 2, its emission spectrum at 253.7nm is split into a series of Zeeman components with different wavelengths. The ultraviolet light after wavelength splitting is collimated After the lens 3, it becomes parallel light. After passing through the sample cell 4 equipped with the gas to be measured, it is divided into transmitted light and reflected light by the spectroscope 5. After the transmitted light passes through the reference cell 6 equipped with a saturated concentration of gaseous elemental mercury, it is at 253.7 The Zeeman component near nm is absorbed to the greatest extent, and the remaining Zeeman component is used as a reference light and then focused by the first convex lens 7 and then received by the first detector 8. The reflected light is sample light, and the reflected light directly passes through the second convex lens 9 After being focused, it is received by the second detector 10, and the signals generated by the first detector 8 and the second detector 10 are input to the data acquisition analyzer 11 for analog/digital conversion and data analysis, and the light of transmitted light and reflected light is collected strong message. When there is no gaseous elemental mercury in the sample cell 4, the light intensity contrast of the two paths of light is zero, and when gaseous elemental mercury appears in the sample cell 4, the light intensity contrast of the two paths of light increases with the increase of the mercury content, and There is a one-to-one relationship between light intensity contrast and mercury content.

分光镜5后的反射光路和透射光路可以对调,即可由反射光经过参考池6后入射至第一凸透镜7,经第一凸透镜7聚焦至第一探测器8,透射光入射至第二凸透镜9,经第二凸透镜9聚焦至第二探测器10。The reflected light path and the transmitted light path behind the beam splitter 5 can be reversed, that is, the reflected light is incident on the first convex lens 7 after passing through the reference cell 6, and then focused to the first detector 8 by the first convex lens 7, and the transmitted light is incident on the second convex lens 9 , focus to the second detector 10 through the second convex lens 9 .

具体实施方式二、结合图1说明本实施方式,本实施方式与具体实施方式一的不同之处在于分光镜5为半反射半透射的分束镜。 Embodiment 2. This embodiment is described with reference to FIG. 1 . The difference between this embodiment and Embodiment 1 is that the beam splitter 5 is a semi-reflective and semi-transmissive beam splitter.

具体实施方式三、结合图1说明本实施方式,本实施方式与具体实施方式一的不同之处在于参考池6中单质汞气体的每米饱和浓度为0.2~20mg/m3 Specific Embodiment 3. This embodiment is described with reference to FIG. 1 . The difference between this embodiment and Embodiment 1 is that the saturation concentration of elemental mercury gas per meter in the reference cell 6 is 0.2-20 mg/m 3 .

具体实施方式四、结合图1说明本实施方式,本实施方式与具体实施方式一的不同之处在于磁铁2所产生的磁感应强度为1~3T。 Embodiment 4. This embodiment is described with reference to FIG. 1 . The difference between this embodiment and Embodiment 1 is that the magnetic induction generated by the magnet 2 is 1-3T.

具体实施方式五、结合图2说明本实施方式,气态单质汞浓度的连续监测方法,具体过程如下: Specific embodiment five, illustrate present embodiment in conjunction with Fig. 2, the continuous monitoring method of gaseous elemental mercury concentration, concrete process is as follows:

步骤一、将样品池4充满待测气态单质汞介质,数据采集分析器11测量第一探测器8探测的透射光强I R 和第二探测器10探测的反射光强I S Step 1, the sample cell 4 is filled with the gaseous elemental mercury medium to be measured, and the data acquisition analyzer 11 measures the transmitted light intensity I R detected by the first detector 8 and the reflected light intensity I S detected by the second detector 10;

步骤二、根据如下公式计算步骤一所述的透射光和反射光的光强对比度MStep 2, calculate the light intensity contrast M of transmitted light and reflected light described in step 1 according to the following formula;

Figure 317578DEST_PATH_IMAGE001
Figure 317578DEST_PATH_IMAGE001

其中,A是样品池4中仅含有空气时光强对比度M为零所对应的常数;Wherein, A is the constant corresponding to the light intensity contrast M being zero when only air is contained in the sample cell 4;

步骤三、将步骤二得到的光强对比度M与光强对比度M与气态单质汞介质浓度的对应关系曲线对照,得到待测气态单质汞介质的浓度。Step 3: compare the light intensity contrast M obtained in step 2 with the corresponding relationship curve between the light intensity contrast M and the concentration of the gaseous elemental mercury medium to obtain the concentration of the gaseous elemental mercury medium to be measured.

