JPS5822922A - Molten metal level gauge by microwave - Google Patents

Molten metal level gauge by microwave

Info

Publication number
JPS5822922A
JPS5822922A JP56120631A JP12063181A JPS5822922A JP S5822922 A JPS5822922 A JP S5822922A JP 56120631 A JP56120631 A JP 56120631A JP 12063181 A JP12063181 A JP 12063181A JP S5822922 A JPS5822922 A JP S5822922A
Authority
JP
Japan
Prior art keywords
antenna
microwave
molten metal
distance
level gauge
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
Application number
JP56120631A
Other languages
Japanese (ja)
Inventor
Yasuo Koyanagi
小柳 弥夫
Takeo Yamada
健夫 山田
Kosaku Kosaka
高阪 廣作
Norio Terajima
寺島 典男
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
JFE Engineering Corp
Original Assignee
NKK Corp
Nippon Kokan Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by NKK Corp, Nippon Kokan Ltd filed Critical NKK Corp
Priority to JP56120631A priority Critical patent/JPS5822922A/en
Publication of JPS5822922A publication Critical patent/JPS5822922A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q13/00Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
    • H01Q13/20Non-resonant leaky-waveguide or transmission-line antennas; Equivalent structures causing radiation along the transmission path of a guided wave
    • H01Q13/24Non-resonant leaky-waveguide or transmission-line antennas; Equivalent structures causing radiation along the transmission path of a guided wave constituted by a dielectric or ferromagnetic rod or pipe
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F23/00Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
    • G01F23/22Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
    • G01F23/28Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Thermal Sciences (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Radar Systems Or Details Thereof (AREA)
  • Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)

Abstract

PURPOSE:To measure a distance between a molten metal surface and an antenna with high accuracy even in case when a place being in the vicinity of the molten metal surface is narrow, by using a dielectric rod antenna for a transmitting and receiving antenna. CONSTITUTION:A transmitting and receiving antenna 3 is formed by attaching a tapered dielectric rod 3b to the tip of a waveguide 3a, and is constituted of small size, comparing with a horn antenna or a parabolic antenna. Accordingly, even in case when a place being in the vicinity of a molten metal surface is narrow, a distance between the molten metal surface and the antenna is measured with high accuracy.

Description

【発明の詳細な説明】 本発明社基準辺と測定辺とからなるマイクロ波ブリッジ
を有し、測定辺上の被測定対象物である溶融金属湯面距
離又社その変位を位相比較方式により一定するマイク−
IIm融金異金属湯面計曳に―すゐ0 従来のこの種(Qwイクロ波溶融金属湯面計は測定範囲
が狭いという欠点があったので、本出願人は先にその欠
点を解消したマイクロ波変位針を特願昭56−9519
1号により提案している。このマイクロ波変位針は、基
準辺と測定辺からなるマイクロ波ブリッジを有し、測定
辺上の被測定対象物の変位を位相比較方式により一定す
るマイクロ波変位計において、移相量が2Kを越える度
にその回数を積算するカウンタを備えたものであシ、高
精wILKかつ広範15 K III定するという所期
の目的を達成しているが、送受信用アンテナはこの種の
アンテナヘッドとして一般的に用いられているホーンア
ンテナ又祉パラボナアンテナを用いておシ、これらめ−
アンテナの寸法線大きいので、例えに小型連続鋳造モー
ルド等の狭い場所に設置する仁とは回前であり九〇 ホーンアンテナ及びパラボナアンテナの大きさは、10
G&帯程度の周tILaで約3C程度の指向性を得るた
めには、例えd第1図及び第2図に示される寸法が必要
となる。開口部の大きさは、ホーンアンテナ1(第1N
!!2)で紘50■×70雪、パラボナアンテナ2 (
1!2図)で紘100■φllfになる0この几め、送
受信に同一アンテナを使用する場合はもとよプ独立のア
ンテナで使用する場合には、これらの二倍のアンテナ設
置空間が必要となる。
Detailed Description of the Invention The present invention has a microwave bridge consisting of a reference side and a measurement side, and the distance and displacement of the molten metal surface, which is the object to be measured, on the measurement side are kept constant by a phase comparison method. Microphone
IIm Financing Dissimilar Metal Level Gauge - Sui 0 This type of conventional (Qw microwave molten metal level gauge) had the drawback of a narrow measurement range, so the applicant first solved that drawback. Patent application for microwave displacement needle 1986-9519
This is proposed by No. 1. This microwave displacement needle has a microwave bridge consisting of a reference side and a measurement side, and is a microwave displacement meter in which the displacement of the object to be measured on the measurement side is fixed by a phase comparison method, and the amount of phase shift is 2K. It is equipped with a counter that adds up the number of times each time it exceeds 15K, and achieves the intended purpose of determining high-precision wILK and a wide range of 15K III. These methods can be achieved using a horn antenna or a parabolic antenna, which is commonly used in
Because the dimensions of the antenna are large, it is difficult to install it in a narrow space such as in a small continuous casting mold.
In order to obtain a directivity of about 3C with a circumference tILa of the G& band size, the dimensions shown in FIGS. 1 and 2 are required, for example. The size of the opening is determined by the size of the horn antenna 1 (1st N
! ! 2) Hiro 50×70 snow, parabon antenna 2 (
Figures 1 and 2) will result in 100 ■ φllf 0 With this method, if you use the same antenna for transmitting and receiving, but if you use separate antennas, you will need twice as much antenna installation space. becomes.

