JPS6220499B2 - - Google Patents
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- Publication number
- JPS6220499B2 JPS6220499B2 JP20115381A JP20115381A JPS6220499B2 JP S6220499 B2 JPS6220499 B2 JP S6220499B2 JP 20115381 A JP20115381 A JP 20115381A JP 20115381 A JP20115381 A JP 20115381A JP S6220499 B2 JPS6220499 B2 JP S6220499B2
- Authority
- JP
- Japan
- Prior art keywords
- tube
- fine particles
- crucible
- particulate
- sample
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/71—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited
- G01N21/73—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited using plasma burners or torches
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- Health & Medical Sciences (AREA)
- Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Plasma & Fusion (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Life Sciences & Earth Sciences (AREA)
- Engineering & Computer Science (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
Description
【発明の詳細な説明】
本発明は、現在実用される固体発光分光分析装
置では形や大きさの制限を受けて対象とならない
小形状の金属試料を、高温で溶解しながら直接発
光分光分析する方法及び装置に関するものであ
る。DETAILED DESCRIPTION OF THE INVENTION The present invention performs direct emission spectroscopic analysis of small metal samples, which cannot be analyzed by currently available solid-state emission spectrometers due to shape and size limitations, while melting them at high temperatures. METHODS AND APPARATUS.
金属製造業における金属や合金の製造工程管理
あるいは製品の品質管理には、主成分や含有され
る微量成分の分析が必須で、この分析には一般に
JIS KO116―1965などに示されている固体発光
分光分析法が活用されている。この発光分光分析
法は金属試料片と対電極間に高電圧をかけてスパ
ーク放電やアーク放電等を行なわせ、蒸発した各
成分による励起光を分光してそれらのスペクトル
線強度から試料中の各成分含有率を求める方法で
ある。対象とする分析試料の形状は、放電を行な
わせる装置構造から一定の制限を受ける。通常、
直径15mmφ以上の平面を有していることが必要
で、これより小形状の塊状試料、シエーパーやド
リルで採取した切削状試料あるいは粉末試料の分
析は困難である。これらの小形状試料は、通常鉱
酸等で溶解して溶液化したのち、吸光光度法、原
子吸光法あるいは溶液発光分光法等の各種の分析
法によつて分析している。これらの分析方法は操
作が煩雑で時間がかかり、個人誤差が生じ易い等
多くの問題があることから、小形金属試料を直接
簡単・迅速に分析できる新規分析方法及び装置の
開発が強く要請されていた。 In the metal manufacturing industry, it is essential to analyze the main components and trace components contained in metals and alloys for manufacturing process control and product quality control.
Solid-state emission spectrometry methods, such as those specified in JIS KO116-1965, are utilized. In this optical emission spectrometry method, a high voltage is applied between a metal sample piece and a counter electrode to cause spark discharge or arc discharge, and the excitation light from each vaporized component is separated into spectra. This is a method for determining component content. The shape of the target analysis sample is subject to certain restrictions due to the structure of the device that causes the discharge. usually,
It is necessary to have a flat surface with a diameter of 15 mm or more, and it is difficult to analyze smaller bulk samples, cut samples taken with a shaper or drill, or powder samples. These small-sized samples are usually dissolved into a solution using a mineral acid or the like, and then analyzed by various analytical methods such as spectrophotometry, atomic absorption spectroscopy, or solution emission spectroscopy. These analytical methods have many problems, such as being complicated and time-consuming to operate and prone to individual errors, so there is a strong demand for the development of new analytical methods and devices that can directly analyze small metal samples simply and quickly. Ta.
本発明はかかる問題点に鑑み、小形状金属試料
を直接発光分光分析するための研究開発を実施
し、高周波誘導加熱溶解―高エネルギー―二次加
熱―蒸発微粒子の溶液捕集搬送―プラズマ励起発
光分光分析法を基本原理とし、簡単・迅速でかつ
定量精度に優れる新規分析方法及び装置を提供す
るにいたつたものである。本発明に関係する先行
発明には、特許第1051683号「超微粉末の生成方
法および装置」などがあるが、この発明は同一金
属からなるべく多量の微粉末を得るための発明で
ある。本発明者らは、毎回異なる分析試料から迅
速に金属微粒子を生成させるとともに、分析する
ために重要な微粒子を安定して効率よく分析装置
へ搬送する技術等を研究し、金属中の含有成分を
プラズマ発光分析する分析システムを新規に発明
したものである。 In view of these problems, the present invention has carried out research and development for direct emission spectroscopic analysis of small-shaped metal samples, and has developed a method that includes: high-frequency induction heating melting, high energy, secondary heating, solution collection and transportation of evaporated fine particles, and plasma-excited luminescence. The present invention has led to the provision of a new analytical method and device that is simple, rapid, and has excellent quantitative accuracy, based on the basic principle of spectroscopic analysis. Prior inventions related to the present invention include Japanese Patent No. 1051683, ``Method and Apparatus for Producing Ultrafine Powder,'' and this invention is an invention for obtaining as much fine powder as possible from the same metal. The present inventors have researched techniques to rapidly generate metal fine particles from a different analysis sample each time, and to stably and efficiently transport the fine particles important for analysis to an analyzer, and to analyze the components contained in metals. This is a newly invented analysis system for plasma emission analysis.
図面に示した本発明の実施例に基づいて本発明
の詳細な説明をする。本発明装置は、分析試料3
を加熱溶解して微粒子として蒸発させる微粒子発
生装置1、微粒子を不活性気体によつて搬送する
ための微粒子搬送管15、微粒子溶液中の捕集す
るための微粒子捕集管20及び微粒子を励起発光
させて分光検出し、試料中の諸成分含有率を求め
るプラズマ発光分光分析装置39を主体に構成さ
れる。 The present invention will be described in detail based on embodiments of the present invention shown in the drawings. The device of the present invention can analyze sample 3.
