JPS58218655A - Particle velocity measuring method - Google Patents
Particle velocity measuring methodInfo
- Publication number
- JPS58218655A JPS58218655A JP10173882A JP10173882A JPS58218655A JP S58218655 A JPS58218655 A JP S58218655A JP 10173882 A JP10173882 A JP 10173882A JP 10173882 A JP10173882 A JP 10173882A JP S58218655 A JPS58218655 A JP S58218655A
- Authority
- JP
- Japan
- Prior art keywords
- light
- particle
- velocity
- particle velocity
- red
- 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.)
- Pending
Links
- 239000002245 particle Substances 0.000 title claims abstract description 63
- 238000000034 method Methods 0.000 title claims description 5
- 239000013307 optical fiber Substances 0.000 claims abstract description 23
- 239000003086 colorant Substances 0.000 claims abstract description 11
- 238000005286 illumination Methods 0.000 claims description 10
- 238000000691 measurement method Methods 0.000 claims description 4
- 230000003287 optical effect Effects 0.000 claims 1
- 239000000203 mixture Substances 0.000 abstract description 2
- 239000000835 fiber Substances 0.000 abstract 1
- 239000007787 solid Substances 0.000 abstract 1
- 239000003245 coal Substances 0.000 description 6
- 238000007796 conventional method Methods 0.000 description 5
- 239000004568 cement Substances 0.000 description 4
- 238000011161 development Methods 0.000 description 2
- 238000002474 experimental method Methods 0.000 description 2
- 238000002309 gasification Methods 0.000 description 2
- 239000000523 sample Substances 0.000 description 2
- 235000008733 Citrus aurantifolia Nutrition 0.000 description 1
- 241000272201 Columbiformes Species 0.000 description 1
- 206010028813 Nausea Diseases 0.000 description 1
- 235000011941 Tilia x europaea Nutrition 0.000 description 1
- 239000011324 bead Substances 0.000 description 1
- 239000003034 coal gas Substances 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 239000008187 granular material Substances 0.000 description 1
- 239000004571 lime Substances 0.000 description 1
- 230000008693 nausea Effects 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 238000011160 research Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P5/00—Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft
- G01P5/18—Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft by measuring the time taken to traverse a fixed distance
- G01P5/20—Measuring speed of fluids, e.g. of air stream; Measuring speed of bodies relative to fluids, e.g. of ship, of aircraft by measuring the time taken to traverse a fixed distance using particles entrained by a fluid stream
Landscapes
- Engineering & Computer Science (AREA)
- Aviation & Aerospace Engineering (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Light Guides In General And Applications Therefor (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は例えば石炭ガス化炉1石炭ミル、セメントプラ
ント等1−おける固気混相流中の粒子速度を計11tu
する粒子速IW#1測法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a total of 11tu particle velocity in a solid-gas mixed phase flow in a coal gasification furnace, coal mill, cement plant, etc.
Regarding the particle velocity IW #1 measurement method.
石炭ガス化炉1石炭ミル、セメントプラント等Cおいて
11!・1気混和尚中の粒子速度を計測する場合、従
来で);J 弔1図(a) (b) l1示す方法(ユ
よって行TJつでいる◎同図において、oiは測定対象
の粒子ノロ′、02は光フアイバプローブ筒体で。Coal gasification furnace 1 Coal mill, cement plant, etc. C 11!・When measuring the particle velocity in a gas mixture, use the conventional method); Noro' and 02 are optical fiber probe cylinders.
後述の3本の光ファイバ中線03.94.05を同右す
る。03は照明用光ファイバで、後述のレーザ装置06
で発生されるレーザ光を上記粒子群O1へ照射1−るr
O4,05はそれぞれ。The same applies to the three optical fiber median lines 03.94.05, which will be described later. 03 is an optical fiber for illumination, and a laser device 06 (described later)
Irradiate the particle group O1 with a laser beam generated by
O4 and 05 respectively.
第1及び第2の受光用1光ファイバで、上記粒子群θ)
で反射されるtv受光して、それぞれgユ後述の第1及
び弔2の光−′嘔気変換器07゜08へ伝送T4)’口
06はレーザ装置でレーザ光を発生する。01.0Bは
それぞれ、第1及び第2の光−山気硬拗器で、上記第1
及び第2の受光用光ファイバ04 、 Ojが伝送する
粒子群01からの反射光な、その光の強さ51比例した
′重圧C−変池一「るo:40ニジて、その出力電圧信
号はそれぞれ後述の相互相関器09へ入力される◎09
は相互相関器で、上記第1及び第2の光−電気変換器0
7 、0 Bの出力電圧信号の相互相関係数を計算して
、その係数が最大となる時間遅延Φtp′を出力表示1
−る、
上記第1図(二おいて、レーザ装置06で発生されたレ
ーザ光を、照明用光ファイバ03で伝送させて測定対象
の粒子群IIに照射させる◎粒子群0II−照射された
レーザ光は粒子群O)で反射され、その反射光の一部分
は第1及び第2の受光用光ファイバDJ、D5の端面へ
入射し、それぞれ、第1及び第2の光−電気変換器oy
、osへ伝送される◎第1及び第2の光−電気便換50
7 、08に入射した光は、それぞれ、その入射光の強
さC二比例した電圧5二変換される。そして、その2つ
の電圧信号は、それぞれ、相互相関器09に入力される
。相互相関器09区−入力された第1及び第2の光−°
電気変換器07.0Bからの出力電圧信号を、それぞれ
。With one optical fiber for first and second light reception, the above particle group θ)
The TV beams reflected by the TV receivers are transmitted to the first and second beams, which will be described later, to the nausea converters 07 and 08, respectively. 01.0B are the first and second light-mountain devices, respectively;
And the reflected light from the particle group 01 transmitted by the second light-receiving optical fiber 04, Oj, whose output voltage signal is proportional to the intensity 51 of the light. are respectively input to the cross-correlator 09 described later◎09
is a cross-correlator, and the first and second optical-to-electrical converters 0
7. Calculate the cross-correlation coefficient of the output voltage signal of 0 B, and output the time delay Φtp' at which the coefficient is maximum.1
- In Figure 1 above (see Figure 2), the laser beam generated by the laser device 06 is transmitted through the illumination optical fiber 03 to irradiate the particle group II to be measured.◎Particle group 0II - irradiated laser beam The light is reflected by the particle group O), and a portion of the reflected light is incident on the end faces of the first and second light-receiving optical fibers DJ, D5, and the first and second optical-to-electrical converters oy, respectively.
◎First and second optical-electrical exchanges 50
7 and 08 are each converted into a voltage 52 proportional to the intensity C2 of the incident light. The two voltage signals are then input to the cross-correlator 09, respectively. Cross-correlator 09 section - input first and second light -°
The output voltage signal from electrical converter 07.0B, respectively.
x(t)、y(4)とおくと、相互相関器09は次式で
表わされる相互相関係数14 x y’(t’ ) l
jr:演算する。Letting x(t) and y(4), the cross-correlator 09 calculates the cross-correlation coefficient 14 x y'(t') l expressed by the following equation.
jr: Calculate.
友だし。We're friends.
ll
そして、七記相bl口1関係数Rxy(t’)が最大と
なる時間遅延量t′の個呻′を求めて出力表示する。こ
こで、上ft12 ’As l及び第2の受光用光ファ
イバo 4 、0 Bの間隔%j 1. I−すると、
所要の粒 1子群Oノの速1uvは。Then, the value of the time delay t' that maximizes the seven-phase-bl-port-1 relational coefficient Rxy(t') is determined and output and displayed. Here, the interval %j 1. I- Then,
The required particle speed of 1 particle group O is 1uv.
y=t/lp’ @−@(51
で求められる〇
上記第1肉に示した従来法は、比較的簡単(二粒子群の
速度を計測できるが1次の欠点なもっている。y=t/lp' @-@(51) The conventional method shown in the first part above is relatively simple (it can measure the velocity of two particle groups, but it has the drawback of first order).
石炭ガス化炉1石炭ミル及びセメントプラント等の性能
同上及び開発研究【二おける実験では。Coal gasifier 1 Performance of coal mills, cement plants, etc. and development research [2] In experiments.
粒子速度?粒子サイズ別に計測する必要があり、現像把
握上非常C二重要であるが、従来法では粒子径サイズ別
の速度を計測できない◎個別C二計測すると挙動が変る
。その為、上記粉粒体実験ではその挙動把握が十分2−
できない。Particle velocity? It is necessary to measure each particle size, which is very important for understanding development, but the conventional method cannot measure the speed for each particle size. ◎ If you measure C2 individually, the behavior will change. Therefore, in the above-mentioned powder and granule experiment, the behavior could be fully understood.
Can not.
本発明は上記の点C二龜みつなされたもので。The present invention combines two of the above points.
固気混相流の粒子屏C二照明用光ファイバで光を照射し
、その反射光をある一定距離隔った2点の位置で受光し
、その2点での光強度信号の相互相関係数が最大値とな
る時間遅延量t。?求めて、上記2点間の距離tより、
V ” L/ 165計算することC−より1粒子群
の速iV&求める粒子速度計測法において、測定対象の
粒子群を粒子経用に互いに異なる色≦−春色し、その複
数色の光を含む照明光で春色粒子群を照明して得られる
反射光な、ある一定距離隔てた2点の位置で受光し、そ
れぞれの反射光を分光して上記古色粒子の各々の色(二
対応した色の単色光の光強度(−号から樹色拉子別の1
0子速度すなわち粒径用の粒子速ハ1[を測定するよう
にしたことを要旨とし、固気混相流、中1−おける粒子
速度を粒子径別C二酊測し得る私”1子速+t Nt側
副法提供することな[1的とする。Solid-Gas Multiphase Flow Particle Screen C2 Light is irradiated with an illumination optical fiber, and the reflected light is received at two points separated by a certain distance, and the cross-correlation coefficient of the light intensity signal at those two points is calculated. The amount of time delay t at which the value becomes the maximum value. ? Find, from the distance t between the two points above,
V ” L / 165 Calculate the speed iV of one particle group from C- In the particle velocity measurement method, the particle group to be measured is colored differently from each other for particle diameter ≦ - spring color, and illumination containing light of multiple colors is used. The reflected light obtained by illuminating a group of spring-colored particles with light is received at two points separated by a certain distance, and each reflected light is divided into two colors (monochromatic colors of two corresponding colors) of the aged-colored particles. Light intensity of light (- from 1 to 1
The gist is that the particle velocity, that is, the particle velocity for particle size, is measured. +t Nt collateral method [1].
以下図1’1llvに照し′C本発明の一実施例を説明
スル・ff12図+Irいて、i−aは測定対象の第1
の粒子群で1例えば粒径5oμmのガラス玉に赤色の染
別布色を1llfi L、たものである◎i −bは測
定対象の第2のネO千群で1例えば粒径500戸 のガ
ラス玉6ユー肖色の染料春色を施したものである・2は
光フアイバプローブ筒体で、後述の3本の光フアイバ単
線3.4.5f固看する◎3は照明用光ファイバで、後
述の白色光源12で発生される白色光な上記114 +
及び第2の粒子群1−8+7−bへ1((1射する。4
.5は、第l及び第2の受光用光ファイバで、ある一定
の間隔tW隔てて粒子群J−a17−bに挿入されてい
る□そして、上記粒子群t−a、t−bで反射される光
を受光して、それぞれ、後述の第1及び第2のプリズム
6.7へ伝送する。6゜7は第1及び弔2のプリズムで
、上記第1及び第2の受光用光ファイバ4.5によねて
伝送された反射光をプリズムの分光機能により、赤色の
光6−a、7−aと汀色の光6−b、7−bを送別する
0そして、赤色の光6−a、7−aは、後述の第1及び
第2の光−電気変換器8゜9へ入射する。また、青色の
光6−b、7−bは、後述の第3及び第4の光−電気変
換器ノ0゜IIへ入射する。8,9は第1及び第2の光
−電気変換器で、それぞれ上占ピ第l及び第2のプリズ
ム6.2で分光された赤色光6−a+7−aの光強度C
二比例した″電圧を発生Tる。そして。An embodiment of the present invention will be explained below with reference to Figure 1'1llv.
For example, i-b is the second group of particles to be measured; Glass beads 6 are painted with spring-colored dye. 2 is the optical fiber probe barrel, and the 3 single optical fibers described later are 3.4.5 f. ◎ 3 is the optical fiber for illumination. The above-mentioned white light 114 + generated by a white light source 12 described below
and 1 ((1 shot. 4
.. Reference numeral 5 denotes the first and second light receiving optical fibers, which are inserted into the particle group J-a 17-b at a certain interval tW, and are reflected by the particle groups ta and tb. It receives the light and transmits it to first and second prisms 6.7, which will be described later. Reference numeral 6.7 denotes first and second prisms, which convert the reflected light transmitted by the first and second light-receiving optical fibers 4.5 into red lights 6-a and 7 using the spectroscopic function of the prisms. -a and the gray light 6-b, 7-b are sent off, and the red light 6-a, 7-a is incident on the first and second opto-electrical converters 8.9 described later do. Furthermore, the blue lights 6-b and 7-b enter third and fourth optical-to-electrical converters 0°II, which will be described later. 8 and 9 are first and second optical-to-electrical converters, and the light intensity C of the red light 6-a+7-a separated by the first and second prisms 6.2, respectively;
Generates two proportional voltages. And.
その出力電圧信号は、それぞれ後述の第1の相互相関器
13へ入力されるolO−11は第3及び第4の光−電
気変換器で、それぞれ、上記第1及び第2のプリズム6
.2で分光された青色光6−b、7−bの光強10’
in比例した電圧を発生する□そし、て、その出力電圧
信号は、それぞれイ%述の第2の相わ一相関器14へ入
力される◎12は白色九階で、白色光を発生し、上記照
明用光ファイバ3へ入射させる◎13は第1の相4相関
器で−−1: fr−! 鳩1と第2の光−電気変換器
8.9の出力電圧信号の相互相関係数を計算して、その
係数が最大となる時間遅延量t、’+を出力表示する◎
14は第2の相互相関器で、上記第3と小4の)し−′
山気変換器10.IIの出力電1ト伯袖のn+ t−を
相関係数1に#l゛算して、その係数が最大となる時間
;P4姐糟1,1を出力する。The output voltage signals are input to first cross-correlators 13, which will be described later. olO-11 are third and fourth optical-to-electrical converters, which are connected to the first and second prisms 6, respectively.
.. Light intensity 10' of blue light 6-b and 7-b separated by 2
□Then, the output voltage signals are respectively input to the second phase-correlator 14 described above. ◎12 is a white ninth order, which generates white light, ◎13, which is input to the illumination optical fiber 3, is the first phase 4 correlator -1: fr-! Calculate the cross-correlation coefficients of the output voltage signals of the pigeon 1 and the second opto-electrical converter 8.9, and output and display the time delay amount t,'+ at which the coefficient becomes the maximum◎
14 is the second cross-correlator, and
Yamaki converter 10. The output voltage of II is calculated by calculating the correlation coefficient 1 (n+t-) and outputs the time at which the coefficient becomes maximum; P4 1,1.
次C二−ヒ記妻施例の動作を説明する。第2図C二おい
て、白色光6+Ht zで発生した白色光?、照明用光
ファイバ3で伝送させて、測定対象の第1及び第2の粒
子−#Fj−a 、 t−bを同時に照射する。白色光
で照明された弔工の粒子群l−aは赤色≦−盲色されて
い心ので、赤色の光を他の色に比べて強く反射する◎そ
して、同様に。Next, the operation of the second embodiment will be explained. In Figure 2 C2, white light generated at 6+Htz? , and is transmitted through the illumination optical fiber 3 to simultaneously irradiate the first and second particles to be measured -#Fj-a and t-b. The particle group la of the funeral rite illuminated with white light is red ≦ - Since it is color blind, it reflects red light more strongly than other colors ◎ And similarly.
白色光で照明された第2の粒子群7−bは青色1−青色
されているので、青色の光を他の色≦1比べて強く反射
する。上記赤色及び青色を含む反射光は、第l及び第2
の受光用光ファイバ4゜5に入射して、第1及び第2の
プリズム6.7へ到達−[る。第1及び第2のプリズム
6.2はその入射光を分光して、それぞれ赤色光6−a
。The second particle group 7-b illuminated with white light is colored blue 1-blue, so it reflects blue light more strongly than other colors≦1. The reflected light including red and blue is the first and second reflected light.
The light enters the light-receiving optical fiber 4.5 and reaches the first and second prisms 6.7. The first and second prisms 6.2 split the incident light into red light 6-a, respectively.
.
2−a、及び青色光6−b、7−bC分離する。2-a, and blue light 6-b, 7-bC are separated.
そして、その赤色光6−a*7−aは第1及び第2の光
−爾′気変換器8.9へ送4mされ、また。The red light 6-a*7-a is then sent 4m to the first and second light-to-air converters 8.9.
青色光6−b、7−bは、第3及び第イの光−4気変換
器10 、77へ送信される。The blue lights 6-b and 7-b are transmitted to the third and the first light-to-four-air converters 10 and 77.
ところで、第1及び第2の光−電気変換器8゜9は、そ
れぞれ赤色光6−a、?−aの光強度1ユ比例した電圧
に変換し、その出力゛市圧他号は。By the way, the first and second optical-to-electrical converters 8.9 each emit red light 6-a, ? -A is converted into a voltage proportional to the light intensity 1 unit, and its output is ``city voltage''.
第]の相互相関器13へ入力される。第1の相互相関器
13は、上記二つの出力4圧4’t<号の相互相関係数
を演算して、相互相関係数が最大となる時間遅延量t、
’ Y求めて出力表示する◎相互相関係数のピーク値
を与える晴間遅延量t、1?求めれば、従来法と同じく
1次式C二て粒子速度V嘗が求められる。]th cross-correlator 13. The first cross-correlator 13 calculates the cross-correlation coefficient of the two output 4 pressures 4′t<, and calculates the time delay amount t at which the cross-correlation coefficient becomes maximum;
' Find Y and output and display ◎ Clearance delay amount t, 1 that gives the peak value of the cross-correlation coefficient? Once determined, the linear equation C2 and the particle velocity V can be determined as in the conventional method.
v、=t/l、’ e−・(6)ただし、tは1
f41及び飢2の受光用光ファイバ4.5の間隔である
◎−ト記vlは、赤色光を使って得らjまた79丁−速
1uであるので、赤色省色粒子すなわち第1の粒−fノ
lI:t −aの速度を与えている。v, = t/l,' e-・(6) However, t is 1
The spacing of the optical fibers 4.5 for receiving light at f41 and 2 is obtained using red light. -f no lI: gives a velocity of t-a.
次に、上記用3及びd64の光−゛電気変換器10*J
Iは、それぞれ、青色光6−b、7−bの光強tf1−
比例した嘔tl: l二変換し、その出力4う′圧伯綺
は、第2の相り、相関614へ入力される。@2の相互
相関614は、上記二つの出力゛婿圧伯吟の相性相関係
数ヶ演葬して、相互相関係数が最大となる時曲遅蛙瞳1
1.1求めて出力表示する。相互相関係数のピーク値を
与える時間遅延−1,′1求めれば、上記と同じく1次
式にて粒子畑IW’ V #が求められる。Next, the optical-to-electrical converter 10*J for the above 3 and d64
I is the light intensity tf1- of the blue lights 6-b and 7-b, respectively.
The proportional tl:l2 transform and its output 4'tl is input to the second ratio, correlation 614. The cross-correlation 614 of @2 is calculated by calculating the compatibility correlation coefficient of the above two outputs and calculating the time when the cross-correlation coefficient is maximum.
1.1 Find and display the output. By finding the time delay -1,'1 that gives the peak value of the cross-correlation coefficient, the particle field IW' V # can be found using the same linear equation as above.
V B =/、 / tH’ ”・・ (7)上
i前VBは、青色光な使って得られた粒子速度であるの
で、青色青色粒子すなわち第2の粒子群t−bの速度を
与えている。V B = /, / tH' ”... (7) Since VB before i above is the particle velocity obtained using blue light, give the velocity of the blue-blue particles, that is, the second particle group t-b. ing.
以上述べたよう1ユ本発明の方法によれば、測定対象の
粒子群を粒経用に複数個の異なる色で古色し、その着色
粒子群?白色光で照明して得られる複数の色を含む反射
光?、ある一足距除隔てた2点の位置で受光したあと、
プリズムで分光し、それぞれの色をもつ光の強度信号の
相互相関係数を求めるようじしたので、古色された粒子
の速度丁なわち1粒子径サイズ別の粒子速度を計測で弄
るようC二なった◎したがって。As described above, according to the method of the present invention, the particle group to be measured is aged with a plurality of different colors for grain size, and the colored particle group? Reflected light containing multiple colors obtained by illuminating with white light? , after receiving light at two points separated by a certain foot distance,
Since the cross-correlation coefficients of the intensity signals of the light of each color were calculated using a prism, the velocity of the aged particles, that is, the particle velocity of each particle size, was measured using C2. ◎Therefore.
従来法では計測できなかった石炭ガス他炉流動Im、石
灰ミル及びセメントプラント等の固気混相流の粒子ぜイ
ズ別粒子速度の計測が可能となIJ、固気混相流の境象
な適確に把握できるものであるーIJ, which is capable of measuring particle velocities by particle size in coal gas and other furnace flow Im, solid-gas mixed-phase flows such as lime mills and cement plants, which could not be measured with conventional methods, is an accurate method for solid-gas mixed-phase flows. It is something that can be grasped in
第1図(a)は従来の粒子速度計測法の#成を示T図、
第1因(blは第1図(a)のX−X線矢視因。
第2図は本発明の一実施例を示す構成囚である、1
7− a ・−m 1の粒子try、 7 ’−b−i
xg 2の粒子群、2・・・光ファイバ10一ブ筒体、
3・・・照明用光ファイバ、4.5・・・第1.第2の
受光用光ファイバ、6.7・・・ffz、第2のプリズ
ム、8゜y・441.m2の)し−山気z e器、10
.11・・・第3.弔4の光−市:気変換器、ノ2・・
・白色光源、7J・・・第lの相1−J二相関器、14
・・・第2の相互相関器。
出願人11代1111人 弁理士 鈴 圧式 彦2Figure 1 (a) shows the # configuration of the conventional particle velocity measurement method;
The first factor (bl is the X-X arrow line factor in FIG. 1(a). FIG. 2 is a particle try of 1 7- a ·-m 1, which is a constituent prisoner showing an example of the present invention. 7'-b-i
xg 2 particle groups, 2... optical fiber 10 tube body,
3... Optical fiber for illumination, 4.5... 1st. Second light-receiving optical fiber, 6.7...ffz, second prism, 8°y, 441. m2) shi-yamaki ze device, 10
.. 11...3rd. Light of Condolence 4 - City: Ki Converter, No 2...
・White light source, 7J...l-th phase 1-J bicorrelator, 14
...Second cross-correlator. 11 applicants 1111 people Patent attorney Rin Ushiki Hiko 2
Claims (1)
その反射光をある一定距離隔った2点の位置で受光し、
その2点での光強度信号の相互相関係数が最大値となる
時間遅延量t。を求めて、上記2点間の距離tより、v
=L/l。を計算すること1−より1粒子群の速度oi
求める粒子速度計側法Cおいて、測定対象の粒子群を粒
子径別(1互い(−異なる色に古色し、その複数色の光
を含む照明光で着色粒子群を照明して得られる反射光を
、ある一定距離隔てた2点の位置で受光し、それぞれの
反射光を分光して上記看色粒子の各々の色C対応した色
の単色光の光強i信号から粒径別の粒子速度を測定する
ようC二したことな特徴とする粒子速度計測法。Light is irradiated onto particles in a solid-gas multiphase flow using an optical fiber for illumination,
The reflected light is received at two points separated by a certain distance,
The time delay amount t at which the cross-correlation coefficient of the optical intensity signal at the two points reaches its maximum value. Then, from the distance t between the above two points, v
=L/l. Calculate the velocity of one particle group oi from 1-
In the particle velocimeter side method C, the particle group to be measured is separated by particle size (1 each other (-) and the reflection obtained by illuminating the colored particle group with illumination light that is aged to different colors and contains light of multiple colors. Light is received at two points separated by a certain distance, and the reflected light from each is divided into particles according to particle size based on the light intensity i signal of monochromatic light of the color corresponding to each color C of the color viewing particles. A particle velocity measurement method characterized by two unique features for measuring velocity.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10173882A JPS58218655A (en) | 1982-06-14 | 1982-06-14 | Particle velocity measuring method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10173882A JPS58218655A (en) | 1982-06-14 | 1982-06-14 | Particle velocity measuring method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS58218655A true JPS58218655A (en) | 1983-12-19 |
Family
ID=14308591
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10173882A Pending JPS58218655A (en) | 1982-06-14 | 1982-06-14 | Particle velocity measuring method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58218655A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6234531A (en) * | 1985-08-08 | 1987-02-14 | コーリン電子株式会社 | Method for measuring brain wave propagation speed |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5218081B2 (en) * | 1973-04-18 | 1977-05-19 | ||
| JPS578423A (en) * | 1980-06-19 | 1982-01-16 | Nec Corp | Method for inspecting printed matter |
-
1982
- 1982-06-14 JP JP10173882A patent/JPS58218655A/en active Pending
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5218081B2 (en) * | 1973-04-18 | 1977-05-19 | ||
| JPS578423A (en) * | 1980-06-19 | 1982-01-16 | Nec Corp | Method for inspecting printed matter |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6234531A (en) * | 1985-08-08 | 1987-02-14 | コーリン電子株式会社 | Method for measuring brain wave propagation speed |
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