JPH0543973B2 - - Google Patents
Info
- Publication number
- JPH0543973B2 JPH0543973B2 JP22283687A JP22283687A JPH0543973B2 JP H0543973 B2 JPH0543973 B2 JP H0543973B2 JP 22283687 A JP22283687 A JP 22283687A JP 22283687 A JP22283687 A JP 22283687A JP H0543973 B2 JPH0543973 B2 JP H0543973B2
- Authority
- JP
- Japan
- Prior art keywords
- wave
- microwave
- antenna
- measurement surface
- polarization
- 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 - Fee Related
Links
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- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
- Radar Systems Or Details Thereof (AREA)
Description
【発明の詳細な説明】
(産業状の利用分野)
連炉や鋳造機内の高温溶融金属や、高炉内原料
など粉粒体を対象としたレベル測定装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION (Industrial field of application) The present invention relates to a level measuring device for high-temperature molten metal in continuous furnaces and casting machines, and powder and granular materials such as raw materials in blast furnaces.
(従来の技術)
高温、多粉塵の悪環境下において溶融金属や粉
粒状の原料レベルを高精度で測定する方法とし
て、マイクロ波を用いたFM(周波数変調)レー
ダが適している。しかしこれら物質のマイクロ波
反射率は低いので、アンテナの不整合に起因する
反射波や対象物体を保持している容器からの反射
波の影響が避け難く、大きな誤差要因となる。(Prior Technology) FM (frequency modulation) radar using microwaves is suitable as a method for measuring the level of molten metal and powdery raw materials with high precision in harsh environments with high temperatures and large amounts of dust. However, since the microwave reflectance of these materials is low, it is difficult to avoid the influence of reflected waves due to antenna mismatching and reflected waves from the container holding the target object, which becomes a major error factor.
送信波と反射波とを混合検波して得られるビー
ト波より、上記不要反射を除去する方法として
は、フイルタを用いて周波数帯域で弁別する方法
が一般的である。しかし、信号波と不要反射波に
よりビート波の周波数は近接している場合が多
く、実用精度を達成するために十分な程度まで不
要反射を除去することは困難である。 A common method for removing unnecessary reflections from a beat wave obtained by mixed detection of a transmitted wave and a reflected wave is to use a filter to discriminate based on frequency bands. However, the frequency of the beat wave due to the signal wave and the unnecessary reflected wave is often close to each other, and it is difficult to remove the unnecessary reflection to a sufficient degree to achieve practical accuracy.
そこで、従来のレベル測定装置には、第7図に
示すようにまずマイクロ波1を吸収又は反射する
遮蔽板2を測定面である液面3上に設置し、液面
3からの反射波がアンテナ4に入射しないように
して、液面3以外から反射してくる不要反射のみ
に起因するビート信号を予め記録しておく。そし
て、液面3の測定時には、液面3からの反射波と
不要反射の両者によつて生じるビート信号から、
上記記録信号を、マイクロ波の変調周期に同期さ
せながら減算することにより、液面3のみからの
反射波に起因するビート信号を抽出したのち、従
来のFMレーダの信号処理方法に基づいてレベル
を算出するようにしたものがある(例えば特開昭
55−82926)。 Therefore, in the conventional level measuring device, as shown in FIG. Beat signals caused only by unnecessary reflections reflected from other than the liquid surface 3 are recorded in advance so that they do not enter the antenna 4. When measuring the liquid level 3, from the beat signal generated by both the reflected waves from the liquid level 3 and unnecessary reflections,
By subtracting the recorded signal while synchronizing with the modulation period of the microwave, the beat signal caused by the reflected wave only from the liquid surface 3 is extracted, and then the level is determined based on the conventional FM radar signal processing method. There are some methods that calculate it (for example, JP-A-Sho
55−82926).
