JPH0692929B2 - Airborne microparticle characteristics measurement device - Google Patents
Airborne microparticle characteristics measurement deviceInfo
- Publication number
- JPH0692929B2 JPH0692929B2 JP3086238A JP8623891A JPH0692929B2 JP H0692929 B2 JPH0692929 B2 JP H0692929B2 JP 3086238 A JP3086238 A JP 3086238A JP 8623891 A JP8623891 A JP 8623891A JP H0692929 B2 JPH0692929 B2 JP H0692929B2
- Authority
- JP
- Japan
- Prior art keywords
- box
- particles
- solid
- heating method
- nichrome plate
- 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 - Lifetime
Links
- 239000011859 microparticle Substances 0.000 title claims description 7
- 238000005259 measurement Methods 0.000 title description 2
- 239000002245 particle Substances 0.000 claims description 63
- 239000007788 liquid Substances 0.000 claims description 29
- 239000007787 solid Substances 0.000 claims description 24
- 229910001120 nichrome Inorganic materials 0.000 claims description 21
- 238000001514 detection method Methods 0.000 claims description 15
- 238000010438 heat treatment Methods 0.000 claims description 10
- 238000000034 method Methods 0.000 claims description 10
- 239000010419 fine particle Substances 0.000 claims description 8
- 239000011521 glass Substances 0.000 claims description 3
- 239000000443 aerosol Substances 0.000 description 11
- 238000001704 evaporation Methods 0.000 description 4
- 230000008020 evaporation Effects 0.000 description 3
- 239000003595 mist Substances 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 239000000428 dust Substances 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 238000000149 argon plasma sintering Methods 0.000 description 1
- 238000012937 correction Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 239000002274 desiccant Substances 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 238000007429 general method Methods 0.000 description 1
- 238000005303 weighing Methods 0.000 description 1
Landscapes
- Sampling And Sample Adjustment (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、気体中に浮遊する固体
状または液体状の微小粒子の粒径分布測定装置に関する
ものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an apparatus for measuring the particle size distribution of solid or liquid fine particles suspended in a gas.
【0002】[0002]
【従来の技術】液体状粒子の粒径分布測定においては、
下方に向けたノズルからエアロゾル(ダストやミストが
気体中に浮遊する系)を高速で噴出させ、これをノズル
の直下に設けた円盤状の衝突板に捕集する方法が一般的
である。すなわち、エアロゾル中の粒子はその粒径の2
乗に比例した慣性力を得て、一定以上の慣性力を有する
粒子のみがこの衝突板に衝突して付着するものであっ
て、ノズルを下方のものほど小径として上下数段に作
り、各ノズルの直下に設けた各衝突板上に溜った液滴を
各段毎に採取し、秤量して粒径ならびに分布量を求める
ものがミスト用カスケードインパクターと呼ばれる装置
である。2. Description of the Related Art In measuring the particle size distribution of liquid particles,
A general method is to eject aerosol (a system in which dust and mist are suspended in a gas) at high speed from a nozzle directed downward and collect the aerosol on a disk-shaped collision plate provided directly below the nozzle. That is, the particles in the aerosol are 2
An inertial force proportional to the power of the square is obtained, and only particles having an inertial force above a certain level collide with and adhere to this collision plate. A device called a mist cascade impactor is a device for collecting the droplets collected on each collision plate provided immediately below the column for each stage and weighing them to determine the particle size and distribution amount.
【0003】しかし、上記装置は、測定対象である液体
状粒子を衝突板に一定時間貯留させたのち、これを外部
に取り出して秤量するものであって実時間測定でなく、
液体状粒子を採取している間の蒸発や再飛散現象による
液滴の減少を起こす場合もあり、正確な粒径分布が得ら
れないという問題があった。However, the above-mentioned device stores the liquid particles to be measured in the collision plate for a certain period of time, then takes them out to the outside and weighs them.
There is a problem in that an accurate particle size distribution cannot be obtained because evaporation or re-scattering phenomenon may cause a drop in liquid particles during the collection of the liquid particles.
【0004】霧の粒径分布測定に用いられる、光散乱式
測定器においては、操作は簡単であるが、固体状粒子
(ダスト)まで測定して、霧の本体である液体状粒子
(ミスト)の情報を得ることはできない。熱線風速計を
応用して用いると液体状粒子の測定は可能であるが、固
体状粒子は不可能であり、既存の粒径分布測定装置では
固体状粒子と液体状粒子が混在する場合、それぞれの粒
径分布を測定することは困難であった。The light-scattering measuring device used for measuring the particle size distribution of fog is easy to operate, but it also measures solid particles (dust) to form liquid particles (mist) which is the main body of the fog. Can't get information about. Liquid particles can be measured by applying a hot-wire anemometer, but solid particles are not possible, and existing solid particles and liquid particles are mixed in the existing particle size distribution measuring device. It was difficult to measure the particle size distribution of.
【0005】[0005]
【発明が解決しようとする課題】解決しようとする問題
点は、固体状と液体状の粒子の区別と粒子の大きさ別の
分布測定を可能とする点である。The problem to be solved is that it is possible to distinguish between solid and liquid particles and to measure the distribution of particle size.
【0006】[0006]
【問題点を解決するための手段】液体状粒子は流動的で
かつ一般に揮発性であるから、固体状粒子と液体状粒子
が混合するエアロゾルを衝突板上に捕集して加熱するこ
とにより捕集液滴を強制的に蒸発させ、蒸発前後の衝突
板の質量を測定することにより、液体状の質量、すなわ
ち捕集液体状粒子の質量が求められる。さらに、捕集前
の衝突板の質量を測定しておけば、蒸発後の質量と捕集
前の質量の差から固体の質量、すなわち固体状の粒子の
質量が分かる。ここで、衝突板の質量の増加分はガラス
筒状の検出素子の振動数変化から求めることができる。[Means for Solving the Problems] Since liquid particles are fluid and generally volatile, the aerosol in which solid particles and liquid particles are mixed is collected on a collision plate and heated to collect the aerosol. By forcibly evaporating the collected liquid droplets and measuring the mass of the collision plate before and after the evaporation, the liquid mass, that is, the mass of the collected liquid particles is obtained. Furthermore, if the mass of the collision plate before collection is measured, the mass of solid, that is, the mass of solid particles can be known from the difference between the mass after evaporation and the mass before collection. Here, the amount of increase in the mass of the collision plate can be obtained from the change in the frequency of the glass tubular detection element.
【0007】本発明はこの点に着目するとともに、上記
従来のカスケードインパクタ装置が数段のノズルおよび
衝突板を設けて各段で粒径分布を測定しているのに対し
て、エアロゾルの吸引流量を段階的に変えることにより
装置全体を一組のノズルと衝突板のみで構成して小型化
したものである。The present invention pays attention to this point and, in contrast to the above-mentioned conventional cascade impactor device, which is provided with several stages of nozzles and collision plates to measure the particle size distribution at each stage, the suction flow rate of aerosol By gradually changing the above, the entire apparatus is made compact with only one set of nozzles and a collision plate.
【0008】[0008]
【実施例】本装置は粒子の捕集および質量検出部と電子
回路部、さらにエアロゾル吸引部から構成される。その
概略をDETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS This apparatus comprises a particle collecting and mass detecting section, an electronic circuit section, and an aerosol suction section. The outline
【図1】に示す。粒子捕集および検出部は検出箱11内に
収納されており、エアロゾルが吸引ポンプ4の作動によ
り検出箱のノズル1に導かれノズル1から衝突板5に向か
って進入する。テーパ形のガラス製筒の検出素子3の先
端に衝突板としてニクロム板5を固定し、ニクロム板5を
加熱するために必要な両電極は、外部の電源8と結線さ
れており、検出素子3の広がった他端は底部に固定され
ている。素子3の中央部には、この素子3を振動させる一
対の電極6,6’と、それに直角方向に、振動数を測定す
るための光学系(発光素子7、受光素子7’)が相対して
配設されている。素子3の振動数は先端のニクロム板5の
質量と、検出素子の物理的特性により決定される。ニク
ロム板5上に、FIG. 1 shows. The particle collecting and detecting unit is housed in the detection box 11, and the aerosol is guided to the nozzle 1 of the detection box by the operation of the suction pump 4 and enters from the nozzle 1 toward the collision plate 5. A nichrome plate 5 is fixed as a collision plate to the tip of the detection element 3 of a tapered glass tube, and both electrodes necessary for heating the nichrome plate 5 are connected to an external power source 8 and the detection element 3 The widened other end of is fixed to the bottom. A pair of electrodes 6 and 6 ′ for vibrating the element 3 and an optical system (light emitting element 7 and light receiving element 7 ′) for measuring the frequency are opposed to the center of the element 3 in the direction perpendicular to the electrodes. Are arranged. The frequency of the element 3 is determined by the mass of the nichrome plate 5 at the tip and the physical characteristics of the detection element. On the nichrome plate 5,
【数1】の慣性衝突式により計算される粒径以上の粒子
は、固体、液体の粒子に関係なくニクロム板5に慣性衝
突し、捕集される。粒子が捕集され、質量が増加すると
振動数は一定の割合で、減少する。振動数を光学系で測
定することにより、逆にニクロム板上の増加した質量を
求めることができる。Particles having a particle size equal to or larger than the particle size calculated by the inertial collision equation of [Equation 1] collide with the nichrome plate 5 regardless of solid or liquid particles and are collected. As the particles are trapped and the mass increases, the frequency decreases at a constant rate. By measuring the frequency with an optical system, on the contrary, the increased mass on the nichrome plate can be determined.
【0009】[0009]
【数1】 Dp=[(18・μ・Dn・ψ50)/(C・ρp・v)]1/2 [Equation 1] D p = [(18 ・ μ ・ D n・ ψ 50 ) / (C ・ ρ p・ v)] 1/2
【0010】上記の数式において、vはノズル1におけ
る平均流速、ρpは粒子の密度、Dpは粒子の直径、C は
カニンガムの補正係数、μは気体の粘性係数、Dnはノズ
ルの直径、ψ50は有効捕集効率50%の粒子径における係
数(=0.14)である。In the above equation, v is the average flow velocity in the nozzle 1, ρ p is the particle density, D p is the particle diameter, C is the Cunningham correction coefficient, μ is the gas viscosity coefficient, and D n is the nozzle diameter. , Ψ 50 is a coefficient (= 0.14) at a particle size with an effective collection efficiency of 50%.
【0011】第1のステップでは、固体と液体の微粒子
の含まない気体を一定吸引流量で吸引し、この状態にお
けるニクロム板5の振動数を測定する。次に、固体状と
液体状の微粒子を含むエアロゾルを一定時間、一定吸引
流量で箱11内へ吸引し、ニクロム板5上に微粒子を捕集
して振動数を測定し、先に測定したニクロム板のみの振
動数と比較することにより、固体と液体状粒子の混合し
た状態での粒子質量を求める。次にニクロム板5へ通電
することにより、ニクロム板5が加熱され捕集粒子の中
で液体状粒子だけが蒸発し、ニクロム板5上には固体状
の微粒子だけが残り、この時の粒子質量を同様に振動数
の変化から求める。固体と液体状粒子を捕集した時の質
量と、固体状になった質量の差から液体状粒子の質量を
求める。次にエアロゾルの捕集前と液体状粒子の蒸発後
の質量から捕集された固体状の粒子の質量を求める。In the first step, a gas containing no solid and liquid fine particles is sucked at a constant suction flow rate, and the frequency of the nichrome plate 5 in this state is measured. Next, the aerosol containing solid and liquid fine particles is sucked into the box 11 at a constant suction flow rate for a certain period of time, the fine particles are collected on the nichrome plate 5 to measure the frequency, and the nichrome previously measured. The particle mass in the mixed state of solid and liquid particles is obtained by comparing with the frequency of only the plate. Next, by energizing the nichrome plate 5, the nichrome plate 5 is heated to evaporate only the liquid particles in the collected particles, and only the solid fine particles remain on the nichrome plate 5, and the particle mass at this time Is similarly obtained from the change in frequency. The mass of the liquid particles is obtained from the difference between the mass when the solid particles and the liquid particles are collected and the mass of the solid particles. Next, the mass of the collected solid particles is obtained from the mass before the aerosol is collected and after the liquid particles are evaporated.
【0012】第2のステップとして、吸引流量を第1ス
テップより増加させる。こうすることにより、As the second step, the suction flow rate is increased from the first step. By doing this,
【数1】の平均流速vが速くなるため、分離粒子径Dpは
より小さくなり、第1ステップよりもさらに粒子径の小
さい微小粒子まで、ニクロム板上に捕集することができ
る。その後の固体および液体状粒子の検出は第1のステ
ップと同様の操作を繰り返す。以下、次々と吸引流量を
大きくし、各ステップにおける固体および液体状粒子の
捕集量を求めることにより、液体と固体状の粒子のそれ
ぞれの粒径分布と質量濃度を求めることができる。Since the average flow velocity v of Eq. (1) becomes faster, the separated particle diameter D p becomes smaller, and even fine particles having a smaller particle diameter than in the first step can be collected on the nichrome plate. Subsequent detection of solid and liquid particles repeats the same operation as the first step. Hereinafter, by increasing the suction flow rate one after another and obtaining the collection amounts of the solid and liquid particles in each step, the particle size distribution and mass concentration of the liquid and solid particles can be obtained.
【0013】[0013]
【発明の効果】以上説明したように本発明の気中微小粒
子特性測定装置は、粒径分布を測定するため慣性衝突方
式を、また加熱による固体および液体状粒子の識別方式
を採用しているので、構造が比較的簡単で、堅固で可動
部がないなどの利点がある。本装置を用いて大気中の霧
などの固体状と液体状の粒子を含むエアロゾルの粒径分
布測定に容易に適用できる。As described above, the apparatus for measuring the characteristics of airborne microparticles of the present invention employs the inertial collision method for measuring the particle size distribution and the method for distinguishing solid and liquid particles by heating. Therefore, there are advantages that the structure is relatively simple, it is solid, and there are no moving parts. This device can be easily applied to the measurement of the particle size distribution of aerosols containing solid and liquid particles such as fog in the atmosphere.
【0014】[0014]
【図1】気中微小粒子特性測定装置の全体の概略図であ
る。FIG. 1 is an overall schematic view of an apparatus for measuring characteristics of airborne microparticles.
【図2】気中微小粒子特性測定装置の検出素子中央部の
平面図である。FIG. 2 is a plan view of a central portion of a detection element of an apparatus for measuring characteristics of airborne microparticles.
【図3】気中微小粒子特性測定装置のニクロム板加熱方
式を赤外線加熱方式にした場合の図である。FIG. 3 is a diagram showing a case where the nichrome plate heating method of the airborne microparticle characteristics measuring apparatus is an infrared heating method.
【図4】気中微小粒子特性測定装置のニクロム板加熱方
式を高周波電磁加熱方式にした場合の図である。FIG. 4 is a diagram showing a case where a nichrome plate heating method of an airborne fine particle characteristic measuring apparatus is a high frequency electromagnetic heating method.
1 ノズル 2 排出口 3 検出素子 4 吸引ポンプ 5 ニクロム板 6,6' 振動電極 7,7' 発光素子と受光素子 8 電源 9 乾燥剤 10 検出素子駆動回路 11 検出箱 12 振動数検出回路 13 赤外線ランプ 14 高周波発振管 1 Nozzle 2 Discharge port 3 Detection element 4 Suction pump 5 Nichrome plate 6,6 'Vibration electrode 7,7' Light emitting element and light receiving element 8 Power supply 9 Drying agent 10 Detection element drive circuit 11 Detection box 12 Frequency detection circuit 13 Infrared lamp 14 high frequency oscillator
Claims (3)
れるためのノズルと箱中の気体を取り出す排出穴を有す
る箱内において、固有周期で振動するテーパ形のガラス
筒状の検出素子が、ノズル直下に検出素子の直径が大き
い方が箱内底に固定され、ノズル側の検出素子上には両
端を箱外の電源に結線して、ニクロム板が固定されてお
り、吸引ポンプにより、微小粒子を含む気体を吸引し、
慣性衝突により固体状粒子と液体状粒子をニクロム板上
に捕集させ、捕集前、捕集後とニクロム板を通電加熱し
た後の振動数から、固体と液体状粒子の粒径分布と粒径
区分毎の質量濃度を測定する装置。1. A tapered glass tube-shaped detection element vibrating at a natural period in a box having a nozzle for introducing gas in which fine particles are suspended into the box and an exhaust hole for taking out gas in the box, The one with the larger detection element diameter is fixed to the bottom of the box directly below the nozzle, and the nichrome plate is fixed on the detection element on the nozzle side by connecting both ends to the power supply outside the box. Inhale gas containing particles,
The solid and liquid particles were collected on the nichrome plate by inertial collision, and the particle size distribution and particle size of the solid and liquid particles were calculated based on the frequencies before and after the collection and after the nichrome plate was electrically heated. A device that measures the mass concentration for each diameter category.
熱方式を、箱内で赤外線電球による加熱方式にしたこと
を特徴とする請求項1の気中微小粒子特性測定装置2. The apparatus for measuring characteristics of airborne microparticles according to claim 1, wherein the heating method by energizing the nichrome plate in claim 1 is a heating method by an infrared light bulb in the box.
熱方式を、箱内で高周波電磁加熱方式にしたことを特徴
とする請求項1の気中微小粒子特性測定装置3. An apparatus for measuring characteristics of airborne microparticles according to claim 1, wherein the heating method by energizing the nichrome plate in claim 1 is a high frequency electromagnetic heating method in a box.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3086238A JPH0692929B2 (en) | 1991-03-26 | 1991-03-26 | Airborne microparticle characteristics measurement device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3086238A JPH0692929B2 (en) | 1991-03-26 | 1991-03-26 | Airborne microparticle characteristics measurement device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH05322739A JPH05322739A (en) | 1993-12-07 |
| JPH0692929B2 true JPH0692929B2 (en) | 1994-11-16 |
Family
ID=13881222
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3086238A Expired - Lifetime JPH0692929B2 (en) | 1991-03-26 | 1991-03-26 | Airborne microparticle characteristics measurement device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0692929B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3850403B2 (en) * | 2003-10-10 | 2006-11-29 | リオン株式会社 | Particle detector |
| DE10357611A1 (en) * | 2003-12-10 | 2005-07-07 | Robert Bosch Gmbh | Measurement of particles in engine exhaust gases comprises using heated oscillator, with heating unit mounted directly on oscillator component |
| US9027385B2 (en) | 2008-06-30 | 2015-05-12 | Saban Ventures Pty Limited | Aerosol sensor |
| US8274655B2 (en) | 2009-02-05 | 2012-09-25 | Massachusetts Institute Of Technology | Method and system for in situ aerosol thermo-radiometric analysis |
-
1991
- 1991-03-26 JP JP3086238A patent/JPH0692929B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH05322739A (en) | 1993-12-07 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |