JPS60187818A - Flow meter for powdery body - Google Patents
Flow meter for powdery bodyInfo
- Publication number
- JPS60187818A JPS60187818A JP59044475A JP4447584A JPS60187818A JP S60187818 A JPS60187818 A JP S60187818A JP 59044475 A JP59044475 A JP 59044475A JP 4447584 A JP4447584 A JP 4447584A JP S60187818 A JPS60187818 A JP S60187818A
- Authority
- JP
- Japan
- Prior art keywords
- powder
- waveguide
- tube
- microwave
- electric field
- 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N9/00—Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity
- G01N9/24—Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity by observing the transmission of wave or particle radiation through the material
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Measuring Volume Flow (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は、マイクロ波を使用して、第5〕炭等の粉体の
流量をリアルタイムで計測する粉体流量計に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a powder flow meter that measures the flow rate of powder such as No. 5 charcoal in real time using microwaves.
従来のマイクロ波を使用した粉体流量計は、第1図に示
すように、粉体を矢印A方向に搬送する金属製の搬送管
1の途中に、所定距離Bだけ&11シてドツプラー送受
信ユニット2と受信ユニット3を導波管4.5を介して
接続して構成している。As shown in Fig. 1, a conventional powder flow meter using microwaves has a Doppler transmitting/receiving unit placed in the middle of a metal conveying pipe 1 that conveys powder in the direction of arrow A by a predetermined distance B. 2 and a receiving unit 3 are connected via a waveguide 4.5.
この粉体流量針では、ドツプラー送受信ユニット2から
マイクロ波を搬送管1内に入射し、その搬送管l内を搬
送されている粉体により反射されてきた反射マイクロ波
をドツプラー送受信ユニット2で受信して、その反射マ
イクロ波と入射マイクロ波とをミキサーにて混合するこ
とより両マイクロ波の周波数差に応じた周波数のビート
、即ちドツプラー周波数を得て、これによりわ)体の搬
送速度の情報を得ている。In this powder flow needle, a Doppler transmitting/receiving unit 2 injects microwaves into the conveying tube 1, and the Doppler transmitting/receiving unit 2 receives the reflected microwaves reflected by the powder being conveyed in the conveying tube 1. Then, by mixing the reflected microwave and the incident microwave in a mixer, a beat of a frequency corresponding to the frequency difference between the two microwaves, that is, a Doppler frequency, is obtained, and from this, information about the transport speed of the body is obtained. I am getting .
また、ドツプラー送受信ユニット2からII!!送管1
内管1内されたマイクロ波の一部は、そのII送管1に
沿って伝搬して、途中で粉体の密度に応じて振幅が減少
(電力損失が発生する)し位相が変化して、受信ユニッ
ト3に到達するので、この受信ユニット3で得られるマ
イクロ波の位相或いは電力と、ドツプラー送受信ユニッ
ト2で送信されたマイクロ波の位相或いは電力とを比較
して、粉体の密度情報を得ている。In addition, Doppler transmitter/receiver unit 2 to II! ! Feed pipe 1
A part of the microwaves entering the inner tube 1 propagate along the II feed tube 1, and along the way, the amplitude decreases (power loss occurs) and the phase changes depending on the density of the powder. , the microwave reaches the receiving unit 3, and the phase or power of the microwave obtained by the receiving unit 3 is compared with the phase or power of the microwave transmitted by the Doppler transmitting/receiving unit 2 to obtain density information of the powder. It has gained.
そして、この密度情報と上記した搬送速度情報とから、
粉体の流量を計測している。Then, from this density information and the above-mentioned conveyance speed information,
Measuring the flow rate of powder.
ところで、上記したマイクロ波の位相の変化或いは電力
の損失は、搬送されている粉体との相互作用により生じ
るものであるが、搬送管1内のマイクロ波の電界分布は
、その搬送管1が丸管の場合には第2図((a)はT
Eu波)に示すように中心軸の電界が一番強く周辺部に
近づくほど弱くなっており(till送管1炉管1の場
合でも同じ。)、また粉体は搬送管1内に充満している
とは限らない。By the way, the above-mentioned change in the phase of the microwave or loss of power is caused by the interaction with the powder being transported, but the electric field distribution of the microwave inside the transport tube 1 is caused by the fact that the transport pipe 1 In the case of a round tube, see Figure 2 ((a) is T
As shown in (Eu wave), the electric field on the central axis is strongest and becomes weaker as it approaches the periphery (the same applies to the case of till feed tube 1 furnace tube 1), and the powder is filled in the conveyor tube 1. It doesn't necessarily mean that
従って、同一密度の粉体であっても、その粉体が搬送管
1内の断面部分のどの位置にあるかによって、得られる
密度情報に差が生し、その密度情報に誤差が生じ、ひい
ては流量計測に誤差が生じる。Therefore, even if the powder has the same density, there will be differences in the density information obtained depending on the position of the powder in the cross section in the conveying pipe 1, and errors will occur in the density information. Errors occur in flow measurement.