具体实施方式六、本实施方式是对具体实施方式五的进一步说明,步骤二中样品池4中仅含有空气时光强对比度M为零所对应的常数A是通过下述方法获得的: Embodiment 6. This embodiment is a further description of Embodiment 5. In step 2, the sample pool 4 only contains air, and the constant A corresponding to the light intensity contrast M being zero is obtained by the following method:

步骤二M、样品池4中仅含有空气时,数据采集分析器11测量第一探测器8探测的透射光强I R0 和第二探测器10探测的反射光强I S0 Step 2M, when the sample cell 4 only contains air, the data acquisition analyzer 11 measures the transmitted light intensity I R0 detected by the first detector 8 and the reflected light intensity I S0 detected by the second detector 10;

步骤二N、求得步骤二M所述的透射光和反射光的光强对比度M为零所对应的常数AStep 2N, obtaining the light intensity contrast M of the transmitted light described in step 2M and reflected light is the constant A corresponding to zero;

其中,光强对比度M通过下式求得:Among them, the light intensity contrast M is obtained by the following formula:

.

具体实施方式七、本实施方式是对具体实施方式五的进一步说明,步骤三所述的光强对比度M与气态单质汞介质浓度的对应关系曲线是通过下述方法获得的: Specific embodiment seven, this embodiment is a further description of specific embodiment five, the corresponding relationship curve of the light intensity contrast M described in step 3 and the gaseous elemental mercury medium concentration is obtained by the following method:

步骤三M、将样品池4充满已知浓度的气态单质汞介质,数据采集分析器11测量第一探测器8探测的透射光强I R 和第二探测器10探测的反射光强I S Step 3M, the sample cell 4 is filled with the gaseous elemental mercury medium of known concentration, and the data acquisition analyzer 11 measures the transmitted light intensity I R detected by the first detector 8 and the reflected light intensity I S detected by the second detector 10;

步骤三N、根据如下公式计算步骤三M所述的透射光和反射光的光强对比度MStep 3N, calculate the light intensity contrast M of the transmitted light and reflected light described in step 3M according to the following formula;

Figure 985450DEST_PATH_IMAGE001
Figure 985450DEST_PATH_IMAGE001

其中,A是样品池4中不含有待测气体时对比度为零所对应的常数;Wherein, A is the constant corresponding to the contrast of zero when the sample cell 4 does not contain the gas to be measured;

步骤三P、重复执行步骤三N,直到获得n组气态单质汞介质浓度的光强对比度M,并以气态单质汞介质浓度为横轴,光强对比度M为纵轴描绘光强对比度M与气态单质汞介质浓度的对应关系曲线。Step 3P, repeat step 3N until the light intensity contrast M of n groups of gaseous elemental mercury medium concentration is obtained, and the horizontal axis is the gaseous elemental mercury medium concentration, and the light intensity contrast M is the vertical axis to depict the light intensity contrast M and the gaseous state Corresponding relationship curve of elemental mercury medium concentration.

具体实施方式八、本实施方式是对具体实施方式五的进一步说明,步骤四中的光强对比度M与气态单质汞介质浓度的对应关系曲线为直线。 Embodiment 8. This embodiment is a further description of Embodiment 5. The corresponding relationship curve between the light intensity contrast M and the concentration of the gaseous elemental mercury medium in step 4 is a straight line.

具体实施方式九、本实施方式是对具体实施方式五的进一步说明,步骤四中的测量n个气态单质汞介质浓度时光强对比度M为测量5-12个值。 Embodiment 9. This embodiment is a further description of Embodiment 5. In step 4, measure the concentration of n gaseous elemental mercury media and the light intensity contrast M is 5-12 values.

具体实施方式十、结合图3说明本实施方式,本实施方式采用具体实施方式一所述的装置和具体实施方式五所述的方法测量待测气态单质汞浓度的具体实例,选定如下参数: Specific embodiment ten, in conjunction with Fig. 3 illustrate this embodiment, present embodiment adopts the device described in specific embodiment one and the method described in specific embodiment five to measure the concrete example of gaseous elemental mercury concentration to be measured, select following parameter:

磁铁2所产生的磁场强度为1T,参考池6中的单质汞气体的每米饱和浓度为1mg/m3The magnetic field intensity generated by the magnet 2 is 1T, and the saturation concentration per meter of the elemental mercury gas in the reference cell 6 is 1 mg/m 3 .

通过公式计算出两光强对比度,根据得到的不同光强对比度确定样品池的气态单质汞浓度,结果如图3所示,横轴为气态单质汞介质浓度;纵轴为光强对比度。 The contrast between the two light intensities was calculated by the formula, and the concentration of gaseous elemental mercury in the sample cell was determined according to the different light intensity contrasts obtained. The results are shown in Figure 3. The horizontal axis is the concentration of the gaseous elemental mercury medium; the vertical axis is the light intensity contrast. the

Claims (9)