(発明が解決しようとする問題点)
上記のような、従来装置は、測定開始前に記録
した不要反射波によるビート波(以下ノイズ成分
と呼ぶ)が液面3測定中も変化しない場合にのみ
適用できる。しかし、実際のレーダにおいては、
発振器の周波数ドリフトによりノイズ波形が変化
する上に、特に溶融金属などを対象とする場合に
は、容器壁などに金属が付着することがあるし、
アンテナ4前面にダストなどが付着することがあ
り、このためノイズ波形は時々刻々変化し、従つ
て従来のものでは正確な測定面の位置測定は困難
であつた。(Problems to be Solved by the Invention) The conventional device as described above only detects noise when the beat waves (hereinafter referred to as noise components) caused by unnecessary reflected waves recorded before the start of measurement do not change during the measurement of the liquid level 3. Applicable. However, in actual radar,
Not only does the noise waveform change due to the frequency drift of the oscillator, but especially when the target is molten metal, metal may adhere to the container wall, etc.
Dust and the like may adhere to the front surface of the antenna 4, causing the noise waveform to change from moment to moment, making it difficult to accurately measure the position of the measurement surface with conventional devices.
本発明は上記問題点に鑑み、ノイズ波形が時々
刻々変化する場合でも測定面のレベルを正確に測
定し得るようにしたものである。 In view of the above-mentioned problems, the present invention is designed to accurately measure the level on a measurement surface even when the noise waveform changes from moment to moment.
(問題点を解決するための手段)
この技術的課題を解決する本発明の技術的手段
は、マイクロ波12の送信波12aと測定面16
からの反射波12bとをミキシングしてビート信
号21をつくり、該ビート信号21から測定面1
6の位置を算出するようにしたレベル測定装置に
おいて、
偏波面を有するマイクロ波12を測定面16に
向けて送信する送信用アンテナ14を設けると共
に、測定面16での乱反射により送信波12aの
偏波面が回転するように、送信波12aの波長を
測定面の凹凸径以下に選定し、測定面16での乱
反射によつて回転した偏波面を有するマイクロ波
12bのみを受信する受信用アンテナ18を設
け、該受信用アンテナ18で受信したマイクロ波
12bと前記送信波12aとをミキシングするよ
うにした点にある。(Means for Solving the Problem) The technical means of the present invention for solving this technical problem is that the transmission wave 12a of the microwave 12 and the measurement surface 16 are
A beat signal 21 is created by mixing the reflected wave 12b from the measurement surface 1.
In the level measuring device configured to calculate the position of 6, a transmitting antenna 14 for transmitting microwaves 12 having a polarized wave plane toward a measuring surface 16 is provided, and the polarization of the transmitted wave 12a is caused by diffuse reflection on the measuring surface 16. The wavelength of the transmitted wave 12a is selected to be equal to or less than the diameter of the unevenness of the measurement surface so that the wave surface is rotated, and the reception antenna 18 receives only the microwave 12b having a polarization plane rotated by diffused reflection on the measurement surface 16. The microwave 12b received by the receiving antenna 18 is mixed with the transmitted wave 12a.
(作 用)
マイクロ波発振器11より周波数変調された送
信波12aは、方向性結合器13を介して送信用
アンテナ14より送信される。その送信波12a
は第2図に示すX方向(Y方向)の偏波面を持
ち、液面16、容器壁19又はアンテナ保護用レ
ドーム20で反射される。この場合、使用マイク
ロ波12の波長を液面の波立ちの波長以下に選定
しているため、液面16で乱反射する際に偏波面
が回転し第2図に示すY方向(又はX方向)の成
分が生じる。一方マイクロ波波長に対し十分鏡面
と見なされるレドーム20や容器壁19からの反
射波12c,12dは送信時の偏波面を保持した
まま受信用アンテナ18に到達する。従つて受信
用アンテナ18は液面16での反射波12bのみ
を受信し、レドーム20や容器壁19からの反射
波12c,12dは受信しない。(Function) The frequency-modulated transmission wave 12a from the microwave oscillator 11 is transmitted from the transmission antenna 14 via the directional coupler 13. The transmitted wave 12a
has a polarization plane in the X direction (Y direction) shown in FIG. 2, and is reflected by the liquid surface 16, the container wall 19, or the antenna protection radome 20. In this case, since the wavelength of the microwave 12 used is selected to be less than the wavelength of the ripples on the liquid surface, the plane of polarization rotates when it is diffusely reflected on the liquid surface 16, causing it to move in the Y direction (or X direction) as shown in Figure 2. components are generated. On the other hand, reflected waves 12c and 12d from the radome 20 and the container wall 19, which are considered to have mirror surfaces sufficiently for microwave wavelengths, reach the receiving antenna 18 while maintaining the plane of polarization at the time of transmission. Therefore, the receiving antenna 18 receives only the reflected wave 12b from the liquid surface 16, and does not receive the reflected waves 12c and 12d from the radome 20 and the container wall 19.
従つて液面16等で反射されたマイクロ波12
b,12c,12dの内、受信用アンテナ18と
同じ偏波面をもつ成分のみが信号として検出さ
れ、受信用アンテナ18により受信されたマイク
ロ波の信号は、検波ミキサ23において、方向性
結合器15にて分離した送信波12aの一部と混
合され、ビート信号21を出力する。ビート信号
21はビート信号処理回路23においてビート波
の波数を計数する等の処理がなされ、液面16ま
での距離すなわちレベルが時々刻々変化するノズ
ル波形の影響を受けることなく正確に算出され
る。 Therefore, the microwave 12 reflected by the liquid surface 16 etc.
b, 12c, and 12d, only the component having the same polarization as the receiving antenna 18 is detected as a signal, and the microwave signal received by the receiving antenna 18 is sent to the detection mixer 23 by the directional coupler 15. It is mixed with a part of the transmitted wave 12a separated at , and a beat signal 21 is output. The beat signal 21 is subjected to processing such as counting the number of beat waves in the beat signal processing circuit 23, and the distance to the liquid surface 16, that is, the level, is accurately calculated without being affected by the nozzle waveform that changes from time to time.
なお、第3図乃至第6図は本発明の有効性を確
認するために行なつた実験の結果である。図中2
5はFMのための掃引電圧のオシロ写真であり、
横軸および縦軸スケールは各々2ms/div、
5mv/divである。26は波長12mmのマイクロ波
を用い送受信に同じ偏波面を持つアンテナ(平行
偏波アンテナと呼ぶ)により、平均粒径約30mmの
コークスを対象として収録したビート波形であ
り、約5mVの信号振幅が得られている。 Note that FIGS. 3 to 6 show the results of experiments conducted to confirm the effectiveness of the present invention. 2 in the diagram
5 is an oscilloscope photo of sweep voltage for FM,
Horizontal and vertical scales are each 2ms/div,
It is 5mv/div. 26 is a beat waveform recorded for coke with an average particle size of about 30 mm using a microwave with a wavelength of 12 mm and an antenna with the same polarization plane for transmission and reception (called a parallel polarization antenna), and the signal amplitude is about 5 mV. It has been obtained.
27は本発明に基づく送受信用アンテナ14,
18を直角に設定したレーダにより収録したビー
ト波形であり、従来の平行偏波アンテナと同程度
の信号振幅が得られている。一方鏡面と見なさせ
る鉄板を対象とした場合には、第5図および第6
図に示すように直角偏波アンテナによるビート波
29の振幅は平行偏波アンテナによるビート波2
8の10分の1以下であり、本発明の有効性が確認
できる。 27 is a transmitting/receiving antenna 14 based on the present invention,
This is a beat waveform recorded by a radar set at right angles to the antenna, and a signal amplitude comparable to that of a conventional parallel polarized antenna is obtained. On the other hand, when the target is an iron plate that is regarded as a mirror surface, Figures 5 and 6
As shown in the figure, the amplitude of the beat wave 29 due to the orthogonally polarized antenna is the same as the amplitude of the beat wave 29 due to the parallel polarized antenna.
It is less than 1/10 of 8, which confirms the effectiveness of the present invention.
(実施例)
以下、本発明を図示の実施例に従つて説明する
と、11はマイクロ波発振器で、マイクロ波12
を周波数変調して出力する。13は方向性結合器
で、マイクロ波発振器11から出力されたマイク
ロ波12の一部を送信用アンテナ14に出力する
と共に、他の一部を検波ミキサ15に送る。送信
用アンテナ14は、第2図に示すY方向(又はX
方向)の偏波面を持ち、マイクロ波発振器11に
より周波数変調されたマイクロ波12のうち、X
方向(又はY方向)の偏波面を持つたものを、送
信波12aとして測定面である溶融金属等の液面
16に向けて出力する。(Embodiment) The present invention will be explained below according to the illustrated embodiment. Reference numeral 11 represents a microwave oscillator;
is frequency modulated and output. 13 is a directional coupler which outputs a part of the microwave 12 output from the microwave oscillator 11 to the transmitting antenna 14 and sends the other part to the detection mixer 15. The transmitting antenna 14 is arranged in the Y direction (or
Of the microwaves 12 which have a polarization plane of
A wave having a polarization plane in the direction (or the Y direction) is output as a transmission wave 12a toward a liquid surface 16 of molten metal or the like that is a measurement surface.
18は受信用アンテナで、Y方向(又はX方
向)の偏波面をもち、液面16、容器壁19又は
アンテナ保護用レドーム20で反射されたマイク
ロ波12b,12c,12dのうち、第2図に示
すY方向(又はX方向)の偏波面をもつものを受
信する。検波ミキサ15は、受信用アンテナ18
で受信したマイクロ波12bと、方向性結合器1
3において分離した送信波12aの一部とを混合
し、ビート信号21を出力する。23はビート信
号処理回路で、ビート波の波数を計数する等の処
理を行なつて、液面16までの距離すなわちレベ
ルを算出する。 Reference numeral 18 denotes a receiving antenna, which has a polarization plane in the Y direction (or Receives a wave having a plane of polarization in the Y direction (or X direction) shown in FIG. The detection mixer 15 is connected to the receiving antenna 18.
The microwave 12b received by the directional coupler 1
3 and a part of the transmitted wave 12a separated in step 3, and outputs a beat signal 21. A beat signal processing circuit 23 performs processing such as counting the number of beat waves to calculate the distance to the liquid level 16, that is, the level.
そして前記マイクロ波発振器11の周波数変調
によつて使用マイクロ波12の波長を液面16の
波立ちの波長以下に選定しており、従つて、送信
波12aが液面で乱反射する際にその偏波面が回
転し、一方マイクロ波12の波長に対し十分鏡面
と見なされるレドーム20や容器壁19からの反
射波12c,12dは送信時の偏波面を保持した
まま受信用アンテナ18に達するので、受信用ア
ンテナ18には液面16からの反射波12bのみ
が受信され、反射波12c,12dは受信されな
いようになつている。 By frequency modulating the microwave oscillator 11, the wavelength of the microwave 12 used is selected to be less than the wavelength of the ripples on the liquid surface 16. Therefore, when the transmitted wave 12a is diffusely reflected on the liquid surface, its polarization On the other hand, the reflected waves 12c and 12d from the radome 20 and the container wall 19, which are considered to have a sufficiently mirror surface with respect to the wavelength of the microwave 12, reach the receiving antenna 18 while maintaining the polarization plane at the time of transmission. The antenna 18 receives only the reflected wave 12b from the liquid surface 16, and does not receive the reflected waves 12c and 12d.
なお、前記実施例では測定面を高温溶融金属等
の液面16としているが、測定面はこれに限定さ
れず、例えば粉粒状の原料レベルを測定面として
もよく、この場合には使用マイクロ波12の波長
を粉粒状体の平均粉粒径以下に選定すればよい。 In the above embodiment, the measurement surface is the liquid level 16 of high-temperature molten metal, etc., but the measurement surface is not limited to this. For example, the measurement surface may be the level of powdery raw material, and in this case, the microwave used The wavelength of 12 may be selected to be equal to or less than the average particle diameter of the powder or granular material.