A particulate generator 1 that heats and melts and evaporates as particulates, a particulate transport pipe 15 that transports particulates with an inert gas, a particulate collection pipe 20 that collects particulates in a particulate solution, and a particulate matter that excites the particulates to emit light. The main component is a plasma emission spectrometer 39 that performs spectroscopic detection to determine the content of various components in the sample.
微粒子発生装置1は、分析試料3を収容する耐
火ルツボ4、これをほとんど密閉状態で収容する
微粒子発生用円筒管2、円筒管2の外周にルツボ
4の高さに見合う位置に設定された高周波誘導加
熱装置6、溶融金属表面の中心に対して垂直位置
の周囲45゜までの傾斜角で挿入された二次加熱装
置7、円筒管2内の所定位置にルツボ4を設置し
て密閉状態に保ちかつ二次加熱源の対極ともなり
得る冷却機構付のルツボ設定装置8、円筒管2内
を不活性雰囲気に保ち蒸発微粒子を分析装置39
へ運ぶ搬送気体供給装置13はどから構成され
る。この微粒子発生装置1は微粒子搬送管15及
び15′によつて搬送気体分配装置17を介して
微粒子捕集管20に接続されており、同捕集管2
0は微粒子捕集溶液注入管25を介して分析装置
39に接続されている。 The particle generator 1 includes a refractory crucible 4 that accommodates an analysis sample 3, a cylindrical tube 2 for particle generation that accommodates the analysis sample 3 in an almost airtight state, and a high-frequency generator set on the outer periphery of the cylindrical tube 2 at a position corresponding to the height of the crucible 4. An induction heating device 6, a secondary heating device 7 inserted at an inclination angle of up to 45° from a position perpendicular to the center of the molten metal surface, and a crucible 4 placed in a predetermined position inside the cylindrical tube 2 in a sealed state. A crucible setting device 8 with a cooling mechanism that can be used as a counter electrode to the secondary heating source, and a device 39 that keeps the inside of the cylindrical tube 2 in an inert atmosphere and analyzes evaporated fine particles.
The carrier gas supply device 13 for conveying the gas to the This particulate generator 1 is connected to a particulate collection pipe 20 via a transport gas distribution device 17 by particulate transport pipes 15 and 15'.
0 is connected to an analyzer 39 via a particle collection solution injection pipe 25.
耐火ルツボ4中に入れた小形状金属試料片3は
高周波誘導加熱装置6によつて短時間で溶解さ
れ、試料は溶融状態に保持される。次に二次加熱
源によつて試料の溶湯表面を過熱し、試料3を微
粒子として蒸発させる。高周波誘導加熱あるいは
プラズマアーク加熱のみでも微粒子の蒸発は起る
が、高周波誘導加熱によつて試料を迅速に溶解し
溶融状態を保持しておいて更に高エネルギーをも
つ二次加熱装置で微粒子を蒸発させる方法は、試
料中の蒸発しにくい成分の蒸発を確実とし、蒸発
量を多くでき、蒸発微粒子の粒度分布を狭くする
ことができるなどの効果があり、定量精度の向
上、分析時間の短縮に寄与する。試料を微粒子と
して蒸発させて分析する時間は通常数分の短い時
間であるので、試料溶解のための高周波加熱と試
料を微粒子として蒸発させるための二次加熱と
は、試料溶解後高周波加熱は止めて二次加熱のみ
で微粒子を蒸発させる、両者の加熱を併行して行
ない微粒子を蒸発させるなどの方法があるが、先
ず最初に試料を高周波誘導加熱によつて溶解し溶
融状態とした後、高周波電流を溶湯の撹拌が起ら
ない程度に低下させて二次加熱によつて微粒子を
蒸発させる方法が適当であつた。 The small metal sample piece 3 placed in the refractory crucible 4 is melted in a short time by the high frequency induction heating device 6, and the sample is maintained in a molten state. Next, the surface of the molten metal of the sample is heated by a secondary heating source, and sample 3 is evaporated as fine particles. Evaporation of fine particles occurs with high-frequency induction heating or plasma arc heating alone, but high-frequency induction heating quickly melts the sample and maintains the molten state, and then evaporates fine particles using a secondary heating device with high energy. This method ensures the evaporation of difficult-to-evaporate components in the sample, increases the amount of evaporation, and narrows the particle size distribution of evaporated particles, improving quantitative accuracy and shortening analysis time. Contribute. The time required to evaporate the sample as fine particles and analyze it is usually a short time of several minutes, so the high-frequency heating for dissolving the sample and the secondary heating for evaporating the sample as fine particles are the same as when the high-frequency heating is stopped after the sample has been dissolved. There are methods to evaporate the fine particles using only secondary heating, or to evaporate the fine particles by performing both heating at the same time.First, the sample is melted by high-frequency induction heating to a molten state, and then the fine particles are evaporated by high-frequency induction heating. An appropriate method was to lower the electric current to such an extent that stirring of the molten metal did not occur, and to evaporate the fine particles by secondary heating.
二次加熱装置は、第1図ではプラズマアーク銃
を示したが、スパークあるいはアーク放電装置、
レーザービーム発振装置など高エネルギーの加熱
源を使用できる。二次加熱源は金属の溶湯表面を
更に高温の過熱状態として蒸発を促進するための
ものであるが、その加熱源の溶湯面への照射方法
は金属の蒸発効率に大きく影響する。特に溶湯面
への照射角度及び湯面との距離が重要である。第
1図は溶湯面に対して直上から照射した実施例を
示した。溶湯面を過熱状態に保ち、なおかつ蒸発
微粒子を効率よく分析装置へ搬送するためには、
ルツボ中の溶湯面の中心に対して直上から二次加
熱源による高エネルギーを照射する方法が最も有
効であつた。ただし、二次加熱装置が大型となつ
て小型の円筒管2の上部への設置が困難な場合
は、溶湯面の中心に対する垂直位置の周囲45゜ま
での傾斜角度内からの照射も適用できた。ただ
し、垂直位置に対して45゜以上傾斜した位置、す
なわち溶湯面に対して水平に近い角度で照射した
場合、二次加熱源による湯面の照射位置の高温過
熱が不均一になり易くなつて効率が悪く、又、プ
ラズマアークの場合などはプラズマ炎が湯面で反
対方向に反射されて蒸発微粒子はこの流れに乗つ
て飛散してしまうなど分析装置への搬送に困難を
きたす。上述のいずれの二次加熱源についても溶
湯面との距離は、それぞれの最適位置に保たなけ
ればならない。これは、溶湯面を効率よく過熱状
態に保つことと、本発明の目的は蒸発微粒子を捕
集して製造することでなく連続的に搬送して分析
するためであるので常時一定速度での蒸発を確保
しなければならないためである。蒸発加熱時間は
短いのでその際の湯面変動は起らないが、毎回の
分析試料毎の湯面位置は一定とする必要がある。
本発明では、二次加熱源位置とルツボ設定位置は
一定とし、ルツボ中に投入する試料を一定重量に
規制して湯面位置の一定化及び二次加熱源と湯面
との間隔の一定化をはかつた。 The secondary heating device is a plasma arc gun shown in Figure 1, but spark or arc discharge devices,
High-energy heating sources such as laser beam oscillators can be used. The secondary heating source is used to heat the surface of the molten metal to a higher temperature to promote evaporation, but the method of irradiating the molten metal surface with the heating source greatly affects the evaporation efficiency of the metal. In particular, the irradiation angle to the molten metal surface and the distance from the molten metal surface are important. FIG. 1 shows an example in which the molten metal surface was irradiated from directly above. In order to maintain the molten metal surface in a superheated state and to efficiently transport the evaporated particles to the analyzer,
The most effective method was to irradiate high energy from a secondary heating source directly above the center of the molten metal surface in the crucible. However, if the secondary heating device is so large that it is difficult to install it above the small cylindrical tube 2, irradiation can also be applied from within an angle of inclination of up to 45° around the vertical position to the center of the molten metal surface. . However, if the irradiation is performed at a position inclined at an angle of 45° or more relative to the vertical position, that is, at an angle close to horizontal to the molten metal surface, the high temperature overheating of the irradiation position of the molten metal surface by the secondary heating source tends to become uneven. It is inefficient, and in the case of a plasma arc, the plasma flame is reflected in the opposite direction from the hot water surface, making it difficult to transport the evaporated particles to the analyzer, as they are scattered along with this flow. The distance from the molten metal surface to any of the above-mentioned secondary heating sources must be maintained at their optimum position. This is to efficiently maintain the molten metal surface in a superheated state, and because the purpose of the present invention is not to collect and manufacture evaporated fine particles, but to continuously transport and analyze them, evaporation is carried out at a constant rate. This is because it is necessary to ensure that Since the evaporation heating time is short, no fluctuations in the hot water level occur during that time, but the hot water level position for each analysis sample must be kept constant.
In the present invention, the position of the secondary heating source and the setting position of the crucible are kept constant, and the weight of the sample introduced into the crucible is controlled to be constant, so that the position of the hot water level is constant and the distance between the secondary heating source and the hot water level is constant. I ran.
ルツボ4は高温で浸食されにくいアルミナ、マ
グネシアあるいは炭素などで製作したものが適当
である。レーサービームを二次加熱源とする場合
は必要ないが、アークやプラズマアークを使用す
る場合はルツボ4の底部に銅電極5を取り付けた
ものを用いる。プラズマ発光分光分析装置24は
検出感度が高いために分析試料量は数グラムの少
量でよく、従つてルツボ4は小型のもので十分で
ある。分析試料の蒸発及び分析は数分間の短時間
で終了してしまうため、微粒子発生用円筒管2内
に分析試料を設定するルツボ設定装置8による試
料変換操作は迅速・簡単に行なわなければならな
い。本発明実施例には最も容易に行なえる例とし
て上部にルツボ4をのせたルツボ設定装置8の上
下動操作による試料交換方法を採用した。ルツボ
設定装置8は熱伝導率及び電気伝導率にすぐれる
銅などで製作したたて長状のもので途中には受け
台9を取りつけてあり、試料変換を行なつた後微
粒子発生用円筒管2に対し上方に押しつけて円筒
管2内を密閉状態に保つことができる。又、ルツ
ボ設定装置8には冷却水供給管10及び同排出管
11を取り付けて、ルツボ4底部の銅電極や設置
装置8自体の冷却を行なつている。又、スパー
ク、アーク、プラズマアークを二次加熱源に用い
る場合は、ルツボ設定装置8はそれらの対電極も
兼ねる。ルツボ設定装置8の受け台9などに搬送
気体吹込み管12を取りつけ、これには気体流量
の調節器14を備えた搬送気体供給装置13を接
続してある。分析試料の高周波誘導加熱による溶
解及び二次加熱装置による微粒子の蒸発は、金属
の酸化反応防止等から通常Ar、He、N2等の不活
性気体の雰囲気で行ない、微粒子の搬送もこれら
の不活性気体の吹込みによつて取り行なう。従つ
て、蒸発微粒子は搬送気体によつて希釈される
が、希釈倍率が高なると分析装置39による検出
が困難となる。そのためには、微粒子を発生させ
る空間を極力小さくすることが必要で、すなわ
ち、円筒管2はその内側に設置されるルツボ4の
外径との距離をなるべく近づけた小径のものを用
いる。円筒管2の材質は熱伝導性、耐熱性にすぐ
れる石英ガラス等が適当である。 The crucible 4 is suitably made of alumina, magnesia, carbon, or the like, which is resistant to corrosion at high temperatures. Although it is not necessary when a laser beam is used as the secondary heating source, when an arc or plasma arc is used, a crucible 4 with a copper electrode 5 attached to the bottom is used. Since the plasma emission spectrometer 24 has a high detection sensitivity, the amount of sample to be analyzed can be as small as several grams, and therefore a small crucible 4 is sufficient. Since the evaporation and analysis of the analysis sample are completed in a short period of several minutes, the sample conversion operation by the crucible setting device 8, which sets the analysis sample in the cylindrical tube 2 for generating fine particles, must be performed quickly and easily. In the embodiment of the present invention, as the easiest example, a sample exchange method was adopted in which the crucible setting device 8 on which the crucible 4 was placed was moved up and down. The crucible setting device 8 is a vertically elongated device made of copper or the like with excellent thermal conductivity and electrical conductivity, and a cradle 9 is attached to the middle of the crucible setting device. The inside of the cylindrical tube 2 can be kept in a sealed state by pressing upward against the tube 2. Further, a cooling water supply pipe 10 and a cooling water discharge pipe 11 are attached to the crucible setting device 8 to cool the copper electrode at the bottom of the crucible 4 and the setting device 8 itself. Further, when a spark, an arc, or a plasma arc is used as a secondary heating source, the crucible setting device 8 also serves as a counter electrode for them. A carrier gas blowing pipe 12 is attached to the pedestal 9 of the crucible setting device 8, and a carrier gas supply device 13 equipped with a gas flow rate regulator 14 is connected to this pipe. Melting of analysis samples by high-frequency induction heating and evaporation of fine particles by a secondary heating device are usually carried out in an atmosphere of inert gases such as Ar, He, and N 2 to prevent metal oxidation reactions. This is done by blowing in an active gas. Therefore, the evaporated fine particles are diluted by the carrier gas, but as the dilution ratio increases, detection by the analyzer 39 becomes difficult. For this purpose, it is necessary to make the space in which the particles are generated as small as possible. That is, the cylindrical tube 2 is of a small diameter and is as close as possible to the outer diameter of the crucible 4 installed inside the tube. A suitable material for the cylindrical tube 2 is quartz glass or the like, which has excellent thermal conductivity and heat resistance.