1. The device for continuously monitoring the concentration of the gaseous elemental mercury is characterized by comprising a mercury element lamp (1), a magnet (2), a collimating lens (3), a sample cell (4), a spectroscope (5), a reference cell (6), a first convex lens (7), a first detector (8), a second convex lens (9), a second detector (10) and a data acquisition analyzer (11), wherein the mercury element lamp (1) is arranged in a magnetic field of the magnet (2) and is arranged at the focal point of the collimating lens (3), a detection surface of the first detector (8) is superposed with a focal plane of the first convex lens (7), a detection surface of the second detector (10) is superposed with a focal plane of the second convex lens (9), output light of the mercury element lamp (1) enters the collimating lens (3) and is transmitted by the collimating lens (3) to obtain parallel light, and the parallel light enters the collimating lens (5) after passing through the sample cell (4), the parallel light is divided into reflected light and transmitted light through the spectroscope (5), wherein the transmitted light is incident to the first convex lens (7) after passing through the reference pool (6), and then is focused to the first detector (8) through the first convex lens (7), the reflected light is incident to the second convex lens (9), and then is focused to the second detector (10) through the second convex lens (9), the output end of the first detector (8) and the output end of the second detector (10) are respectively connected with two access ends of the data acquisition analyzer (11), and the medium in the reference pool (6) is elemental mercury gas with saturated concentration.
2. The continuous monitoring device of gaseous elemental mercury concentration according to claim 1, characterized in that the beam splitter (5) is a half-reflective and half-transmissive beam splitter.
3. The continuous monitoring device of gaseous elemental mercury concentration according to claim 1, characterized in that the saturated concentration per meter of elemental mercury gas in the reference cell (6) is 0.2-20 mg/m3
4. The device for continuously monitoring the concentration of gaseous elemental mercury according to claim 1, characterized in that the magnetic induction generated by the magnet (2) is 1-3T.
5. The continuous monitoring method using the continuous monitoring device of gaseous elemental mercury concentration according to claim 1, characterized by the following specific procedures:
step one, filling a sample cell (4) with a gaseous elementary mercury medium to be detected, and measuring the transmitted light intensity detected by a first detector (8) by a data acquisition analyzer (11)I R And the intensity of the reflected light detected by the second detector (10)I S
Step two, calculating the light intensity contrast of the transmitted light and the reflected light according to the following formulaM
Figure 2010101714180100001DEST_PATH_IMAGE001
Wherein,Athe contrast of light intensity is only when the sample cell (4) contains airMA constant corresponding to zero;
step three, the light intensity contrast obtained in the step twoMContrast with light intensityMAnd comparing with the corresponding relation curve of the concentration of the gaseous elementary substance mercury medium to obtain the concentration of the gaseous elementary substance mercury medium to be detected.
6. The method according to claim 5, wherein the sample cell (4) in step two contains only air and has a light intensity contrastMConstant corresponding to zeroAIs obtained by the following method:
step two M, when the sample cell (4) only contains air, the data acquisition analyzer (11) measures the transmitted light intensity detected by the first detector (8)I R0 And the intensity of the reflected light detected by the second detector (10)I S0
Step two N, the light intensity contrast ratio of the transmission light and the reflection light in the step two M is obtainedMConstant corresponding to zeroA
Wherein the contrast of light intensityMThe following equation is used to obtain:
Figure 2010101714180100001DEST_PATH_IMAGE002
7. the method of claim 5, wherein the step three of continuously monitoring the concentration of gaseous elemental mercury is characterized by a light intensity contrastMThe corresponding relation curve with the concentration of the gaseous elementary mercury medium is obtained by the following method:
step three M, filling the sample cell (4) with gaseous elementary mercury medium with known concentration, and measuring the transmitted light intensity detected by the first detector (8) by the data acquisition analyzer (11)I R And the intensity of the reflected light detected by the second detector (10)I S
Step three N, calculating the light intensity contrast of the transmitted light and the reflected light in step three M according to the following formulaM
Figure 155324DEST_PATH_IMAGE001
Wherein,Ais a constant corresponding to the contrast being zero when the sample cell (4) does not contain the gas to be measured;
step three P, repeatedly executing step three N until obtaining the light intensity contrast of N groups of gaseous elementary mercury medium concentrationMAnd the concentration of the gaseous elementary mercury medium is taken as the horizontal axis, and the light intensity contrast ratioMPlotting intensity contrast for the vertical axisMAnd (4) a corresponding relation curve with the concentration of the gaseous elementary mercury medium.
8. The method of claim 5 or 7, wherein the method comprises continuously monitoring the concentration of gaseous elemental mercury by light intensity contrastMThe curve of the corresponding relation with the concentration of the gaseous elementary substance mercury medium is a straight line.
9. The method according to claim 7, wherein the step three P comprises obtaining the light intensity contrast of the concentrations of n groups of gaseous elemental mercury mediaMTo obtain 5-12 sets of light intensity contrastMNumerical values.
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Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101498665A (en) * 2009-02-27 2009-08-05 哈尔滨工业大学 Sulphur dioxide gas concentration detection apparatus based on associated spectrum technology

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