(発明の効果)
本発明によれば、測定面での乱反射による偏波
面の回転をうまく利用して、測定面で乱反射した
マイクロ波のみを受信し、その受信したマイクロ
波と送信波とをミキシングして測定面の位置を算
出するので、測定面以外から反射する不要反射の
マイクロ波の影響を全く受けずに済み、従つて不
要反射波によるビート波が時々刻々変化する場合
でも、測定面で反射したマイクロ波のみから測定
面の位置を正確かつ簡単に測定でき、その効果は
著大である。(Effects of the Invention) According to the present invention, by making good use of the rotation of the plane of polarization due to diffuse reflection on the measurement surface, only the microwaves diffusely reflected on the measurement surface are received, and the received microwaves and the transmitted waves are mixed. Since the position of the measurement surface is calculated by using The position of the measurement surface can be measured accurately and easily using only the reflected microwaves, and the effect is significant.
第1図は本発明の一実施例を示す構成図、第2
図は同マイクロ波の偏波面を示す図、第3図乃至
第6図は夫々実験結果を示すビート波形図であ
る。第7図は従来例を示す構成図である。
12…マイクロ波、14…送信用アンテナ、1
6…測定面、18…受信用アンテナ。
FIG. 1 is a configuration diagram showing one embodiment of the present invention, and FIG.
The figure shows the polarization plane of the microwave, and FIGS. 3 to 6 are beat waveform diagrams showing the experimental results. FIG. 7 is a configuration diagram showing a conventional example. 12...Microwave, 14...Transmission antenna, 1
6...Measurement surface, 18...Receiving antenna.
Claims (1)
からの反射波12bとをミキシングしてビート信
号21をつくり、該ビート信号21から測定面1
6の位置を算出するようにしたレベル測定装置に
おいて、 偏波面を有するマイクロ波12を測定面16に
向けて送信する送信用アンテナ14を設けると共
に、測定面16での乱反射により送信波12aの
偏波面が回転するように、送信波12aの波長を
測定面の凹凸径以下に選定し、測定面16での乱
反射によつて回転した偏波面を有するマイクロ波
12のみを受信する受信用アンテナ18を設け、
該受信用アンテナ18で受信した偏波面を持つマ
イクロ波12と前記送信波12aとをミキシング
するようにしたことを特徴とするレベル測定装
置。[Claims] 1. Transmission wave 12a of microwave 12 and measurement surface 16
A beat signal 21 is created by mixing the reflected wave 12b from the measurement surface 1.
In the level measuring device configured to calculate the position of 6, a transmitting antenna 14 for transmitting microwaves 12 having a polarized wave plane toward a measuring surface 16 is provided, and the polarization of the transmitted wave 12a is caused by diffuse reflection on the measuring surface 16. The wavelength of the transmitted wave 12a is selected to be equal to or less than the diameter of the unevenness of the measurement surface so that the wave surface is rotated, and the reception antenna 18 receives only the microwave 12 having a polarization plane rotated by diffused reflection on the measurement surface 16. established,
A level measuring device characterized in that the microwave 12 having a polarized wave plane received by the receiving antenna 18 and the transmitted wave 12a are mixed.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22283687A JPS6465420A (en) | 1987-09-05 | 1987-09-05 | Level measuring instrument |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22283687A JPS6465420A (en) | 1987-09-05 | 1987-09-05 | Level measuring instrument |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6465420A JPS6465420A (en) | 1989-03-10 |
| JPH0543973B2 true JPH0543973B2 (en) | 1993-07-05 |
Family
ID=16788671
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22283687A Granted JPS6465420A (en) | 1987-09-05 | 1987-09-05 | Level measuring instrument |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6465420A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2021110019A (en) * | 2020-01-14 | 2021-08-02 | 日本製鉄株式会社 | Level measuring device and level measuring method |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| SE466519B (en) * | 1989-04-10 | 1992-02-24 | Saab Marine Electronics | DEVICE FOR Saturation of the level of a fluid present in a container |
| US6759976B1 (en) | 2002-12-20 | 2004-07-06 | Saab Marine Electronics Ab | Method and apparatus for radar-based level gauging |
| JP2006317162A (en) * | 2005-05-10 | 2006-11-24 | Matsushita Electric Ind Co Ltd | Radar equipment |
-
1987
- 1987-09-05 JP JP22283687A patent/JPS6465420A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2021110019A (en) * | 2020-01-14 | 2021-08-02 | 日本製鉄株式会社 | Level measuring device and level measuring method |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6465420A (en) | 1989-03-10 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |