JPS623729Y2 - - Google Patents

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Publication number
JPS623729Y2
JPS623729Y2 JP8632382U JP8632382U JPS623729Y2 JP S623729 Y2 JPS623729 Y2 JP S623729Y2 JP 8632382 U JP8632382 U JP 8632382U JP 8632382 U JP8632382 U JP 8632382U JP S623729 Y2 JPS623729 Y2 JP S623729Y2
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JP
Japan
Prior art keywords
light
optical fiber
optical fibers
diameter optical
differential amplifier
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Expired
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JP8632382U
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Japanese (ja)
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JPS58187768U (en
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Publication of JPS58187768U publication Critical patent/JPS58187768U/en
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  • Length Measuring Devices By Optical Means (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Description

【考案の詳細な説明】 本考案は例えば石炭ガス化炉、石炭ミル、セメ
ントプラント等において、固気混相流中の粒子速
度を計測する粒子速度計測装置に関する。
[Detailed Description of the Invention] The present invention relates to a particle velocity measuring device for measuring particle velocity in a solid-gas mixed phase flow in, for example, a coal gasifier, a coal mill, a cement plant, etc.

この種従来における粒子速度計測装置は、第1
図a,bに示すように構成されている。第1図
a,bにおいて、01は、測定対象の粒子群、0
2は光フアイバプローブで、後述の照明用光フア
イバ及び受光用光フアイバを固着している。0
3,04,05,06,07,08,09,01
0は、第1,第2,第3,第4,第5,第6,第
7及び第8の照明用光フアイバで、後述のレーザ
装置からレーザ光を受けて、粉粒体を照明する。
011,012,013,014,015,01
6,017,018は、第1,第2,第3,第
4,第5,第6,第7及び第8の受光用光フアイ
バで、粉粒体からの反射光を受光して、後述の受
光素子へ伝送する。019はレーザ装置でレーザ
光を発生する。020,021は第1及び第2の
受光素子で、反射光の強度に比例した電圧を発生
し、その出力電圧を後述の差動増幅器に入力す
る。022は差動増幅器で、2つの入力電圧信号
の差に比例した電圧を発生する。そして、その出
力電圧は後述の周波数分析器に入力される。02
3は周波数分析器で入力された電圧信号の周波数
スペクトラムを解析処理して、その結果を出力す
る。
This type of conventional particle velocity measuring device has a first
It is constructed as shown in Figures a and b. In Figures 1a and b, 01 is the particle group to be measured, 0
Reference numeral 2 denotes an optical fiber probe to which an illumination optical fiber and a light receiving optical fiber, which will be described later, are fixed. 0
3,04,05,06,07,08,09,01
0 are first, second, third, fourth, fifth, sixth, seventh, and eighth illumination optical fibers that receive laser light from a laser device to be described later to illuminate the granular material. .
011,012,013,014,015,01
6,017,018 are first, second, third, fourth, fifth, sixth, seventh and eighth optical fibers for receiving light, which receive reflected light from powder and granular material, and The light is transmitted to the light receiving element. A laser device 019 generates laser light. Reference numerals 020 and 021 denote first and second light receiving elements, which generate voltages proportional to the intensity of reflected light, and input the output voltages to a differential amplifier to be described later. 022 is a differential amplifier that generates a voltage proportional to the difference between two input voltage signals. The output voltage is then input to a frequency analyzer, which will be described later. 02
3 analyzes the frequency spectrum of the input voltage signal using a frequency analyzer and outputs the result.

上記第1図において、レーザ装置019で発生
されたレーザ光を照明用光フアイバ群03,0
4,05,06,07,08,09及び010で
伝送させて、測定対象の粉粒体01に照射させ
る。粉粒体からの反射光の一部分は、第1,第
2,第3,第4,第5,第6,第7,及び第8の
受光用光フアイバ011,012,013,01
4,015,016,017,及び018に入射
する。そして、第1,第3,第5,及び第7の受
光用光フアイバ011,013,015,017
を伝送された反射光は第1の受光素子020に入
射する。また、第2,第4,第6及び第8の受光
用光フアイバ012,014,016及び018
を伝送された反射光は、第2の受光素子021に
入射する。
In the above FIG.
4, 05, 06, 07, 08, 09, and 010 to irradiate the granular material 01 to be measured. A portion of the reflected light from the granular material is transmitted to the first, second, third, fourth, fifth, sixth, seventh, and eighth light-receiving optical fibers 011, 012, 013, 01.
4,015,016,017, and 018. The first, third, fifth, and seventh light receiving optical fibers 011, 013, 015, 017
The reflected light that has been transmitted is incident on the first light receiving element 020. In addition, second, fourth, sixth and eighth light receiving optical fibers 012, 014, 016 and 018
The reflected light that has been transmitted is incident on the second light receiving element 021.

上記第1及び第2の受光素子020,021に
入射した反射光はその光の強さに比例した電圧信
号となつて、差動増幅器022に入力される。上
記差動増幅器022は、2つの入力電圧信号すな
わち、第1の受光素子020の出力電圧x1(t)
と第2の受光素子021の出力電圧x2(t)の差
〔x1(t)−x2(t)〕に比例した電圧x(t)を
発生し、周波数分析器023に入力する。上記周
波数分析器023はその入力信号x(t)の周波
数スペクトラムを解析してその結果を出力する。
その出力結果より、卓越したピークの周波数p
が判る。
The reflected light incident on the first and second light receiving elements 020 and 021 becomes a voltage signal proportional to the intensity of the light, and is input to the differential amplifier 022. The differential amplifier 022 receives two input voltage signals, that is, the output voltage x 1 (t) of the first light receiving element 020.
A voltage x(t) proportional to the difference [x 1 (t) - x 2 (t)] between the output voltage x 2 (t) of the second light receiving element 021 and the output voltage x 2 (t) of the second light receiving element 021 is generated and input to the frequency analyzer 023 . The frequency analyzer 023 analyzes the frequency spectrum of its input signal x(t) and outputs the result.
From the output results, the outstanding peak frequency p
I understand.

ところで、上記周波数pが求められると上記
受光用光フアイバ群011,012,013,0
14,015,016,017,018の間隔d
との関係より、所要の粉粒体の速度νは ν=2dp ……(1) で求められる。
By the way, when the frequency p is determined, the light receiving optical fiber group 011, 012, 013, 0
Interval d of 14,015,016,017,018
From the relationship between

上記従来の粒子速度計測装置は粒子速度を比較
的簡単に測定できるが、以下に述べる欠点をもつ
ている。
Although the conventional particle velocity measuring device described above can measure particle velocity relatively easily, it has the following drawbacks.

第2図は第1図の従来装置で用いられている光
フアイバプローブの基本構造を示している。同図
において、照明用光フアイバ03から出射するレ
ーザ光は、実線矢印で示している領域を照射す
る。そして、その反射光を受光する受光用光フア
イバ011が受光する領域は、点線矢印で示して
いる部分である。したがつて、同図の斜線部02
4には粉粒体が存在するが、その部分以外には存
在しないという条件下では、測定対象の粉粒体は
照明用光フアイバ03で照明され、そして、その
反射光は受光用光フアイバ011で受光されるの
で不都合はない。
FIG. 2 shows the basic structure of the optical fiber probe used in the conventional device shown in FIG. In the figure, the laser light emitted from the illumination optical fiber 03 irradiates the area indicated by the solid arrow. The area where the light-receiving optical fiber 011 receives the reflected light is the area indicated by the dotted arrow. Therefore, the shaded area 02 in the same figure
4, but under the condition that the powder or granule is not present in other parts, the powder or granule to be measured is illuminated by the illumination optical fiber 03, and the reflected light is transmitted to the light receiving optical fiber 011. There is no problem because the light is received by the

しかしながら、上記斜線部024以外にも高濃
度の粉粒体が存在する場合には、照明用光フアイ
バ03からのレーザ光がしやへいされ、また、受
光用光フアイバ011に入射すべき反射光がしや
へいされて、所要の粉粒体速度信号が得られな
い。
However, if there is a high concentration of powder other than the shaded area 024, the laser light from the illumination optical fiber 03 will be suppressed, and the reflected light that should be incident on the light receiving optical fiber 011 will be suppressed. The required powder velocity signal cannot be obtained because of the powder and granule material being washed away.

それ故、従来装置では、石炭ガス化炉、石炭ミ
ル及びセメントプラント等の性能向上及び開発研
究実験における高濃度粉粒体の速度計測には適用
できないという欠点がある。
Therefore, the conventional device has the disadvantage that it cannot be applied to speed measurement of highly concentrated powder and granular materials in performance improvement and development research experiments of coal gasifiers, coal mills, cement plants, etc.

本考案は上記の点に鑑みてなされたもので、固
気混相流の粒子群中に等間隔を有して先端を夫々
挿入される少なくとも3本以上の大径光フアイバ
と、同大径光フアイバの後端に夫々接続される2
本一組の小径光フアイバと、同小径光フアイバの
一方より光を照射する手段と、上記小径光フアイ
バの他方に入つた光を受光しその強度を検出する
受光素子と、上記等間隔に並べられた大径光フア
イバの順に交互に極性を変換して差を取る差動増
幅器と、同差動増幅器で得られた周波数スペクト
ラムを解析処理する周波数分析器と、同分析器で
得られた周波数のピーク値と上記大径光フアイバ
の間隔とから粒子の速度を求めるようにしたこと
を要旨とし、高濃度粉粒体においても粒子の速度
を確実に計測し得る粒子速度計測装置を提供する
ことを目的とする。
The present invention has been made in view of the above points, and includes at least three large-diameter optical fibers whose tips are inserted at equal intervals into a group of particles in a solid-gas multiphase flow, and the same large-diameter optical fibers. 2 connected to the rear end of the fiber respectively
A set of small-diameter optical fibers, a means for emitting light from one side of the small-diameter optical fibers, and a light-receiving element for receiving the light entering the other side of the small-diameter optical fibers and detecting its intensity, arranged at equal intervals as described above. A differential amplifier that alternately converts the polarity of the large-diameter optical fibers and calculates the difference, a frequency analyzer that analyzes and processes the frequency spectrum obtained by the differential amplifier, and a frequency analyzer that analyzes the frequency spectrum obtained by the differential amplifier. The object of the present invention is to provide a particle velocity measuring device that can reliably measure the velocity of particles even in highly concentrated powder and granular materials, by determining the velocity of particles from the peak value of and the distance between the large-diameter optical fibers. With the goal.

以下図面を参照して本考案の一実施例を説明す
る。第3図a,bにおいて、1は測定対象の粉粒
体、2は光フアイバプローブで、後述の第1,第
2,第3,第4,第5,第6,第7及び第8の光
フアイバ単線を固着している。3,4,5,6,
7,8,9,10は、第1,第2,第3,第4,
第5,第6,第7及び第8の光フアイバ単線で、
その両端面の一方は上記粉粒体1に挿入され、他
方の端面はそれぞれ、後述第9と第10、第11と第
12、第13と第14、第15と第16、第17と第18、第19
と第20、第21と第22及び第23と第24の光フアイバ
単線に連結されている。そして、粉粒体に挿入さ
れた部分ではある一定の間隔d′で上記光フアイバ
プローブに固着されている。11,13,15,
17,19,21,23,25は、第9,第11,
第13,第15,第17,第19,第21及び第23の光フア
イバ単線で、その両端面の一方は、それぞれ、上
記第1,第2,第3,第4,第5,第6,第7及
び第8の光フアイバ単線に連結されている。ま
た、他方の端面は、第9,第13,第17及び第21の
光フアイバ単線については後述の第1の受光素子
に連結され、第11,第15,第19及び第23の光フア
イバ単線については、後述の第2の受光素子に連
結されている。12,14,16,18,20,
22,24,26は、第10,第12,第14,第16,
第18,第20,第22及び第24の光フアイバ単線で、
その両端面の一方は、それぞれ、上記第1,第
2,第3,第4,第5,第6,第7及び第8の光
フアイバ単線に連結され、他方の端面は後述のレ
ーザ装置に連結されている。27はレーザ装置で
レーザ光を発生する。28,29は、第1及び第
2の受光素子で、それぞれ入射光の強さに比例し
た電圧を発生し、その出力信号を後述の差動増幅
器へ送信する。30は差動増幅器で、2つの入力
電圧信号の差に比例した電圧を発生する。そし
て、その出力電圧信号は後述の周波数分析器に入
力される。31は周波数分析器で、入力された電
圧信号の周波数スペクトラムを解析処理して、そ
の結果を出力する。
An embodiment of the present invention will be described below with reference to the drawings. In FIGS. 3a and 3b, 1 is the granular material to be measured, 2 is an optical fiber probe, and the 1st, 2nd, 3rd, 4th, 5th, 6th, 7th, and 8th A single optical fiber is fixed. 3, 4, 5, 6,
7, 8, 9, 10 are the first, second, third, fourth,
With the fifth, sixth, seventh and eighth single optical fibers,
One of its both end faces is inserted into the powder 1, and the other end face is inserted into the 9th and 10th, and 11th and 11th, which will be described later.
12th, 13th and 14th, 15th and 16th, 17th and 18th, 19th
and 20th, 21st and 22nd, and 23rd and 24th single optical fibers. The part inserted into the powder is fixed to the optical fiber probe at a certain interval d'. 11, 13, 15,
17, 19, 21, 23, 25 are the 9th, 11th,
13th, 15th, 17th, 19th, 21st, and 23rd single optical fibers, one of the end surfaces of which are connected to the first, second, third, fourth, fifth, and sixth single fibers, respectively. , seventh and eighth single optical fibers. Further, the other end face is connected to a first light-receiving element described later for the 9th, 13th, 17th, and 21st single optical fibers, and the 11th, 15th, 19th, and 23rd single optical fibers are connected to a first light receiving element described later. is connected to a second light-receiving element, which will be described later. 12, 14, 16, 18, 20,
22, 24, 26 are the 10th, 12th, 14th, 16th,
18th, 20th, 22nd and 24th single optical fiber,
One of the end faces is connected to the first, second, third, fourth, fifth, sixth, seventh and eighth single optical fibers, respectively, and the other end face is connected to the laser device described below. connected. A laser device 27 generates a laser beam. Reference numerals 28 and 29 denote first and second light-receiving elements, each of which generates a voltage proportional to the intensity of incident light, and transmits the output signal to a differential amplifier to be described later. 30 is a differential amplifier that generates a voltage proportional to the difference between two input voltage signals. The output voltage signal is then input to a frequency analyzer, which will be described later. A frequency analyzer 31 analyzes the frequency spectrum of the input voltage signal and outputs the result.

次に上記実施例の動作について説明する。 Next, the operation of the above embodiment will be explained.

第3図a,bにおいて、レーザ装置27で発生
されたレーザ光を第10,第12,第14,第16,第
18,第20,第22及び第24の光フアイバ単線12,
14,16,18,20,22,24,26でそ
れぞれ、第1,第2,第3,第4,第5,第6,
第7及び第8の光フアイバ単線3,4,5,6,
7,8,9,10へ伝送する。上記第1,第2,
第3,第4,第5,第6,第7及び第8の光フア
イバ単線は、それぞれ、上記レーザ光を計測対象
の粉粒体1へ照射する。粉粒体1で反射された光
は、再び、第1,第2,第3,第4,第5,第
6,第7及び第8の光フアイバ単線へそれぞれ、
入射し第9,第11,第13,第15,第17,第19,第
21及び第23の光フアイバ単線11,13,15,
17,19,21,23,25へ伝送される。
In FIGS. 3a and 3b, the laser beams generated by the laser device 27 are
18, 20th, 22nd and 24th single optical fiber 12,
14, 16, 18, 20, 22, 24, 26, respectively, the first, second, third, fourth, fifth, sixth,
seventh and eighth single optical fibers 3, 4, 5, 6,
Transmit to 7, 8, 9, 10. Above 1st, 2nd,
The third, fourth, fifth, sixth, seventh, and eighth single optical fibers each irradiate the above-mentioned laser light onto the powder 1 to be measured. The light reflected by the granular material 1 is again transmitted to the first, second, third, fourth, fifth, sixth, seventh and eighth single optical fibers, respectively.
9th, 11th, 13th, 15th, 17th, 19th,
21 and 23rd single optical fiber 11, 13, 15,
It is transmitted to 17, 19, 21, 23, and 25.

上記第9,第13,第17及び第21の光フアイバ単
線11,15,19,23を伝送された上記反射
光は、第1の受光素子28へ入射し、その入射光
の強さに比例した電圧信号x1(t)に変換され
て、差動増幅器30の二つの入力部の一つに入力
される。上記第11,第15,第19及び第23の光フア
イバ単線13,17,21,25を伝送された上
記反射光は、第2の受光素子29へ入射し、その
入射光の強さに比例した電圧信号x2(t)に変換
されて、上記差動増幅器30の他方の入力部に入
力される。
The reflected light transmitted through the 9th, 13th, 17th, and 21st optical fiber single wires 11, 15, 19, and 23 enters the first light receiving element 28, and is proportional to the intensity of the incident light. The voltage signal x 1 (t) is then input to one of the two input sections of the differential amplifier 30 . The reflected light transmitted through the 11th, 15th, 19th, and 23rd optical fiber single wires 13, 17, 21, and 25 enters the second light receiving element 29, and is proportional to the intensity of the incident light. It is converted into a voltage signal x 2 (t) and input to the other input section of the differential amplifier 30.

上記差動増幅器30はそれに入力された上記二
つの電圧信号x1(t)及びx2(t)の差〔x1
(t)−x2(t)〕に比例した電圧信号x(t)を
発生し、その信号を周波数分析器31に入力す
る。上記周波数分析器31は、その入力信号x
(t)の周波数スペクトラムを解析処理して、そ
の結果を出力する。その出力結果より、卓越した
ピークの周波数′pが判る。この′pが求められ
ると、従来法と同様にして、粉粒体の速度ν′が ν′=2d′′p として求められる。ただし、d′は上記第1,第
2,第3,第4,第5,第6,第7及び第8の光
フアイバ間隔である。
The differential amplifier 30 calculates the difference [x 1
(t)−x 2 (t)] and inputs the signal to the frequency analyzer 31. The frequency analyzer 31 receives its input signal x
The frequency spectrum of (t) is analyzed and the result is output. From the output result, the prominent peak frequency ′ p can be found. Once this ′ p is determined, the velocity ν′ of the powder is determined as ν′=2d′′ p in the same manner as in the conventional method. However, d' is the distance between the first, second, third, fourth, fifth, sixth, seventh, and eighth optical fibers.

ところで、以上述べた本考案によれば、粉粒体
に挿入された第1,第2,第3,第4,第5,第
6,第7及び第8の光フアイバ単線が、第4図に
示しているように、照明光Aの出射と反射光Bの
受光を一つの光フアイバ単線の端面で行なうこと
から、照明光あるいは反射光を粉粒体でしやへい
されることが全くない。したがつて、粉粒体の濃
度によらず、高濃度の場合についても適用がで
き、従来では測定できなかつた石炭ガス化炉流動
層、石炭ミル微分炭輸送管等の粒子速度計測が可
能となり、本考案装置の産業上の価値は著しく大
きいものがある。
By the way, according to the present invention described above, the first, second, third, fourth, fifth, sixth, seventh and eighth single optical fibers inserted into the powder material are as shown in FIG. As shown in Figure 2, since the emission of illumination light A and the reception of reflected light B are performed on the end face of a single optical fiber, there is no possibility that the illumination light or reflected light is suppressed by powder or granules. . Therefore, it can be applied to high concentrations regardless of the concentration of powder and granules, and it is now possible to measure particle velocity in fluidized beds in coal gasifiers, differential coal transport pipes in coal mills, etc., which were previously impossible to measure. , the industrial value of the device of the present invention is extremely large.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図aは従来の粒子速度計測装置の構成を示
す図、第1図bは第1図aのX−X線矢視図、第
2図は第1図における光フアイバプローブの基本
構造を示す図、第3図aは本考案の一実施例を示
す構成図、第3図bは第3図aのX−X線矢視
図、第4図は第3図における光フアイバ単線部分
を示す図である。 1……粉粒体、2……光フアイバプローブ、3
〜10……第1〜第8の光フアイバ単線、11〜
26……第9〜第24の光フアイバ単線、27……
レーザ装置、28,29……第1,第2の受光素
子、30……差動増幅器、31……周波数分析
器。
Figure 1a is a diagram showing the configuration of a conventional particle velocity measuring device, Figure 1b is a view taken along the line X-X in Figure 1a, and Figure 2 shows the basic structure of the optical fiber probe in Figure 1. Figure 3a is a configuration diagram showing an embodiment of the present invention, Figure 3b is a view taken along the line X--X in Figure 3a, and Figure 4 shows the single optical fiber portion in Figure 3. FIG. 1... Powder, 2... Optical fiber probe, 3
~10...first to eighth single optical fibers, 11~
26... 9th to 24th single optical fiber, 27...
Laser device, 28, 29...first and second light receiving elements, 30...differential amplifier, 31...frequency analyzer.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 固気混相流の粒子群中に等間隔を有して先端を
夫々挿入される少なくとも3本以上の大径光フア
イバと、同大径光フアイバの後端に夫々接続され
る2本一組の小径光フアイバと、同小径光フアイ
バの一方より光を照射する手段と、上記小径光フ
アイバの他方に入つた光を受光しその強度を検出
する受光素子と、上記等間隔に並べられた大径光
フアイバの順に交互に極性を変換して差を取る差
動増幅器と、同差動増幅器で得られた周波数スペ
クトラムを解析処理する周波数分析器と、同分析
器で得られた周波数のピーク値と上記大径光フア
イバの間隔とから粒子の速度を求めるようにした
ことを特徴とする粒子速度計測装置。
At least three or more large-diameter optical fibers whose tips are inserted at equal intervals into the particle group of the solid-gas multiphase flow, and a set of two large-diameter optical fibers whose tips are respectively connected to the rear ends of the same large-diameter optical fibers. a small-diameter optical fiber, a means for irradiating light from one side of the small-diameter optical fiber, a light-receiving element that receives the light entering the other side of the small-diameter optical fiber and detects its intensity, and a large-diameter arranged at equal intervals. A differential amplifier that takes the difference by alternately converting the polarity of the optical fiber, a frequency analyzer that analyzes the frequency spectrum obtained by the differential amplifier, and a frequency peak value obtained by the analyzer. A particle velocity measuring device characterized in that the particle velocity is determined from the interval between the large-diameter optical fibers.
JP8632382U 1982-06-10 1982-06-10 Particle velocity measuring device Granted JPS58187768U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8632382U JPS58187768U (en) 1982-06-10 1982-06-10 Particle velocity measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8632382U JPS58187768U (en) 1982-06-10 1982-06-10 Particle velocity measuring device

Publications (2)

Publication Number Publication Date
JPS58187768U JPS58187768U (en) 1983-12-13
JPS623729Y2 true JPS623729Y2 (en) 1987-01-28

Family

ID=30095142

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8632382U Granted JPS58187768U (en) 1982-06-10 1982-06-10 Particle velocity measuring device

Country Status (1)

Country Link
JP (1) JPS58187768U (en)

Also Published As

Publication number Publication date
JPS58187768U (en) 1983-12-13

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