CN114778507B - Atomic fluorescence spectrometer based on integrated full-angle excitation source and measuring method - Google Patents
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- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N21/6428—Measuring fluorescence of fluorescent products of reactions or of fluorochrome labelled reactive substances, e.g. measuring quenching effects, using measuring "optrodes"
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Abstract
Description
技术领域Technical Field
本发明属于分析仪器技术领域,特别涉及一种基于一体化全角度激发源的原子荧光光谱仪及原子荧光光谱测量方法。The invention belongs to the technical field of analytical instruments, and particularly relates to an atomic fluorescence spectrometer based on an integrated full-angle excitation source and an atomic fluorescence spectrum measurement method.
背景技术Background Art
在原子光谱分析仪器中,激发源(原子化器和或激发光源)是其关键与核心,它直接决定了仪器的结构和分析性能的好坏。在现有的原子荧光光谱仪中,激发光源与原子化器在物理空间上是分离的。通常,原子化器采用石英管炉内的氢氧火焰,激发光源则采用高强度空心阴极灯。石英管原子化器仅适用于在常温下能生成气态氢化物的元素,利用氢化物发生法附带产生的氢气与空气中的氧气在氩气环境下燃烧,实现样品原子化。因此,被测样品元素的种类受到一定的限制。In atomic spectrometers, the excitation source (atomizer and/or excitation light source) is the key and core, which directly determines the structure of the instrument and the quality of the analytical performance. In existing atomic fluorescence spectrometers, the excitation light source and the atomizer are separated in physical space. Usually, the atomizer uses a hydrogen-oxygen flame in a quartz tube furnace, and the excitation light source uses a high-intensity hollow cathode lamp. The quartz tube atomizer is only suitable for elements that can generate gaseous hydrides at room temperature. The hydrogen generated by the hydride generation method is burned with oxygen in the air in an argon environment to achieve sample atomization. Therefore, the types of elements in the sample being tested are subject to certain restrictions.
作为激发光源的空心阴极灯存在的最大问题是灯的发光强度漂移严重,仪器需要定时校正标准曲线,用户使用不便。其次,常用的空心阴极灯属于锐线光源,一种空心阴极灯只能发射一种与之对应的元素的光辐射,也只能用于测量与该元素种类相同的被测样品。当需要测量不同种类的元素时,需要更换不同元素的空心阴极灯。例如,如果测量样品中的锌元素,就需要配置锌元素灯才能进行分析。由于空心阴极灯种类限制,不能随意扩展被测元素的种类。另外,对于多种元素的样品分析,必需配置多个元素的灯,需要占用更大的仪器空间。The biggest problem with hollow cathode lamps as excitation light sources is that the luminous intensity of the lamp drifts severely, and the instrument needs to calibrate the standard curve regularly, which is inconvenient for users. Secondly, the commonly used hollow cathode lamps are sharp-line light sources. A hollow cathode lamp can only emit light radiation of one element corresponding to it, and can only be used to measure samples of the same type as the element. When different types of elements need to be measured, hollow cathode lamps of different elements need to be replaced. For example, if the zinc element in the sample is measured, a zinc element lamp needs to be configured for analysis. Due to the limitation of the types of hollow cathode lamps, the types of elements to be measured cannot be expanded at will. In addition, for the analysis of samples of multiple elements, lamps of multiple elements must be configured, which requires a larger instrument space.
在仪器布局方面,为了避免激发光源所发射的光辐射对微弱原子荧光信号测量产生影响,必需使荧光检测器接收光信号的方向与激发光照射原子化器的方向成直角或者成锐角分布,激发光束充其量照射原子化器180度的范围,如图1所示。众所周知,荧光信号强度与激发光的强度成正比。由于石英管原子化器的整个圆周最多只有180度范围能接收到激发光,因此仪器的测量灵敏度必然会受到影响。In terms of instrument layout, in order to prevent the light radiation emitted by the excitation light source from affecting the measurement of weak atomic fluorescence signals, the direction in which the fluorescence detector receives the light signal must be at right angles or at an acute angle to the direction in which the excitation light irradiates the atomizer, and the excitation light beam irradiates the atomizer within a range of 180 degrees at best, as shown in Figure 1. As we all know, the intensity of the fluorescence signal is proportional to the intensity of the excitation light. Since the entire circumference of the quartz tube atomizer can only receive the excitation light within a range of 180 degrees at most, the measurement sensitivity of the instrument will inevitably be affected.
综上,现有的原子荧光光谱仪还需要进一步优化。In summary, the existing atomic fluorescence spectrometers need further optimization.
发明内容Summary of the invention
为了克服上述现有原子荧光光谱仪存在的不足,本发明提供一种基于一体化全角度激发源的原子荧光光谱仪,所述一体化全角度激发源基于微波同轴谐振腔,在微波同轴谐振腔引入易电离工质气体、可燃气体和助燃气体,在相同的时空范围内,获得微波耦合等离子体与高温火焰融合激发光源,完成脉冲方式进样的标准样品的激发,获得脉冲式激发光。同时,在微波同轴谐振腔的外导体内部或外部设置环形原子化器,利用火焰完成待测样品的原子化。脉冲式激发光在360度方向上照射原子化之后的待测样品,获得环形脉冲荧光。In order to overcome the shortcomings of the above-mentioned existing atomic fluorescence spectrometers, the present invention provides an atomic fluorescence spectrometer based on an integrated full-angle excitation source, which is based on a microwave coaxial resonant cavity. An easily ionized working gas, a combustible gas, and a combustion-supporting gas are introduced into the microwave coaxial resonant cavity. In the same time and space range, a microwave coupled plasma and a high-temperature flame fusion excitation light source are obtained to complete the excitation of the standard sample injected in a pulsed manner and obtain pulsed excitation light. At the same time, a ring atomizer is arranged inside or outside the outer conductor of the microwave coaxial resonant cavity, and the atomization of the sample to be tested is completed by using a flame. The pulsed excitation light irradiates the atomized sample to be tested in a 360-degree direction to obtain a ring-shaped pulse fluorescence.
一种基于一体化全角度激发源的原子荧光光谱仪,包括气体控制单元21、进样系统22、微波源23、激发源24、荧光检测单元25、数据处理单元26和显示记录单元27;其中气体控制单元21用来精确控制各路气体流量,由钢瓶输入气体,经减压阀、稳压阀、稳流阀和流量计精密控制各路气体输出至激发源24的外层气体入口5、中层气体入口7、内层气体入口9、工作气入口13和屏蔽气入口15以及进样系统22所需的载气;所述微波源23输出微波功率至激发源24的微波输入端口2;所述荧光检测单元25经光电检测器接收荧光信号,然后经过电子电路输出至数据处理单元26;所述数据处理单元26利用微处理器采集、处理、运算荧光信号,并输出至显示记录单元27,完成显示和存储;An atomic fluorescence spectrometer based on an integrated full-angle excitation source comprises a gas control unit 21, an injection system 22, a microwave source 23, an excitation source 24, a fluorescence detection unit 25, a data processing unit 26 and a display and recording unit 27; wherein the gas control unit 21 is used to accurately control the flow of each gas, inputs gas from a steel cylinder, and accurately controls the output of each gas to the outer gas inlet 5, the middle gas inlet 7, the inner gas inlet 9, the working gas inlet 13 and the shielding gas inlet 15 of the excitation source 24 and the carrier gas required by the injection system 22 through a pressure reducing valve, a pressure regulating valve, a flow regulating valve and a flow meter; the microwave source 23 outputs microwave power to the microwave input port 2 of the excitation source 24; the fluorescence detection unit 25 receives the fluorescence signal through a photoelectric detector, and then outputs it to the data processing unit 26 through an electronic circuit; the data processing unit 26 uses a microprocessor to collect, process and calculate the fluorescence signal, and outputs it to the display and recording unit 27 to complete display and storage;
其特征在于,所述激发源24包括激发光源模块和环形原子化器模块;所述激发光源模块为微波同轴谐振腔,包括外导体1、微波输入端口2、微波天线3、内导体4、外层气入口5、中管6、中层气入口7、内管8、内层气入口9、标准样品管10、标准样品入口11;外导体1、内导体4、中管6、内管8、标准样品管10按由外到内的顺序依次嵌套且同轴,内导体4、中管6、内管8和样品管10在出口端面处齐平,内导体4、中管6、内管8和标准样品管10与外导体1构成嵌套同轴结构的微波谐振腔,该谐振腔的特性阻抗范围为50~80欧姆;外导体1为内部中空的圆柱体,内径为35~60mm;内导体4、中管6与内管8构成的嵌套同轴结构出口端面还兼有高温火焰燃烧喷嘴功能,在出口端面处同时产生微波耦合等离子体和高温火焰;微波输入端口2的轴线距离微波同轴谐振腔底面为所用微波波长的1/4倍,微波天线3经微波输入端口2引入微波能量并与内导体4电气连接;外导体1上端面距离微波同轴谐振腔底面为所用微波波长的(2n+1)/4倍,其中n取1、2或3;The invention is characterized in that the excitation source 24 includes an excitation light source module and a ring atomizer module; the excitation light source module is a microwave coaxial resonant cavity, including an outer conductor 1, a microwave input port 2, a microwave antenna 3, an inner conductor 4, an outer gas inlet 5, a middle tube 6, a middle gas inlet 7, an inner tube 8, an inner gas inlet 9, a standard sample tube 10, and a standard sample inlet 11; the outer conductor 1, the inner conductor 4, the middle tube 6, the inner tube 8, and the standard sample tube 10 are nested in sequence from outside to inside and are coaxial, the inner conductor 4, the middle tube 6, the inner tube 8 and the sample tube 10 are flush at the outlet end face, and the inner conductor 4, the middle tube 6, the inner tube 8 and the standard sample tube 10 form a micro-cavity with a nested coaxial structure with the outer conductor 1. The invention discloses a microwave resonant cavity, wherein the characteristic impedance of the resonant cavity ranges from 50 to 80 ohms; the outer conductor 1 is a hollow cylinder with an inner diameter of 35 to 60 mm; the outlet end face of the nested coaxial structure formed by the inner conductor 4, the middle tube 6 and the inner tube 8 also has the function of a high-temperature flame combustion nozzle, and microwave coupled plasma and high-temperature flame are simultaneously generated at the outlet end face; the axis of the microwave input port 2 is 1/4 times the wavelength of the microwave used at the bottom of the microwave coaxial resonant cavity, and the microwave antenna 3 introduces microwave energy through the microwave input port 2 and is electrically connected to the inner conductor 4; the upper end face of the outer conductor 1 is (2n+1)/4 times the wavelength of the microwave used at the bottom of the microwave coaxial resonant cavity, wherein n is 1, 2 or 3;
外层气入口5位于内导体4下部靠近内导体4底端的径向位置,中层气入口7位于中管6下部靠近中管6底端的径向位置,内层气入口9位于内管8下部靠近内管8底端的径向位置,均采用径向进气方式;从外层气入口5、中层气入口7和内层气入口9进入的易电离气体在其出口端面均以层流状态流出,利用微波电场能量电离形成微波耦合等离子体;从外层气入口5、中层气入口7和内层气入口9进入的可燃气体和助燃气体在其出口端面构成的燃烧喷嘴以层状态流出,进行燃烧形成高温火焰;微波耦合等离子体和高温火焰在相同的时间和空间上融合,形成标准样品激发光源;标准样品入口11位于样品管10的底部,与待测样品元素种类相同的高浓度标准样品气溶胶经过标准样品入口11进入标准样品管10,并在标准样品管10出口侧端面进入激发光源,激发之后获得待测样品荧光测量所需的激发光;The outer gas inlet 5 is located at a radial position at the lower part of the inner conductor 4 near the bottom end of the inner conductor 4, the middle gas inlet 7 is located at a radial position at the lower part of the middle tube 6 near the bottom end of the middle tube 6, and the inner gas inlet 9 is located at a radial position at the lower part of the inner tube 8 near the bottom end of the inner tube 8, all of which adopt a radial air intake method; the easily ionized gas entering from the outer gas inlet 5, the middle gas inlet 7 and the inner gas inlet 9 all flows out at its outlet end face in a laminar state, and is ionized by the microwave electric field energy to form a microwave coupled plasma; the easily ionized gas entering from the outer gas inlet 5, the middle gas inlet 7 and the inner gas inlet 9 The combustible gas and the combustion-supporting gas flow out of the combustion nozzle formed by the outlet end face thereof in a layered state, and burn to form a high-temperature flame; the microwave coupled plasma and the high-temperature flame merge at the same time and space to form a standard sample excitation light source; the standard sample inlet 11 is located at the bottom of the sample tube 10, and the high-concentration standard sample aerosol with the same element type as the sample to be tested enters the standard sample tube 10 through the standard sample inlet 11, and enters the excitation light source at the outlet side end face of the standard sample tube 10, and after excitation, the excitation light required for the fluorescence measurement of the sample to be tested is obtained;
所述环形原子化器模块包括导流环12、工作气入口13、待测样品入口14、屏蔽气入口15、内层导流管16、中层导流管17和外层导流管18,所述环形原子化器模块位于微波输入端口2的上方,在微波同轴谐振腔的外导体1的内侧或外侧。The annular atomizer module includes a guide ring 12, a working gas inlet 13, a sample inlet 14, a shielding gas inlet 15, an inner layer guide tube 16, a middle layer guide tube 17 and an outer layer guide tube 18. The annular atomizer module is located above the microwave input port 2, on the inner or outer side of the outer conductor 1 of the microwave coaxial resonant cavity.