また、第1図に示す構成の粉体流量計では、マイクロ波
が必要な距111B内以外にも伝搬して受信ユニット3
に到達しないものが生じるので、これも密度情報の誤差
の原因となっている。Furthermore, in the powder flowmeter having the configuration shown in FIG.
This is also a cause of error in the density information, as there are some that do not reach .
本発明は斯かる点に鑑みて成されたもので、その目的は
、マイクロ波電界の強弱やマイクロ波の他への漏洩等に
よって密度情報に誤差が発生せず、よって高精度な流量
計測ができるようにした粉体流量針を提供することであ
る。The present invention has been made in view of the above points, and its purpose is to prevent errors in density information due to the strength of the microwave electric field or leakage of microwaves to other sources, and thereby enable highly accurate flow rate measurement. It is an object of the present invention to provide a powder flow needle that can perform powder flow.
以下、本発明の実施例について説明する。第3図はその
一実施例を示すものであり、6はマイクロ波損失の少な
い低損失誘電体で成る粉体搬送用の断面が丸形の搬送管
(低損失誘電体管)、7は断面が矩形で全体形状がほぼ
コ字形状に曲折した金属製の導波管であり、tU送前管
6その軸心が導波管7の中央部分7aの軸心と同軸とな
るように、その中央部分7aを貫通している。そして、
導波管7の曲折した一方の端部(粉体の搬送されてくる
側)にドツプラー送受信ユニット2が、また他方の@部
(粉体の搬送されて行く側)に受信ユニット3が各々取
り付けられている。8.9は搬送管6を導波管7内に固
定貫通するための金属製の丸形のガイド管である。Examples of the present invention will be described below. Fig. 3 shows an example of this, in which 6 is a conveyor tube (low-loss dielectric tube) with a round cross section for conveying powder made of a low-loss dielectric with little microwave loss, and 7 is a cross-section. is a metal waveguide whose overall shape is rectangular and bent into a substantially U-shape. It passes through the central portion 7a. and,
A Doppler transmitter/receiver unit 2 is attached to one bent end of the waveguide 7 (the side where the powder is conveyed), and a receiver unit 3 is attached to the other @ part (the side where the powder is conveyed). It is being Reference numeral 8.9 denotes a round metal guide tube for fixedly passing the carrier tube 6 into the waveguide 7.
以上において、導波管7におけるマイクロ波電界の分布
は、TE+o波では第4図に示すように、その中心部の
電界が強く、長手方向の両側が一番弱い。ところが、こ
の実施例では搬送管6を、導波管7の中央部7aに同軸
的に貫通させているので、その搬送管6は電界が強(そ
の大きさがほぼ同一の部分に位置することになる。従っ
て、搬送管6内の粉体には、その搬送管6内における断
面方向の位置の如何に拘らず、はぼ同一の電界が加わる
。In the above, the distribution of the microwave electric field in the waveguide 7 is such that for TE+o waves, the electric field is strong at the center and weakest at both sides in the longitudinal direction, as shown in FIG. However, in this embodiment, since the carrier tube 6 coaxially penetrates the central portion 7a of the waveguide 7, the carrier tube 6 has a strong electric field (the electric field is located in a portion where the magnitude is almost the same). Therefore, the same electric field is applied to the powder in the transport pipe 6 regardless of its position in the cross-sectional direction within the transport pipe 6.
一方、導波管にはその寸法に応じて、特定周波数以下の
マイクロ波は伝搬させないカットオフ周波数があり、例
えば長辺がaの矩形の導波管では、そのカットオフ周波
数のときの波長、つまりカットオフ波長λCはλc=2
aである。また、半径がrの丸形導波管ではλc=2π
r / k (k ハ使用する電磁界のモードによって
決まる定数。)である。従って、上記実施例では、使用
マイクロ波の周波数が予め決まっているときには、搬送
管6の外径を上記カットオフ波長となる寸法に設定する
ことにより、或いは搬送管6の径が予め決まっていると
きには、その搬送管6の外径で決まるカットオフ波長以
上の波長のマイロク波を使用することにより、その搬送
管6におけるガイド管8.9の取付部より外側の部分に
対しては、マイクロ波が漏洩することはなくなり、そこ
におけるマイクロ波損失をか無くなる。On the other hand, depending on the size of the waveguide, there is a cutoff frequency that prevents microwaves below a certain frequency from propagating.For example, in a rectangular waveguide with long sides a, the wavelength at that cutoff frequency, In other words, the cutoff wavelength λC is λc=2
It is a. In addition, for a round waveguide with radius r, λc=2π
r/k (k is a constant determined by the mode of the electromagnetic field used). Therefore, in the above embodiment, when the frequency of the microwave to be used is determined in advance, the outer diameter of the conveying tube 6 is set to a dimension that corresponds to the above-mentioned cutoff wavelength, or the diameter of the conveying tube 6 is determined in advance. Sometimes, by using microwaves with a wavelength longer than the cutoff wavelength determined by the outer diameter of the conveyor tube 6, microwaves can be applied to the portion of the conveyor tube 6 outside the attachment part of the guide tube 8.9. There will be no leakage, and the microwave loss there will be eliminated.
以上により、搬送管6内の粉体にはほぼ同一の電界が加
わり、またマイクロ波の外R1+への漏洩もなくなるの
で、ドツプラー送受信ユニット2がら受信ユニット3に
至るマイクロ波は、その位相や電力が搬送管6内の粉体
の密度によって連続的に変化する。なお、マイクロ波の
位相や電力は導波管7の曲折部分や搬送管6自体の影響
もうけるが、これらは定数として扱うことができるので
、そこで得られる密度信号或いは最終的に得られる流量
信号を補正することにより、正確な流量を計測すること
ができる。As a result of the above, almost the same electric field is applied to the powder in the conveying tube 6, and there is no leakage of microwaves to the outside R1+, so the microwaves that reach the receiving unit 3 from the Doppler transmitting/receiving unit 2 are controlled by their phase and power. changes continuously depending on the density of the powder in the conveying tube 6. Note that the phase and power of the microwave are affected by the bending part of the waveguide 7 and the carrier tube 6 itself, but these can be treated as constants, so the density signal or the final flow rate signal obtained therein can be treated as constants. By correcting, accurate flow rate can be measured.
第5図は別の実施例の構造を示すものであり、導波管7
′におけるドツプラー送受信ユニット2や受信ユニット
3に対する取り付は部分の曲折部分がほぼ90度となっ
ている以外は第3図に示したものと同一である。FIG. 5 shows the structure of another embodiment, in which the waveguide 7
The attachment to the Doppler transmitting/receiving unit 2 and the receiving unit 3 at ' is the same as that shown in FIG. 3 except that the bent portions of the parts are approximately 90 degrees.
なお、搬送管6はその少なくとも導波管7.7′を貫通
する部分が低損失誘電体で形成されていれば良く、他は
通常の搬送管と同様の金属であっても良い。また、導波
管7.7′は丸形であっても良く、更に搬送管6は矩形
であっても良い。Note that at least the portion of the transport tube 6 that passes through the waveguides 7 and 7' may be formed of a low-loss dielectric material, and the rest may be made of the same metal as a normal transport tube. Further, the waveguides 7, 7' may be round, and furthermore, the conveying pipe 6 may be rectangular.
以上から本発明によれば、ドツプラー送受信ユニットか
ら受信ユニットに至るマイクロ波の漏洩や不均一電界に
基づく密度情報の誤差の発生を防止することができ、精
度の向上した流Witを実現することができるという特
徴がある。As described above, according to the present invention, it is possible to prevent the leakage of microwaves from the Doppler transmitting/receiving unit to the receiving unit and the occurrence of errors in density information due to non-uniform electric fields, and it is possible to realize flow Wit with improved accuracy. It has the characteristic that it can be done.
第1図は従来の流量計の構造を示す断面図、第2図(旬
は従来のINN送向内電界モードを丞ず図、fblはそ
の電界の分布を示す特性図、第3図は本発明の一実施例
の流量針の構造を示す断面図、第4図(alば第3図に
おける導波管の中央部分の電界モードを示す断面図、(
blはその電界の分布を示す特性図、第5図は別の実施
例の流量計の構造を示す断面図である。
1・・・金属で成る搬送管、2・・・ドツプラー送受信
ユニット、3・・・受信ユニット、4.5・・・導波管
、6・・・搬送管(低損失誘電体管)、7.7′・・・
導波管、8.9・・・金属で成るガイド管。
特許出願人 新日本製鐵株式会社
同 新日本無線株式会社
代 理 人 弁理士 長尾常明
第3 図
第5図Figure 1 is a cross-sectional view showing the structure of a conventional flowmeter, Figure 2 is a diagram showing the electric field mode in the conventional INN feed direction, fbl is a characteristic diagram showing the distribution of the electric field, and Figure 3 is a diagram showing the current electric field mode. FIG. 4 is a sectional view showing the structure of a flow rate needle according to an embodiment of the invention;
bl is a characteristic diagram showing the distribution of the electric field, and FIG. 5 is a sectional view showing the structure of a flowmeter according to another embodiment. DESCRIPTION OF SYMBOLS 1... Conveyance tube made of metal, 2... Doppler transmission/reception unit, 3... Receiving unit, 4.5... Waveguide, 6... Conveyance tube (low loss dielectric tube), 7 .7'...
Waveguide, 8.9...A guide tube made of metal. Patent applicant Nippon Steel Corporation New Japan Radio Co., Ltd. Agent Patent attorney Tsuneaki Nagao Figure 3 Figure 5
Claims (1)
を入射して、その入射マイクロ波と上記粉体で反射した
反射マイクロ波とから得られるドツプラー周波数により
上記粉体の流速信号を得ると共に、上記入射マイクロ波
の上記粉体による損失酸゛ いは位相遅れにより上記粉
体の密度信号を得、該密度信号と上記流速信号とにより
上記わ〕体の流量を計測するようにした粉体流量計にお
いて、上記搬送管の少なくとも−g8を低損失誘電体管
にて形成し、はぼコ字形状に曲折した金属製の導波管の
中央部分に上記低損失誘電体管を同軸となるように貫通
させ、上記導波管の一端にドツプラー送受信ユニットを
接続すると共に、他端に受信ユニットを接続し、且つ上
記低損失誘電体管の径で決まるカットオフ周波数以下の
周波数のマイクロ波を使用して成る粉体流量針。(1j, Inject a microwave in the transport direction of the transport pipe that transports the powder, and obtain the flow velocity signal of the powder using the Doppler frequency obtained from the incident microwave and the reflected microwave reflected by the powder. In addition, a density signal of the powder is obtained by the loss of acid or phase delay of the incident microwave due to the powder, and the flow rate of the powder is measured based on the density signal and the flow velocity signal. In the mass flowmeter, at least -g8 of the conveying pipe is formed of a low-loss dielectric pipe, and the low-loss dielectric pipe is coaxially placed in the center of a metal waveguide bent in a box-shaped shape. A Doppler transmitting/receiving unit is connected to one end of the waveguide, and a receiving unit is connected to the other end of the waveguide. The powder flow consists of using a needle.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59044475A JPS60187818A (en) | 1984-03-08 | 1984-03-08 | Flow meter for powdery body |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59044475A JPS60187818A (en) | 1984-03-08 | 1984-03-08 | Flow meter for powdery body |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60187818A true JPS60187818A (en) | 1985-09-25 |
| JPH0510611B2 JPH0510611B2 (en) | 1993-02-10 |
Family
ID=12692547
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59044475A Granted JPS60187818A (en) | 1984-03-08 | 1984-03-08 | Flow meter for powdery body |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60187818A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102837837A (en) * | 2011-06-20 | 2012-12-26 | 罗伯特·博世有限公司 | Device and method used for proportioning powder product |
| CN113324603A (en) * | 2021-04-16 | 2021-08-31 | 浙江纺织服装职业技术学院 | Detection apparatus for nonmetal pipe flow through state |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4106075B2 (en) | 2006-11-02 | 2008-06-25 | オーム電機株式会社 | Flow measuring device |
-
1984
- 1984-03-08 JP JP59044475A patent/JPS60187818A/en active Granted
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102837837A (en) * | 2011-06-20 | 2012-12-26 | 罗伯特·博世有限公司 | Device and method used for proportioning powder product |
| CN113324603A (en) * | 2021-04-16 | 2021-08-31 | 浙江纺织服装职业技术学院 | Detection apparatus for nonmetal pipe flow through state |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0510611B2 (en) | 1993-02-10 |
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