耐火ルツボ4中で溶解された分析試料3から煙
状となつて発生する微粒子は熱による対流から通
常溶湯表面上に上昇する動きをとり、その後に周
囲に拡散してゆく。蒸発微粒子を粉体として捕集
することが目的の場合は、拡散による多少の損失
も問題にならないが、試料の成分量を分析する本
発明に於いては、蒸発微粒子の全量あるいは常時
安定した一定割合量を搬送気体と共に分析装置へ
送り込まなければならない。蒸発微粒子を捕集し
て製造する場合とはこの点が大いに異なり、より
効率の良い微粒子の搬送技術が必須となる。溶湯
表面に対して水平に近い斜め方向から搬送気体を
吹きつけて微粒子をその反対側の水平方向へ送り
込む方法なども考えられるが、本発明で必須とな
る定量的な微粒子の搬送を目的とする場合には、
溶湯表面より発生して直上方向に立ち昇つた微粒
子を周囲への拡散が起る前に、やはり溶湯面を直
上方向に向つて流れる搬送気体の流れに乗せて迅
速に運び去る方法が最も効率良く、適切であつ
た。すなわち、微粒子搬送管15は、ルツボ4中
の溶湯表面から一定間隔をもつてその直上に垂直
に設置されるべきである。搬送管15の開口部の
形状はルツボ4の内径よりも小径の円筒管ないし
はルツボの外径近くまで先端を円錐形状に拡げた
ものが適当である。搬送気体は吹込み管12から
吹込まれて円筒管2内を不活性雰囲気に保つが、
出口は微粒子搬送口きりないので溶湯表面近傍を
通つてその開口部に向う気体の流れができる。溶
湯面から二次加熱源によつて発生させられ上昇し
た微粒子は、その搬送気体の気流に引き込まれ
て、常時一定希釈倍率をもつて搬送管口へ送り込
まれる。二次加熱源を溶湯直上部から照射する場
合、加熱源の周囲を同心円状に囲つた円筒管を搬
送口14とする構造が適当である。二次加熱源を
斜め方向から照射する場合は、照射中心面直上に
搬送管15の開口部を設けるのがよい。プラズマ
アーク銃7等を用いる場合に於いても、その設置
角度を溶湯面に対して垂直位置を中心に45゜以内
の傾斜角度とするならば、プラズマの照射の強さ
にも影響されるが、通常の場合プラズマ炎によつ
て微粒子は多少の拡散を生じるが搬送気体の気流
に乗せられてほとんど確実に直上部の搬送管15
へと送り込まれる。円筒管2の内壁及び微粒子搬
送管15は、高温の溶融試料による加熱でかなり
の高温となつているために微粒子は付着しにく
い。微粒子が円筒管2内に拡散浮遊してしまう
と、次の試料の分析に移る前にそれらを予め排除
しなければならず非常に煩雑になるが、本方式に
よれば微粒子が溶湯面より発生して上昇する流れ
を一種のエアーカーテン状の搬送気体の気流で包
み込んでしまうので微粒子の拡散は起りにくくそ
の心配はない。 Fine particles generated in the form of smoke from the analysis sample 3 melted in the refractory crucible 4 usually move upward onto the surface of the molten metal due to convection caused by heat, and then diffuse into the surroundings. If the purpose is to collect evaporated fine particles as a powder, some loss due to diffusion is not a problem, but in the present invention, which analyzes the amount of components in a sample, it is necessary to collect the total amount of evaporated fine particles or a stable constant amount at all times. A proportionate amount must be delivered to the analyzer together with the carrier gas. This point is very different from the case where evaporated fine particles are collected and manufactured, and a more efficient fine particle transport technology is essential. Although methods such as blowing a carrier gas from an oblique direction close to horizontal to the molten metal surface and sending the fine particles to the opposite horizontal direction are possible, the purpose of this method is to quantitatively convey the fine particles, which is essential in the present invention. in case of,
The most efficient method is to carry the fine particles that are generated from the molten metal surface and rise directly upwards, and quickly carry them away by carrying them in the flow of carrier gas that flows directly above the molten metal surface, before they diffuse to the surroundings. , was appropriate. That is, the particulate transport pipe 15 should be installed vertically and directly above the surface of the molten metal in the crucible 4 at a constant distance. The shape of the opening of the transport tube 15 is suitably a cylindrical tube with a diameter smaller than the inner diameter of the crucible 4, or one whose tip expands into a conical shape close to the outer diameter of the crucible. The carrier gas is blown in from the blowing pipe 12 to maintain an inert atmosphere inside the cylindrical pipe 2.
Since the outlet is not a particulate transport port, gas flows toward the opening through the vicinity of the molten metal surface. The fine particles generated by the secondary heating source and raised from the surface of the molten metal are drawn into the flow of the carrier gas and are sent to the port of the carrier pipe at a constant dilution ratio. When the secondary heat source is applied from directly above the molten metal, it is appropriate to use a structure in which the transfer port 14 is a cylindrical tube concentrically surrounding the heat source. When irradiating with the secondary heat source from an oblique direction, it is preferable to provide the opening of the transport pipe 15 directly above the irradiation center plane. Even when using a plasma arc gun 7, etc., if the angle of installation is within 45° from the vertical position to the molten metal surface, it will be affected by the intensity of plasma irradiation. In normal cases, the particles will be diffused to some extent by the plasma flame, but they will be carried by the carrier gas airflow and will almost certainly reach the carrier pipe 15 directly above.
sent to. The inner wall of the cylindrical tube 2 and the particle transport tube 15 are heated to a considerably high temperature by the high-temperature molten sample, so that particles are difficult to adhere to. If fine particles are diffused and suspended in the cylindrical tube 2, they must be removed before proceeding to the analysis of the next sample, which becomes very complicated, but with this method, fine particles are generated from the molten metal surface. Since the rising flow is surrounded by a kind of air curtain-like carrier gas flow, diffusion of fine particles is unlikely to occur, so there is no need to worry about it.
微粒子の蒸発発生速度及び粒径は、蒸発させる
雰囲気の圧力、加熱温度、雰囲気気体の種類等に
よつて大きく影響される。雰囲気を減圧にすれば
蒸発速度は大となり、より多量の微粒子を得られ
る。従つて、微粒子発生量を多くする必要がある
場合には、実施例の説明図には示していないが、
微粒子発生用円筒管2内を最初に真空にしてAr
等の不活性気体を導入して減圧状態に保持し、微
粒子を発生させ、次に大気圧に戻すと共に分析装
置へ搬送するなどの方法を採用する。微粒子の粒
径は、プラズマを励起源とする発光分光分析装置
39で分析する際に定量精度に影響するので重要
であり、特に粒径を極力小さくし、その粒度分布
を狭くする必要がある。本発明装置によつて鉄鋼
試料を対象に発生させた微粒子を電子顕微鏡観察
によつて調査したところ、粒径は大略0.1μm以
下の極めて微粒であり、粒度分布の巾も比較的狭
く、プラズマ発光分光分析には最適であつた。微
小粒径の蒸発微粒子を得る条件としては、発生雰
囲気の圧力を低くする、加熱温度をあまり高くし
ない、雰囲気気体に原子量の小さいArなどを用
いることが最も適当であつた。本発明の微粒子搬
送管15の開口部を溶湯の中心の表面直上に一定
間隔をもつて設置する方法は、プラズマアークな
ど二次加熱源で発生したスプラツシユによる粗大
粒子は自重によつて落下して搬送管15へは到達
しないなどの微粒子の粒度を整えるためにも効果
が認められた。 The evaporation rate and particle size of fine particles are greatly influenced by the pressure of the evaporating atmosphere, the heating temperature, the type of atmospheric gas, and the like. If the atmosphere is reduced in pressure, the evaporation rate will increase and a larger amount of fine particles can be obtained. Therefore, if it is necessary to increase the amount of fine particles generated, although it is not shown in the explanatory diagram of the example,
The inside of the cylindrical tube 2 for particle generation is first evacuated and filled with Ar.
A method is adopted in which an inert gas such as the like is introduced and maintained in a reduced pressure state to generate fine particles, which are then returned to atmospheric pressure and transported to an analysis device. The particle size of the fine particles is important because it affects the quantitative accuracy when analyzed by the emission spectrometer 39 that uses plasma as an excitation source, and in particular, it is necessary to make the particle size as small as possible and narrow the particle size distribution. When the fine particles generated in a steel sample by the apparatus of the present invention were investigated by electron microscopy, they were found to be extremely fine particles with a diameter of approximately 0.1 μm or less, the width of the particle size distribution was also relatively narrow, and plasma emission was observed. It was ideal for spectroscopic analysis. The most suitable conditions for obtaining evaporated fine particles with a fine particle size were to lower the pressure of the generated atmosphere, to not raise the heating temperature too high, and to use Ar, which has a small atomic weight, as the atmospheric gas. The method of installing the openings of the particulate transport pipe 15 of the present invention at regular intervals just above the surface of the center of the molten metal is such that coarse particles caused by splash generated by a secondary heating source such as a plasma arc fall due to their own weight. It was also found to be effective in adjusting the particle size of the particles so that they do not reach the conveying pipe 15.
蒸発微粒子は吹込んだ不活性気体に乗せられて
搬送管15を通つて搬送気体分配装置17へ入
り、再び搬送管15′を通つて微粒子捕集管20
へ送られるが、ここで搬送管15,15′及び分
配装置17等の内壁に付着残存させないことが重
要な問題となる。単に同一蒸発微粒子を捕集する
場合には多少の残留は問題にならないが、本発明
のように微粒子を分析してもとの試料中の成分量
を求める場合には、付着残留によつて搬送気体中
の微粒子濃度が変動したり、次分析試料に対する
コンタミネーシヨンとなつて正確な分析値が得ら
れなくなる。蒸発微粒子は遅い静かな流れでの搬
送や搬送中の温度低下が起ると微粒子間の凝集や
壁面への付着残留が起り易くなる。従つて、搬送
管15,15′はなるべく小径として搬送気体の
流速を速くし、搬送気体分配装置17も小型に
し、又これらの部分には図示するようにヒーター
16を取りつけて加熱する等の配慮を行なう。
又、一旦管内壁等に付着した蒸発微粒子は、付着
後短時間以内に気体を吹きつけてやれば容易に剥
離できることが判明したので、1試料の分析終了
直後ごとに搬送気体供給装置13の流量調節弁1
4の自動切換操作によつて搬送気体の吹込み流量
を増大させて排除する方法の併用も効果があつ
た。 The evaporated particulates are carried by the blown inert gas and enter the transport gas distribution device 17 through the transport pipe 15, and then pass through the transport pipe 15' again to the particulate collection pipe 20.
However, it is an important issue here that the particles do not remain attached to the inner walls of the conveyor pipes 15, 15', the distribution device 17, etc. When simply collecting the same evaporated fine particles, a small amount of residue is not a problem, but when analyzing fine particles to determine the amount of components in the original sample as in the present invention, it is difficult to transport the particles due to the attached residue. This may cause the concentration of fine particles in the gas to fluctuate or cause contamination of the next analysis sample, making it impossible to obtain accurate analysis values. When evaporated fine particles are conveyed in a slow, quiet flow or when the temperature decreases during conveyance, aggregation among the fine particles and adhesion to the wall surface tend to occur. Therefore, the diameters of the transport pipes 15, 15' are made as small as possible to increase the flow rate of the transport gas, the transport gas distribution device 17 is also made small, and heaters 16 are attached to these parts to heat them as shown in the figure. Do the following.
In addition, it has been found that evaporated fine particles once attached to the inner wall of the tube can be easily peeled off by blowing gas within a short time after attachment. Control valve 1
It was also effective to use the method of increasing the flow rate of the carrier gas and removing it by automatic switching operation in step 4.
搬送気体分配装置17は、搬送管15より不活
性気体と共に送り込まれてきた微粒子を一旦空間
部で拡散させて更に均一化する、微粒子捕集管2
0へ導入する搬送気体の最適流量に調節するある
いは粗大微粒子を系外に排除するなどの働きを行
なうが、これらの必要がない場合には省略するこ
とができる。分配装置17は外周にヒーター16
を取りつけた小径の円筒管で、微粒子搬送管15
を側壁より挿入して管末端部を上向きに、又出口
側の搬送管15′を円筒管上部より前記搬送管1
5の末端部と対向するように一定間隔をもつて垂
直に取り付け、円筒管底部に流量調節弁19を備
えた搬送気体排出管18を取り付けてある。これ
らの各管はいずれも10mmφ以下の細管である。粗
大粒子及び分配された微粒子は余剰の搬送気体と
共に底部排出管18より系外に排出され、残りの
微粒子は一定流量の搬送気体と共に搬送管15′
を経て微粒子捕集管20へ導入される。 The carrier gas distribution device 17 is a particulate collection pipe 2 that once diffuses the particulates sent in together with an inert gas from the transport pipe 15 in a space to make them more uniform.
The function is to adjust the flow rate of the carrier gas introduced into the system to an optimum value or to exclude coarse particles from the system, but these functions can be omitted if they are not necessary. The distribution device 17 has a heater 16 on the outer periphery.
Particle transport pipe 15 is a small diameter cylindrical pipe equipped with
is inserted from the side wall with the tube end facing upward, and the outlet side conveyor tube 15' is inserted into the conveyor tube 1 from the upper part of the cylindrical tube.
The carrier gas exhaust pipe 18 is installed vertically at a constant interval so as to face the end of the cylinder 5, and a carrier gas discharge pipe 18 equipped with a flow rate control valve 19 is installed at the bottom of the cylindrical pipe. Each of these tubes is a thin tube with a diameter of 10 mm or less. Coarse particles and distributed fine particles are discharged from the system through the bottom discharge pipe 18 together with excess carrier gas, and the remaining fine particles are discharged from the conveyor pipe 15' together with a constant flow rate of carrier gas.
The particles are introduced into the particle collection tube 20 through the .
微粒子捕集管20は、小径の円筒管で上部に溶
液貯蔵タンク22及び定流量ポンプ23に接続す
る溶液供給管24を、底部に溶液排出管21を、
側部や上部などに微粒子搬送管15′及び溶液注
入管25を取り付けたものである。微粒子捕集管
20は、搬送管15′によつて送り込まれてくる
微粒子を溶液中に捕集して分析装置39へ導入す
る働きをする。微粒子の捕集の仕方にはいくつか
の方法があるが、一定量の溶液を溶液供給管24
から捕集管20に注入しておき、搬送管15′か
らの微粒子を一定時間導入して捕集する方法及び
捕集管20に溶液を一定流速で常時供給しながら
搬送管15′から導入される微粒子を連続的に捕
集する方法などが一般に採用できる。前者は微粒
子を濃縮できる利点があり、後者は捕集管20を
長尺管とすることにより微粒子を付着残留など起
さずに一定距離離れた分析装置へ搬送できる利点
がある。溶液はプラズマ発光分光分析に支障とな
らず、微粒子の分散に効果のあるものが適当で水
溶液やイソプロピルアルコール、メチルイソブチ
ルケトンのような有機溶媒が適している。又、分
散効果をあげるために捕集管20に超音波発振装
置を付属させる方法や分散剤の併用は適当であ
る。 The particulate collection tube 20 is a small diameter cylindrical tube with a solution supply tube 24 connected to a solution storage tank 22 and a constant flow pump 23 at the top, and a solution discharge tube 21 at the bottom.
A particle transport pipe 15' and a solution injection pipe 25 are attached to the side or top. The particulate collection tube 20 functions to collect particulates sent through the transport pipe 15' into a solution and introduce the collected particulates into the analyzer 39. There are several methods for collecting fine particles.
A method of injecting the solution into the collection tube 20 and then introducing it from the transport pipe 15' for a certain period of time to collect it. Generally, a method of continuously collecting fine particles can be adopted. The former has the advantage of being able to concentrate the fine particles, and the latter has the advantage of being able to transport the fine particles to an analyzer a certain distance away without causing any adhesion or residue by making the collecting tube 20 a long tube. Suitable solutions are those that do not interfere with plasma emission spectroscopy and are effective in dispersing fine particles, and suitable are aqueous solutions and organic solvents such as isopropyl alcohol and methyl isobutyl ketone. Further, in order to increase the dispersion effect, it is appropriate to attach an ultrasonic oscillator to the collection tube 20 or to use a dispersant together.
溶液に捕集された微粒子は溶液注入管25を通
つて分析装置39に導入される。分析装置39は
原子吸光分析装置などでもよいが、多成分を同時
に定量できる溶液発光分光分析装置が最も適して
いる。溶液発光分光分析の中でも定量精度、感度
に優れる高周波誘導結合型プラズマ発光分光分析
装置39が適切である。本装置39は溶液注入管
25に接続された霧化装置26、霧化装置に接続
する試料導入管27、プラズマガス供給管28、
冷却ガス供給管29から構成されるプラズマトー
チ30、トーチ上部に取り付けた高周波発生装置
31、及びプラズマ部32中で励起発光した微粒
子成分の発光スペクトルの集光レンズ33、反射
鏡35、回析格子36から構成される分光器3
4、各成分のスペクトル線強度を測定する検出器
37及び含有率算出装置38などから構成され
る。微粒子が分散して捕集された微粒子捕集器2
0中の溶液は霧化装置26に吹き込まれるArガ
スによつて、溶液注入管25を介して吸引され霧
化され、微粒子は粒径が0.1μm以下の微粉であ
るので試料導入管27からプラズマトーチ30に
導入されて励起発光され、試料中の各成分量が測
定される。 The fine particles collected in the solution are introduced into the analyzer 39 through the solution injection tube 25. The analyzer 39 may be an atomic absorption spectrometer or the like, but a solution emission spectrometer that can quantify multiple components simultaneously is most suitable. Among solution emission spectroscopy, the high frequency inductively coupled plasma emission spectrometer 39 is suitable because it has excellent quantitative accuracy and sensitivity. This device 39 includes an atomization device 26 connected to the solution injection tube 25, a sample introduction tube 27 connected to the atomization device, a plasma gas supply tube 28,
A plasma torch 30 consisting of a cooling gas supply pipe 29, a high frequency generator 31 attached to the upper part of the torch, a condensing lens 33 for the emission spectrum of the particulate component excited and emitted in the plasma section 32, a reflecting mirror 35, and a diffraction grating. Spectrometer 3 consisting of 36
4. Consists of a detector 37 that measures the spectral line intensity of each component, a content rate calculation device 38, and the like. Particulate collector 2 in which particulates are dispersed and collected
The solution in 0 is sucked through the solution injection tube 25 by the Ar gas blown into the atomization device 26 and atomized, and since the fine particles are fine particles with a particle size of 0.1 μm or less, they are injected into the plasma from the sample introduction tube 27. The sample is introduced into a torch 30 and excited to emit light, and the amount of each component in the sample is measured.
本発明によれば、分析試料の微粒子発生装置へ
の挿入から微粒子を発生させて試料中の各成分の
含有率を求めるまでの分析所要時間は約5分以内
の短時間で、ほとんど人手を用いずに簡単に分析
することができる。定量精度についても、試料を
鉱酸で溶解して、操作が煩雑で長時間を要する吸
光光度分析法などと比較して遜色のない良好な結
果を得ることができた。以上説明したように、本
発明によつてこれまで直接発光分光分析が困難で
あつた小形状金属試料に対して簡単・迅速な直接
発光分光分析が可能になつた。又、これまでの一
定形状のブロツク試料を対象とするスパーク、ア
ークあるいはグロー放電による固体発光分光分析
で、試料形状制限以外に問題となつていた試料の
熱処理履歴による金属組織や試料内の各成分の偏
析に基づく定量精度の低下等の問題解決も成し得
ることができた。 According to the present invention, the time required for analysis from inserting an analysis sample into a particle generator to generating particles and determining the content of each component in the sample is within about 5 minutes, and requires almost no manual effort. can be easily analyzed without In terms of quantitative accuracy, we were able to obtain good results comparable to those of spectrophotometric analysis, which involves dissolving the sample in mineral acid and requires a complicated and time-consuming operation. As explained above, the present invention has made it possible to perform simple and rapid direct emission spectroscopic analysis of small-sized metal samples, for which direct emission spectroscopic analysis has been difficult until now. In addition, in solid-state emission spectroscopy analysis using spark, arc, or glow discharge that targets block samples with a certain shape, in addition to the sample shape limitations, problems such as the metal structure and each component in the sample due to the heat treatment history of the sample have also been encountered. We were also able to solve problems such as a decrease in quantitative accuracy due to segregation.
本発明は、金属製造業に於る工程管理あるいは
品質管理などに必須である金属材料中に含有され
る各成分を試料形状、金属組織あるいは成分偏析
の影響を受けずに簡単・迅速に高精度で分析する
新規分析方法及び装置を提供したものであり、こ
の分野に於いて多大の貢献を成すものである。 The present invention enables easy, quick, and highly accurate measurement of each component contained in metal materials, which is essential for process control or quality control in the metal manufacturing industry, without being affected by sample shape, metal structure, or component segregation. The present invention provides a new analytical method and device for analysis, making a significant contribution to this field.
図面は本発明実施例の説明図である。
1:微粒子発生装置、2:微粒子発生用円筒
管、3:分析試料、4:耐火ルツボ、6:高周波
誘導加熱装置、7:二次加熱装置、8:ルツボ設
定装置、15,15′:微粒子搬送管、17:搬
送気体分配装置、20:微粒子捕集管、24:溶
液供給管、25:溶液注入管、26:霧化装置、
30:プラズマトーチ、34:分光器、39:プ
ラズマ発光分光分析装置。
The drawings are explanatory diagrams of embodiments of the present invention. 1: Particulate generator, 2: Cylindrical tube for particulate generation, 3: Analysis sample, 4: Refractory crucible, 6: High frequency induction heating device, 7: Secondary heating device, 8: Crucible setting device, 15, 15': Particulates Transport pipe, 17: Transport gas distribution device, 20: Particulate collection pipe, 24: Solution supply pipe, 25: Solution injection pipe, 26: Atomization device,
30: Plasma torch, 34: Spectrometer, 39: Plasma emission spectrometer.
Claims (1)
中で小形状の金属試料片を一次加熱源の高周波誘
導加熱によつて溶解し、溶解された溶湯表面中心
の直上ないしはその垂直位置の周囲45度までの傾
斜角度範囲内の位置からの高エネルギー二次加熱
源のエネルギー照射によつて蒸発金属微粒子を発
生させ、該蒸発金属微粒子を前記密閉状容器内に
吹込まれた搬送気体によつて微粒子搬送管を介し
て微粒子捕集用溶液供給装置を備えた微粒子捕集
管へ搬送して該微粒子捕集管内の溶液中に分散捕
集し、該微粒子捕集溶液を注入管、霧化装置及び
導入管を介して発光分光分析装置のプラズマ発光
部に導入し、該プラズマ発光部で発生した励起光
を発光分光分析装置の分光器で分光してその各成
分のスペクトル線強度から分析試料中に含有され
る各成分量を測定することを特徴とする小形状金
属試料の直接溶解発光分光分析方法。 2 分析試料を入れる小型耐火ルツボ、該耐火ル
ツボの外周を直近にとりまく小径でたて長の密閉
状円筒管、ルツボの高さに見合つて前記円筒管の
外周に設置した一次加熱源としての高周波誘導加
熱装置、ルツボ中の溶融金属表面の中心に対向し
た直上位置ないしはその直上位置の周囲45℃まで
の傾斜角をもつて前記円筒管に取付けた蒸発金属
微粒子を発生させるための高エネルギー照射用二
次加熱装置、流量調節器を備えて前記円筒管の下
部ないしは上部に吹込み口を設置した微粒子搬送
気体供給装置、前記円筒管の底部に設置されてル
ツボの出し入れを可能ならしめるとともに前記二
次加熱装置の対電極を兼ね、かつ前記円筒管の密
閉状態を保持できるようにしたルツボ設定装置及
び一端がルツボ中の溶融金属表面の中心部に対し
て直上部に垂直に開口し他端が後記微粒子捕集管
に接続する微粒子搬送管からなる微粒子発生装置
と; 前記微粒子搬送管の末端、微粒子捕集用溶液供
給装置、同溶液の排出管及び微粒子捕集溶液を後
記プラズマ発光装置へ注入するための微粒子捕集
溶液注入管を取付けた容器からなる微粒子捕集管
と; 該微粒子捕集管に対し前記微粒子捕集溶液注入
管により接続されるとともに後記プラズマ発光装
置への導入管を取付けた霧化装置、プラズマ励起
原を有するプラズマ発光装置、分光器、検出器及
び成分含有率演算装置等からなるプラズマ発光分
光分析装置と; を具備することを特徴とする小形状金属試料の直
接発光分光分析装置。[Claims] 1. A small metal sample piece is melted in a refractory crucible placed in a small-volume closed container by high-frequency induction heating of a primary heat source, and the sample is placed directly above or directly above the center of the surface of the molten metal. Vaporized metal fine particles are generated by energy irradiation from a high-energy secondary heating source from a position within a tilt angle range of up to 45 degrees around the vertical position, and the vaporized metal fine particles are blown into the sealed container. The particles are transported by a carrier gas through a particle transport tube to a particle collection tube equipped with a particle collection solution supply device, dispersed and collected in the solution in the particle collection tube, and the particle collection solution is injected. The excitation light is introduced into the plasma emission section of the emission spectrometer through the tube, atomization device, and introduction tube, and the excitation light generated in the plasma emission section is separated by the spectrometer of the emission spectrometer to obtain the spectral lines of each component. A direct dissolution emission spectroscopic analysis method for small metal samples, which is characterized by measuring the amount of each component contained in an analysis sample from the intensity. 2. A small refractory crucible to hold the analysis sample, a closed cylindrical tube with a small diameter and a vertical length that immediately surrounds the outer periphery of the refractory crucible, and a high frequency as a primary heating source installed on the outer periphery of the cylindrical tube in proportion to the height of the crucible. Induction heating device, for high-energy irradiation to generate evaporated metal fine particles, attached to the cylindrical tube at a position directly above the center of the molten metal surface in the crucible, or at an angle of inclination of up to 45°C around the position directly above it. a secondary heating device, a particulate carrier gas supply device equipped with a flow rate regulator and having an inlet at the bottom or top of the cylindrical tube; A crucible setting device that also serves as a counter electrode for the secondary heating device and is capable of keeping the cylindrical tube in a sealed state; one end opens vertically directly above the center of the molten metal surface in the crucible; A particulate generator comprising a particulate transport pipe connected to the particulate collection pipe described below; an end of the particulate transport pipe, a particulate collection solution supply device, a discharge pipe for the solution, and a particulate collection solution injected into the plasma light emitting device described later. a particulate collection tube consisting of a container fitted with a particulate collection solution injection pipe for the purpose of A plasma emission spectrometer comprising: an atomizer having a plasma excitation source, a plasma light emitting device having a plasma excitation source, a spectrometer, a detector, a component content calculation device, etc.; Spectroscopic analyzer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20115381A JPS58102136A (en) | 1981-12-14 | 1981-12-14 | Direct spectrochemical analytical method and apparatus for small-sized metal sample through fine particle generation and solution collection |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20115381A JPS58102136A (en) | 1981-12-14 | 1981-12-14 | Direct spectrochemical analytical method and apparatus for small-sized metal sample through fine particle generation and solution collection |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58102136A JPS58102136A (en) | 1983-06-17 |
| JPS6220499B2 true JPS6220499B2 (en) | 1987-05-07 |
Family
ID=16436259
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP20115381A Granted JPS58102136A (en) | 1981-12-14 | 1981-12-14 | Direct spectrochemical analytical method and apparatus for small-sized metal sample through fine particle generation and solution collection |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58102136A (en) |
-
1981
- 1981-12-14 JP JP20115381A patent/JPS58102136A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58102136A (en) | 1983-06-17 |
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