具体的,当环形原子化器设置于微波输入端口2上方微波同轴谐振腔外导体1的内侧时,导流环12位于外导体1与内导体4构成的环形空间内部,导流环12为非金属材料;外导体1侧面有工作气入口13、待测样品入口14和屏蔽气入口15;导流环12外侧有凹形导气沟槽,导流环12内侧设计有工作气入口13和待测样品入口14;导气沟槽高度分别与外导体1侧面的工作气入口13和待测样品入口14高度一致;导流环12内侧依次安装内层导流管16、中层导流管17和外层导流管18,并且内层导流管16、中层导流管17和外层导流管18在上出口端面处齐平;内层导流管16、中层导流管17和外层导流管18采用不影响腔体内部电磁场分布的非金属材料,优选石英或陶瓷等;内层导流管16与中层导流管17构成待测样品的环形原子化器,完成待测样品的原子化,并全角度被脉冲式激发光源激发,产生环形荧光;工作气通入内导流管16和中导流管17构成的环形间隙;工作气以内层导流管16与中导流管17构成的环形间隙的切线方向或径向方向引入,以涡流或层流形式流向端面,参与火焰燃烧过程;待测样品气溶胶通入中导流管17和外导流管18构成的环形间隙;屏蔽气通入外导流管18与外导体1构成的环形间隙;屏蔽气以外导体1内径的切线或径向方向引入,形成涡流或层流屏蔽层。Specifically, when the annular atomizer is arranged on the inner side of the outer conductor 1 of the microwave coaxial resonant cavity above the microwave input port 2, the guide ring 12 is located inside the annular space formed by the outer conductor 1 and the inner conductor 4, and the guide ring 12 is made of non-metallic material; the outer conductor 1 has a working gas inlet 13, a sample inlet 14 and a shielding gas inlet 15 on the side; the guide ring 12 has a concave gas guide groove on the outside, and the guide ring 12 is designed with a working gas inlet 13 and a sample inlet 14 on the inside; the height of the gas guide groove is respectively consistent with the height of the working gas inlet 13 and the sample inlet 14 on the side of the outer conductor 1; the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 are installed in sequence on the inner side of the guide ring 12, and the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 are flush at the upper outlet end face; the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 are flush at the upper outlet end face; the inner layer guide tube 16, the middle layer guide tube 1 7 and the outer flow guide tube 18 are made of non-metallic materials that do not affect the electromagnetic field distribution inside the cavity, preferably quartz or ceramics; the inner flow guide tube 16 and the middle flow guide tube 17 constitute an annular atomizer for the sample to be tested, complete the atomization of the sample to be tested, and are excited by the pulsed excitation light source at all angles to generate annular fluorescence; the working gas is introduced into the annular gap formed by the inner flow guide tube 16 and the middle flow guide tube 17; the working gas is introduced in the tangential direction or radial direction of the annular gap formed by the inner flow guide tube 16 and the middle flow guide tube 17, flows to the end face in the form of eddy current or laminar flow, and participates in the flame combustion process; the aerosol of the sample to be tested is introduced into the annular gap formed by the middle flow guide tube 17 and the outer flow guide tube 18; the shielding gas is introduced into the annular gap formed by the outer flow guide tube 18 and the outer conductor 1; the shielding gas is introduced in the tangential or radial direction of the inner diameter of the outer conductor 1 to form an eddy current or laminar shielding layer.
具体的,当环形原子化器设置于微波输入端口2上方微波同轴谐振腔外导体1的外侧时,导流环12位于微波输入端口2的上方外导体1的外部,导流环12为金属或非金属材料;导流环12侧面有工作气入口13、待测样品入口14和屏蔽气入口15;导流环12内侧依次安装内层导流管16、中层导流管17和外层导流管18,并且内层导流管16、中层导流管17和外层导流管18在上出口端面处齐平;内层导流管16、中层导流管17和外层导流管18可以是非金属材料,优选石英或陶瓷;也可以是金属材料,优选黄铜;外导体1与内层导流管16构成待测样品的环形原子化器,完成待测样品的原子化,并全角度被脉冲式激发光源激发,产生环形荧光;工作气通入外导体1和内导流管16构成的环形间隙;工作气以外导体1与内导流管16构成的环形间隙的切线或径向方向引入,以涡流或层流形式流向端面,参与火焰燃烧过程;待测样品气溶胶通入内导流管16和中导流管17构成的环形间隙;屏蔽气通入中导流管17与外导流管18构成的环形间隙;屏蔽气以中导流管17与外导流管18构成的环形间隙的切线方向或径向方向引入,并形成涡流或层流屏蔽层。Specifically, when the annular atomizer is arranged on the outside of the outer conductor 1 of the microwave coaxial resonant cavity above the microwave input port 2, the guide ring 12 is located outside the outer conductor 1 above the microwave input port 2, and the guide ring 12 is made of metal or non-metal material; the side of the guide ring 12 has a working gas inlet 13, a sample inlet 14 and a shielding gas inlet 15; the inner side of the guide ring 12 is successively installed with an inner layer guide tube 16, a middle layer guide tube 17 and an outer layer guide tube 18, and the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 are flush at the upper outlet end face; the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 can be non-metallic materials, preferably quartz or ceramics; or they can be metal materials, preferably brass; the outer conductor 1 and the inner flow guide tube 16 form an annular atomizer for the sample to be tested, complete the atomization of the sample to be tested, and are excited by the pulsed excitation light source at all angles to generate annular fluorescence; the working gas is introduced into the annular gap formed by the outer conductor 1 and the inner flow guide tube 16; the working gas is introduced in the tangential or radial direction of the annular gap formed by the outer conductor 1 and the inner flow guide tube 16, flows to the end face in the form of eddy current or laminar flow, and participates in the flame combustion process; the aerosol of the sample to be tested is introduced into the annular gap formed by the inner flow guide tube 16 and the middle flow guide tube 17; the shielding gas is introduced into the annular gap formed by the middle flow guide tube 17 and the outer flow guide tube 18; the shielding gas is introduced in the tangential direction or radial direction of the annular gap formed by the middle flow guide tube 17 and the outer flow guide tube 18, and forms an eddy current or laminar shielding layer.
作为优选,所述标准样品激发光源位于微波同轴谐振腔的中心轴线上(如图2所示),微波同轴谐振腔内导体4上端面低于环形原子化器上端面5~15mm;所述原子化器部分环绕所述标准样品激发光源周围相同高度上;所述标准样品激发光源发出的激发光在360度(全角度)方向上照射环绕其周围的原子化器,待测样品在原子化器内原子化后被激发光全角度激发,产生环形荧光;在荧光环外部可以设置多个荧光检测器,提高测量灵敏度。Preferably, the standard sample excitation light source is located on the central axis of the microwave coaxial resonant cavity (as shown in FIG. 2 ); the upper end surface of the conductor 4 in the microwave coaxial resonant cavity is 5 to 15 mm lower than the upper end surface of the annular atomizer; the atomizer portion surrounds the standard sample excitation light source at the same height; the excitation light emitted by the standard sample excitation light source illuminates the atomizer surrounding it in a 360-degree (full angle) direction, and the sample to be tested is atomized in the atomizer and excited at all angles by the excitation light to generate annular fluorescence; multiple fluorescence detectors can be arranged outside the fluorescence ring to improve the measurement sensitivity.
作为优选,所述进样系统22具体结构包括蠕动泵220、电磁阀A221、注射泵222、电磁阀B223、气动雾化器A224、旋流雾室A225、旋流雾室B226、气动雾化器B227。Preferably, the specific structure of the sampling system 22 includes a peristaltic pump 220, a solenoid valve A221, a syringe pump 222, a solenoid valve B223, a pneumatic nebulizer A224, a cyclonic mist chamber A225, a cyclonic mist chamber B226, and a pneumatic nebulizer B227.
一种使用所述的基于一体化全角度激发源的原子荧光光谱仪进行荧光测量方法,有以下步骤:A method for fluorescence measurement using the atomic fluorescence spectrometer based on the integrated full-angle excitation source comprises the following steps:
1)与待测样品元素种类相同的标准样品气溶胶以脉冲方式进样到激发光源,获得脉冲式激发光;1) The standard sample aerosol with the same element type as the sample to be tested is injected into the excitation light source in a pulsed manner to obtain pulsed excitation light;
2)未知浓度的待测样品气溶胶以连续方式进样到环形原子化器,被连续原子化;2) The sample aerosol of unknown concentration is continuously injected into the annular atomizer and atomized continuously;
3)激发光脉冲式激发原子化后的待测样品原子,获得在时间上可分辨的待测样品脉冲荧光信号;3) Exciting the atomized atoms of the sample to be tested by pulsed excitation light to obtain a temporally resolvable pulse fluorescence signal of the sample to be tested;
4)利用光电检测器测量脉冲荧光信号,再结合仪器标准曲线,经数据处理获得待测样品的浓度。4) The pulse fluorescence signal is measured using a photodetector, and then combined with the instrument standard curve, the concentration of the sample to be tested is obtained through data processing.
有益效果:Beneficial effects:
1、本发明的原子荧光光谱仪使用一体化全角度激发源的光源替代现有技术中的空心阴极灯,在时间和空间上都具有很高的稳定性,可以获得良好的测量精密度。同时,该激发光源辐射强度高,谱线窄,有利于后续荧光光谱测量。并且,该激发光源的光谱选择性好,更换激发谱线方便,只需更换引入激发光源的、与待测物元素种类相同的高浓度标准溶液即可,理论上可以适用于任何元素。1. The atomic fluorescence spectrometer of the present invention uses an integrated full-angle excitation source to replace the hollow cathode lamp in the prior art, which has high stability in time and space and can obtain good measurement precision. At the same time, the excitation light source has high radiation intensity and narrow spectrum, which is conducive to subsequent fluorescence spectrum measurement. In addition, the excitation light source has good spectral selectivity and is convenient to replace the excitation spectrum. It only needs to replace the high-concentration standard solution of the same element type as the object to be measured that introduces the excitation light source. In theory, it can be applied to any element.
2、本发明的原子荧光光谱仪使用一体化全角度激发源的原子化器替代现有技术中的氢氧火焰,可以通过调节气体流量,获得理想的原子化效率和与荧光效率,提高测量灵敏度,降低检出限。同时,还可以扩大测量对象的种类,使之不再局限于依赖氢化物发生法进样的元素。2. The atomic fluorescence spectrometer of the present invention uses an atomizer with an integrated full-angle excitation source to replace the hydrogen-oxygen flame in the prior art. By adjusting the gas flow rate, the ideal atomization efficiency and fluorescence efficiency can be obtained, the measurement sensitivity can be improved, and the detection limit can be reduced. At the same time, the types of measurement objects can be expanded so that they are no longer limited to elements that rely on hydride generation method for sampling.
3、本发明中的激发源结构紧凑,光源位于中心,可以360度方向全角度激发被测样品,产生环形荧光,并且可以全角度接收荧光信号,测量灵敏度高。3. The excitation source in the present invention has a compact structure, and the light source is located in the center. It can excite the sample to be tested in 360-degree directions to generate annular fluorescence, and can receive fluorescence signals at all angles, with high measurement sensitivity.
附图说明BRIEF DESCRIPTION OF THE DRAWINGS
图1为现有的原子荧光光谱仪光路图。FIG. 1 is a light path diagram of an existing atomic fluorescence spectrometer.
图2为本发明的原子荧光光谱仪光路图。FIG. 2 is a light path diagram of the atomic fluorescence spectrometer of the present invention.
图3为实施例1的一体化全角度激发源结构示意图。FIG3 is a schematic diagram of the structure of the integrated full-angle excitation source of Example 1.
图4为实施例2的一体化全角度激发源结构示意图。FIG. 4 is a schematic diagram of the structure of an integrated full-angle excitation source of Example 2.
图5为本发明的原子荧光光谱仪总体结构流程图。FIG5 is a flow chart of the overall structure of the atomic fluorescence spectrometer of the present invention.
图6为本发明的原子荧光光谱仪进样系统流程图。FIG6 is a flow chart of the atomic fluorescence spectrometer sampling system of the present invention.
具体实施方式DETAILED DESCRIPTION
实施例1Example 1
图3为本发明使用的一体化全角度激发源的一种结构示意图,由激发光源模块和环形原子化器模块组成。所述的激发光源模块为微波同轴谐振腔,包括外导体1、微波输入端口2、微波天线3、内导体4、外层气入口5、中管6、中层气入口7、内管8、内层气入口9、标准样品管10、标准样品入口11;外导体1、内导体4、中管6、内管8、标准样品管10按由外到内的顺序依次嵌套且同轴,内导体4、中管6、内管8和样品管10在出口端面处齐平,内导体4、中管6、内管8和标准样品管10与外导体1构成嵌套同轴结构的微波谐振腔,该谐振腔的特性阻抗范围为50~80欧姆;外导体1为内部中空的圆柱体,内径为35~60mm;内导体4、中管6与内管8构成的嵌套同轴结构出口端面兼有高温火焰燃烧喷嘴功能,可同时获得微波耦合等离子体和高温火焰。FIG3 is a schematic diagram of the structure of an integrated full-angle excitation source used in the present invention, which is composed of an excitation light source module and a ring-shaped atomizer module. The excitation light source module is a microwave coaxial resonant cavity, comprising an outer conductor 1, a microwave input port 2, a microwave antenna 3, an inner conductor 4, an outer gas inlet 5, a middle tube 6, a middle gas inlet 7, an inner tube 8, an inner gas inlet 9, a standard sample tube 10, and a standard sample inlet 11; the outer conductor 1, the inner conductor 4, the middle tube 6, the inner tube 8, and the standard sample tube 10 are nested and coaxial in order from outside to inside, the inner conductor 4, the middle tube 6, the inner tube 8 and the sample tube 10 are flush at the outlet end face, the inner conductor 4, the middle tube 6, the inner tube 8 and the standard sample tube 10 and the outer conductor 1 form a microwave resonant cavity of a nested coaxial structure, and the characteristic impedance range of the resonant cavity is 50 to 80 ohms; the outer conductor 1 is a hollow cylinder with an inner diameter of 35 to 60 mm; the outlet end face of the nested coaxial structure formed by the inner conductor 4, the middle tube 6 and the inner tube 8 also has the function of a high-temperature flame combustion nozzle, and microwave coupled plasma and high-temperature flame can be obtained simultaneously.
微波输入端口2的轴线距离微波同轴谐振腔底面为所用微波波长的1/4倍,微波天线3经微波输入端口2引入微波能量并与内导体4电气连接。The axis of the microwave input port 2 is 1/4 times the wavelength of the microwave used from the bottom surface of the microwave coaxial resonant cavity. The microwave antenna 3 introduces microwave energy through the microwave input port 2 and is electrically connected to the inner conductor 4 .
作为优选,外导体1上端面与谐振腔体底面的深度为所用微波波长的(2n+1)/4倍,其中n取1、2或3,例如,当n=1时,外导体上部端面距离谐振腔体底面大约90~100mm。作为优选,内导体5的外径为10~18mm,内径为9~16mm。Preferably, the depth between the upper end surface of the outer conductor 1 and the bottom surface of the resonance cavity is (2n+1)/4 times the wavelength of the microwave used, where n is 1, 2 or 3. For example, when n=1, the distance between the upper end surface of the outer conductor and the bottom surface of the resonance cavity is about 90-100 mm. Preferably, the outer diameter of the inner conductor 5 is 10-18 mm, and the inner diameter is 9-16 mm.
外层气入口5位于内导体4下部靠近内导体4底端的径向位置,中层气入口7位于中管6下部靠近中管6底端的径向位置,内层气入口9位于内管8下部靠近内管8底端的径向位置,均采用径向进气方式。The outer gas inlet 5 is located at a radial position at the lower part of the inner conductor 4 near the bottom end of the inner conductor 4, the middle gas inlet 7 is located at a radial position at the lower part of the middle tube 6 near the bottom end of the middle tube 6, and the inner gas inlet 9 is located at a radial position at the lower part of the inner tube 8 near the bottom end of the inner tube 8, all of which adopt a radial air intake method.
从外层气入口5、中层气入口7和内层气入口9进入的易电离气体在其出口端面均以层流状态流出,利用微波电场能量电离形成微波耦合等离子体;从外层气入口5、中层气入口7和内层气入口9进入的可燃气体和助燃气体在其出口端面构成的燃烧喷嘴以层状态流出,进行燃烧形成高温火焰;微波耦合等离子体和高温火焰在相同的时间和空间上融合,形成标准样品激发光源。The easily ionized gas entering from the outer gas inlet 5, the middle gas inlet 7 and the inner gas inlet 9 flows out in a laminar state at its outlet end face, and is ionized by the microwave electric field energy to form a microwave coupled plasma; the combustible gas and the combustion-supporting gas entering from the outer gas inlet 5, the middle gas inlet 7 and the inner gas inlet 9 flow out in a layer state at the combustion nozzle formed at its outlet end face, and burn to form a high-temperature flame; the microwave coupled plasma and the high-temperature flame merge at the same time and space to form a standard sample excitation light source.
标准样品入口11位于样品管10的底部,与待测样品元素种类相同的高浓度标准样品气溶胶,经过标准样品入口11进入标准样品管10,并在标准样品管10出口侧端面进入激发光源,激发之后获得待测样品荧光测量所需的激发光。当标准样品以脉冲方式进入激发光源后,就可以获得待测样品荧光激发所需的脉冲式激发光。The standard sample inlet 11 is located at the bottom of the sample tube 10. The high-concentration standard sample aerosol with the same element type as the sample to be tested enters the standard sample tube 10 through the standard sample inlet 11 and enters the excitation light source at the end face of the outlet side of the standard sample tube 10. After excitation, the excitation light required for fluorescence measurement of the sample to be tested is obtained. When the standard sample enters the excitation light source in a pulsed manner, the pulsed excitation light required for fluorescence excitation of the sample to be tested can be obtained.
环形原子化器模块包括导流环12、工作气入口13、待测样品入口14、屏蔽气入口15、内层导流管16、中层导流管17和外层导流管18。The annular atomizer module includes a guide ring 12 , a working gas inlet 13 , a sample inlet 14 , a shielding gas inlet 15 , an inner layer guide tube 16 , a middle layer guide tube 17 and an outer layer guide tube 18 .
本实施例中,环形原子化器设置于微波输入端口2上方微波同轴谐振腔外导体1的内部,导流环12位于外导体1与内导体4构成的环形空间内部,导流环12为非金属材料;外导体1侧面设计有工作气入口13、待测样品入口14和屏蔽气入口15;导流环12外侧设计有凹形导气沟槽,导流环12内侧设计有工作气入口13和待测样品入口14;导气沟槽高度分别与外导体1侧面设计的工作气入口13和待测样品入口14高度一致;导流环12内侧依次安装内层导流管16、中层导流管17和外层导流管18,并且内层导流管16、中层导流管17和外层导流管18在上出口端面处齐平;内层导流管16、中层导流管17和外层导流管18采用石英或陶瓷,不影响腔体内部电磁场分布。内层导流管16与中层导流管17构成待测样品的环形原子化器,完成待测样品的原子化,并全角度被脉冲式激发光源激发,产生环形荧光。In this embodiment, the annular atomizer is arranged inside the outer conductor 1 of the microwave coaxial resonant cavity above the microwave input port 2, and the guide ring 12 is located inside the annular space formed by the outer conductor 1 and the inner conductor 4, and the guide ring 12 is made of non-metallic material; the side of the outer conductor 1 is designed with a working gas inlet 13, a sample inlet 14 to be tested and a shielding gas inlet 15; the outer side of the guide ring 12 is designed with a concave gas guide groove, and the inner side of the guide ring 12 is designed with a working gas inlet 13 and a sample inlet 14 to be tested; the height of the gas guide groove is respectively consistent with the height of the working gas inlet 13 and the sample inlet 14 to be tested designed on the side of the outer conductor 1; the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 are installed in sequence on the inner side of the guide ring 12, and the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 are flush at the upper outlet end face; the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 are made of quartz or ceramic, which does not affect the electromagnetic field distribution inside the cavity. The inner layer flow guide tube 16 and the middle layer flow guide tube 17 form an annular atomizer for the sample to be tested, which completes the atomization of the sample to be tested and is excited at all angles by a pulsed excitation light source to generate annular fluorescence.
工作气通入内导流管16和中导流管17构成的环形间隙;工作气以内层导流管16与中导流管17构成的环形间隙的切线方向引入,以涡流形式流向端面,参与火焰燃烧过程。工作气还可以采用内层导流管16与中导流管17构成的环形间隙的径向方向引入,以层流形式流向端面,参与火焰燃烧过程;工作气可以混合助燃气体与可燃气体,还可以同时混入惰性气体;助燃气可以采用空气或氧气,优选的采用氧气;可燃气体可以采用氢气或甲烷,优选的采用氢气。The working gas is introduced into the annular gap formed by the inner flow guide tube 16 and the middle flow guide tube 17; the working gas is introduced in the tangential direction of the annular gap formed by the inner flow guide tube 16 and the middle flow guide tube 17, flows to the end face in the form of vortex flow, and participates in the flame combustion process. The working gas can also be introduced in the radial direction of the annular gap formed by the inner flow guide tube 16 and the middle flow guide tube 17, flows to the end face in the form of laminar flow, and participates in the flame combustion process; the working gas can be mixed with combustion-supporting gas and combustible gas, and can also be mixed with inert gas at the same time; the combustion-supporting gas can be air or oxygen, preferably oxygen; the combustible gas can be hydrogen or methane, preferably hydrogen.
待测样品气溶胶通入中导流管17和外导流管18构成的环形间隙;待测样品气溶胶以中导流管17和外导流管18构成的环形间隙引入,待测样品气溶胶可以混入可燃气体或助燃气体。混入的助燃气体或可燃气体同时参与火焰燃烧过程。待测样品气溶胶还可以混入惰性气体,优选的,惰性气体选用氩气。待测样品在环形原子化器端面的火焰内进行原子化。The aerosol of the sample to be tested is introduced into the annular gap formed by the middle flow tube 17 and the outer flow tube 18; the aerosol of the sample to be tested is introduced into the annular gap formed by the middle flow tube 17 and the outer flow tube 18, and the aerosol of the sample to be tested can be mixed with combustible gas or combustion-supporting gas. The mixed combustion-supporting gas or combustible gas participates in the flame combustion process at the same time. The aerosol of the sample to be tested can also be mixed with an inert gas, and preferably, argon is selected as the inert gas. The sample to be tested is atomized in the flame on the end face of the annular atomizer.
屏蔽气通入外导流管18与外导体1构成的环形间隙;屏蔽气以外导体1的切线方向引入,并形成涡流屏蔽层。屏蔽气还可以外导体1的径向方向引入,并形成层流屏蔽层。屏蔽气可以抑制待测样品向自由空间的扩散,也避免大气成分卷入火焰原子化区产生背景干扰,有效防止原子荧光的淬灭,提高原子荧光强度。屏蔽气可以采用氧气或氩气,优选的,采用氩气。The shielding gas is passed into the annular gap formed by the outer flow guide tube 18 and the outer conductor 1; the shielding gas is introduced in the tangential direction of the outer conductor 1 to form an eddy current shielding layer. The shielding gas can also be introduced in the radial direction of the outer conductor 1 to form a laminar shielding layer. The shielding gas can inhibit the diffusion of the sample to be tested into the free space, and also prevent the atmospheric components from being involved in the flame atomization zone to produce background interference, effectively prevent the quenching of atomic fluorescence, and improve the atomic fluorescence intensity. The shielding gas can be oxygen or argon, preferably, argon.
实施例2Example 2
图4为本发明使用的一体化全角度激发源的另一种结构示意图,由激发光源模块和环形原子化器模块组成。所述的激发光源模块为微波同轴谐振腔,与激发源实施例1相同,在此不再赘述。Fig. 4 is another structural schematic diagram of the integrated full-angle excitation source used in the present invention, which is composed of an excitation light source module and a ring atomizer module. The excitation light source module is a microwave coaxial resonant cavity, which is the same as the excitation source embodiment 1 and will not be described in detail here.
本实施例中,环形原子化器设置于微波输入端口2上方微波同轴谐振腔外导体1的外部,导流环12位于微波输入端口2的上方外导体1的外部;导流环12侧面设计有工作气入口13、待测样品入口14和屏蔽气入口15;导流环12内侧依次安装内层导流管16、中层导流管17和外层导流管18,并且内层导流管16、中层导流管17和外层导流管18在上出口端面处齐平。In this embodiment, the annular atomizer is arranged outside the outer conductor 1 of the microwave coaxial resonant cavity above the microwave input port 2, and the guide ring 12 is located outside the outer conductor 1 above the microwave input port 2; the side of the guide ring 12 is designed with a working gas inlet 13, a sample inlet 14 and a shielding gas inlet 15; the inner side of the guide ring 12 is installed with an inner layer guide tube 16, a middle layer guide tube 17 and an outer layer guide tube 18 in sequence, and the inner layer guide tube 16, the middle layer guide tube 17 and the outer layer guide tube 18 are flush at the upper outlet end face.
内层导流管16、中层导流管17和外层导流管18可以采用非金属材料,如石英或陶瓷,也可以采用金属材料,如黄铜。The inner layer flow guide tube 16 , the middle layer flow guide tube 17 and the outer layer flow guide tube 18 may be made of non-metallic materials, such as quartz or ceramic, or metallic materials, such as brass.
工作气通入外导体1和内导流管16构成的环形间隙;工作气以外导体1与内导流管16构成的环形间隙的切线方向引入,以涡流形式流向端面,参与火焰燃烧过程。工作气还可以采用外导体1与内导流管16构成的环形间隙的径向方向引入,以层流形式流向端面,参与火焰燃烧过程。工作气可以混合助燃气体与可燃气体,还可以同时混入惰性气体;助燃气可以采用空气或氧气,优选的采用氧气;可燃气体可以采用氢气或甲烷,优选的采用氢气。The working gas is introduced into the annular gap formed by the outer conductor 1 and the inner flow tube 16; the working gas is introduced in the tangential direction of the annular gap formed by the outer conductor 1 and the inner flow tube 16, flows to the end face in the form of eddy current, and participates in the flame combustion process. The working gas can also be introduced in the radial direction of the annular gap formed by the outer conductor 1 and the inner flow tube 16, flows to the end face in the form of laminar flow, and participates in the flame combustion process. The working gas can be mixed with combustion-supporting gas and combustible gas, and can also be mixed with inert gas at the same time; the combustion-supporting gas can be air or oxygen, preferably oxygen; the combustible gas can be hydrogen or methane, preferably hydrogen.
待测样品气溶胶通入内导流管16和中导流管17构成的环形间隙;待测样品气溶胶以内导流管16和中导流管17构成的环形间隙引入,待测样品气溶胶可以混入可燃气体或助燃气体。混入的助燃气体或可燃气体同时参与火焰燃烧过程。待测样品气溶胶还可以混入惰性气体,优选的,惰性气体选用氩气。待测样品在环形原子化器端面的火焰内进行原子化。The aerosol of the sample to be tested is introduced into the annular gap formed by the inner flow tube 16 and the middle flow tube 17; the aerosol of the sample to be tested is introduced into the annular gap formed by the inner flow tube 16 and the middle flow tube 17, and the aerosol of the sample to be tested can be mixed with combustible gas or combustion-supporting gas. The mixed combustion-supporting gas or combustible gas participates in the flame combustion process at the same time. The aerosol of the sample to be tested can also be mixed with an inert gas, and preferably, argon is selected as the inert gas. The sample to be tested is atomized in the flame on the end face of the annular atomizer.
屏蔽气通入中导流管17与外导流管18构成的环形间隙;屏蔽气以中导流管17与外导流管18构成的环形间隙的切线方向引入,形成涡流屏蔽层。屏蔽气还可以中导流管17与外导流管18构成的环形间隙的径向方向引入,形成层流屏蔽层。屏蔽气可以抑制待测样品向自由空间的扩散,也避免大气成分卷入火焰原子化区产生背景干扰,有效防止原子荧光的淬灭,提高原子荧光强度。屏蔽气可以采用氧气或氩气,优选的,采用氩气。The shielding gas is introduced into the annular gap formed by the middle flow tube 17 and the outer flow tube 18; the shielding gas is introduced in the tangential direction of the annular gap formed by the middle flow tube 17 and the outer flow tube 18 to form an eddy current shielding layer. The shielding gas can also be introduced in the radial direction of the annular gap formed by the middle flow tube 17 and the outer flow tube 18 to form a laminar shielding layer. The shielding gas can inhibit the diffusion of the sample to be tested into the free space, and also prevent the atmospheric components from being involved in the flame atomization zone to produce background interference, effectively preventing the quenching of atomic fluorescence and improving the atomic fluorescence intensity. The shielding gas can be oxygen or argon, preferably, argon.
可以理解的是,本发明使用的激发源由于激发光源是以等离子体为主体,激发能力强,并且不存在空心阴极灯的漂移问题,因而不用定期校正仪器的工作曲线,应用更加方便。同时,与现有仪器相比,由于激发光源全角度激发环形火焰原子化器中的被测样品,可以在原子化器周围设置多个荧光检测器,且距离近,因而能够获得更高的测量灵敏度。It is understandable that the excitation source used in the present invention has a strong excitation ability because the excitation light source is mainly plasma, and there is no drift problem of hollow cathode lamp, so there is no need to regularly calibrate the working curve of the instrument, and the application is more convenient. At the same time, compared with the existing instruments, since the excitation light source excites the sample to be tested in the annular flame atomizer at all angles, multiple fluorescence detectors can be set around the atomizer, and the distance is close, so that higher measurement sensitivity can be obtained.
实施例3Example 3
参照附图5说明本发明的一种原子荧光光谱仪的结构。The structure of an atomic fluorescence spectrometer of the present invention is described with reference to FIG5 .
本发明的一种基于一体化全角度激发源的原子荧光光谱仪,包括气体控制单元21、进样系统22、微波源23、激发源24、荧光检测单元25、数据处理单元26和显示记录单元27。其中气体控制单元21用来精确控制各路气体流量,由钢瓶输入气体,经减压阀、稳压阀、稳流阀和流量计精密控制各路气体输出至激发源24的外层气体入口5、中层气体入口7、内层气体入口9、工作气入口13和屏蔽气入口15以及进样系统22中气动雾化器A和B所需的载气。以气体控制单元21输出的载气为动力,完成高浓度标准样品的雾化与脉冲进样,输送至激发光源的标准样品管内。同时,以气体控制单元21输出的载气为动力,利用氢化物发生器进行汽化或气动雾化器进行雾化,实现待测样品的连续进样,引入到激发源的环形原子化器中。进样系统22中标准样品经蠕动泵220、电磁阀A221、注射泵222和电磁阀B223输入气动雾化器A224,然后利用气体控制单元21输入到气动雾化器A224的载气,将标准样品输出到旋流雾室A225缓冲之后,以脉冲方式进样到激发源24。进样系统22中待测样品经蠕动泵220输入气动雾化器B227,然后利用气体控制单元21输入到气动雾化器B227的载气,将待测样品输出到旋流雾室B226缓冲之后,以连续方式进样到激发源24;所述气动雾化器B可以用氢化物发生器代替;所述旋流雾室B可以采用气液分离器代替。微波源23输出微波功率至激发源24的微波输入端口2。启动微波输出,激发光源产生等离子体炬焰,脉冲进样的标准样品在炬焰内被激发,发射特定波长的脉冲光辐射。待测样品进入环形火焰中被原子化。激发光源产生的脉冲光辐射以全角度照射到原子化器,激发被测样品的原子产生可以时间分辨的脉冲荧光信号,该信号进入荧光检测单元25。所述荧光检测单元25经光电检测器接收荧光信号,然后经过电子电路输出至数据处理单元26。所述数据处理单元26利用微处理器采集、处理、运算荧光信号,并输出至显示记录单元27,完成显示和存储。The present invention discloses an atomic fluorescence spectrometer based on an integrated full-angle excitation source, comprising a gas control unit 21, an injection system 22, a microwave source 23, an excitation source 24, a fluorescence detection unit 25, a data processing unit 26 and a display and recording unit 27. The gas control unit 21 is used to accurately control the flow of each gas. The gas is input from a steel cylinder, and the gas is accurately controlled by a pressure reducing valve, a pressure stabilizing valve, a flow stabilizing valve and a flow meter to be output to the outer gas inlet 5, the middle gas inlet 7, the inner gas inlet 9, the working gas inlet 13 and the shielding gas inlet 15 of the excitation source 24 and the carrier gas required by the pneumatic atomizers A and B in the injection system 22. The carrier gas output by the gas control unit 21 is used as a power to complete the atomization and pulse injection of high-concentration standard samples and transport them to the standard sample tube of the excitation light source. At the same time, the carrier gas output by the gas control unit 21 is used as a power to vaporize by a hydride generator or atomize by a pneumatic atomizer to achieve continuous injection of the sample to be tested and introduce it into the annular atomizer of the excitation source. The standard sample in the injection system 22 is input into the pneumatic nebulizer A224 via the peristaltic pump 220, the solenoid valve A221, the syringe pump 222 and the solenoid valve B223, and then the carrier gas input into the pneumatic nebulizer A224 by the gas control unit 21 is used to output the standard sample to the cyclonic spray chamber A225 for buffering, and then the sample is injected into the excitation source 24 in a pulsed manner. The sample to be tested in the injection system 22 is input into the pneumatic nebulizer B227 via the peristaltic pump 220, and then the carrier gas input into the pneumatic nebulizer B227 by the gas control unit 21 is used to output the sample to be tested to the cyclonic spray chamber B226 for buffering, and then the sample is injected into the excitation source 24 in a continuous manner; the pneumatic nebulizer B can be replaced by a hydride generator; the cyclonic spray chamber B can be replaced by a gas-liquid separator. The microwave source 23 outputs microwave power to the microwave input port 2 of the excitation source 24. Start the microwave output, the excitation light source generates a plasma torch flame, and the pulsed standard sample is excited in the torch flame, emitting pulsed light radiation of a specific wavelength. The sample to be tested enters the annular flame and is atomized. The pulsed light radiation generated by the excitation light source irradiates the atomizer at all angles, exciting the atoms of the sample to be tested to generate a pulsed fluorescence signal that can be resolved in time, and the signal enters the fluorescence detection unit 25. The fluorescence detection unit 25 receives the fluorescence signal through a photodetector, and then outputs it to the data processing unit 26 through an electronic circuit. The data processing unit 26 uses a microprocessor to collect, process, and calculate the fluorescence signal, and outputs it to the display recording unit 27 to complete the display and storage.
实施例4Example 4
结合附图6说明利用本发明的原子荧光光谱仪进行荧光光谱测量方法。基于本发明的原子荧光光谱仪,具体的荧光光谱测量步骤为:The fluorescence spectrum measurement method using the atomic fluorescence spectrometer of the present invention is described in conjunction with Figure 6. Based on the atomic fluorescence spectrometer of the present invention, the specific fluorescence spectrum measurement steps are:
(1)取合适含量的、与待测样品元素种类相同的标准样品溶液,利用注射泵和电磁阀经同轴气动雾化器雾化后形成脉冲气溶胶进入旋流雾室A,缓冲之后进入标准样品入口11。经样品管10进入激发光源的中央通道,被激发光源激发,获得被测样品荧光测量所需的脉冲式激发光;(1) Take a standard sample solution with an appropriate content and the same element type as the sample to be tested, use a syringe pump and a solenoid valve to form a pulse aerosol after being atomized by a coaxial pneumatic atomizer and enter the cyclonic spray chamber A, and then enter the standard sample inlet 11 after buffering. Enter the central channel of the excitation light source through the sample tube 10, be excited by the excitation light source, and obtain the pulsed excitation light required for fluorescence measurement of the sample to be tested;
(2)未知浓度的待测样品经氢化物发生器或气动雾化器雾化后进入旋流雾室B,缓冲之后连续进入待测样品入口14,在环形原子化器的火焰内被连续原子化;(2) The sample to be tested of unknown concentration is atomized by a hydride generator or a pneumatic atomizer and enters the cyclonic spray chamber B. After being buffered, it continuously enters the sample inlet 14 to be tested and is continuously atomized in the flame of the annular atomizer.
(3)激发光脉冲式激发原子化后的待测样品,获得在时间上可以分辨的环形脉冲荧光信号;(3) Exciting the atomized sample with a pulsed excitation light to obtain a time-resolvable annular pulse fluorescence signal;
(4)利用光电检测器测量脉冲荧光信号,再结合仪器标准曲线,经数据处理获得待测样品的浓度,完成待测样品的测量。(4) The pulse fluorescence signal is measured using a photodetector, and then combined with the instrument standard curve, the concentration of the sample to be tested is obtained through data processing to complete the measurement of the sample to be tested.
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| CN207163911U (en) * | 2017-07-17 | 2018-03-30 | 吉林大学 | A kind of Atomic Emission Spectrometer AES based on microwave coupling plasma |
| CN108398414B (en) * | 2018-05-30 | 2024-03-08 | 吉林大学 | Microwave coupling plasma excitation light source |
| CN108387567A (en) * | 2018-05-30 | 2018-08-10 | 吉林大学 | A kind of microwave coupling Plasma-Atomic device for Atomic Fluorescence Spectrometer |
| CN212059915U (en) * | 2020-03-23 | 2020-12-01 | 四川大学 | Atomic emission spectroscopy excitation source and its atomic emission spectroscopy analysis device |
| CN211905077U (en) * | 2020-03-26 | 2020-11-10 | 四川大学 | Atomic Absorption, Fluorescence and Emission Spectroscopy Simultaneous Measurement Analysis Detection System |
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| CN114845454A (en) * | 2022-03-24 | 2022-08-02 | 吉林大学 | A microwave-coupled plasma and high-temperature flame fusion excitation source |
| CN114778506A (en) * | 2022-04-28 | 2022-07-22 | 吉林大学 | Integrated all-angle excitation source for atomic fluorescence spectrometer |
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