さらに、より鋭い指向性が要求される場合にはアンテナ
の寸法もその指向性に反比例して増大するため、狭い空
間での設置はますます困難になる。
Furthermore, if sharper directivity is required, the size of the antenna increases in inverse proportion to the directivity, making installation in a narrow space increasingly difficult.

元来マイクロ波による湯面計は悪環境下での針側に強味
を発揮するが、上述した理由によシ小型連続鋳造モール
ドの湯面レベル測定のように狭い場所での使用は困難で
あシ、未だその解決策はないという実情にあった。
Microwave level gauges are originally effective on the needle side in adverse environments, but for the reasons mentioned above, they are difficult to use in confined spaces, such as when measuring the level of hot water in small continuous casting molds. The reality is that there is still no solution to this problem.

本発明はこのような情況に僑みて発明されたものであり
、掬定領斌が広範囲であpがっ小型連続鋳造モールドの
場合のような狭い空間においても溶融金属の湯面レベル
又はその変位の測定を可能にしたマイクロ波溶融金属湯
面計を提供するものである0すなわち本発明に係る湯面
計拡、基準辺と測定辺とからなるマイクロ波ブリッジと
、移相量が2Kを越える度にその回数を積算するカウン
タとを備え、6111定辺上の被測定対象物の距離又は
その変位を位相比較方式により測定するマイクロ波溶融
金属湯面計において、マイクロ波の送受信用アンテナに
コーンアンテナを用いた本のである。
The present invention was devised in view of this situation, and it is possible to control the level of the molten metal or its displacement even in a narrow space such as in the case of a small continuous casting mold where the scooping range is wide and wide. In other words, the present invention provides a microwave bridge consisting of a reference side and a measurement side, and a phase shift amount exceeding 2K. 6111 A microwave molten metal level meter that measures the distance or displacement of an object on a constant side using a phase comparison method, is equipped with a counter that adds up the number of times, and is equipped with a cone on an antenna for transmitting and receiving microwaves. This is a book that uses antennas.

以下本発明の実施例を内面に基づきながら説明するO 易4図社本発明の一実施例に係るマイクロ波溶融金属湯
面計のアンテナの説明図であり、このアンテナ3拡導波
管3aの先にテーパのついたSt体棒6bが過当な整合
条件で接続されて構成されている0棒の長手方向にテー
パ部3bから電波が放射さ亀アンテナと1.7での機能
を発揮する。この図からも明らかなように、ホーンアン
テナ1やパラボテアンテナ20大きさと比較して、この
アンテナ3は断面が円形又は楕円形である九め小型にな
っている。
Embodiments of the present invention will be described below based on the inner surface. Radio waves are radiated from the tapered portion 3b in the longitudinal direction of the 0 rod, which is constructed by connecting the St body rod 6b with a taper at the tip under an excessive matching condition, and exhibits the function of the turtle antenna and 1.7. As is clear from this figure, compared to the size of the horn antenna 1 and the parabolic antenna 20, this antenna 3 has a circular or elliptical cross section and is nine times smaller.

例えば10G&帯で指向性を必要とする場合は、このア
ンテナ3の寸法は13霞φx193mmであり、@1図
及び第2図に示されている従来例の寸法と比べて見ても
、明らかに小型になっている。
For example, if directivity is required in the 10G & band, the dimensions of this antenna 3 are 13mm φ x 193mm, which is clearly seen when compared with the dimensions of the conventional example shown in @Figure 1 and Figure 2 It is small.

また、このアンテナ30指向性祉テーパ部の長さによっ
て決まシ、その断面積には関係がないため、必要に応じ
た指向性を得るためKf−1長さを変える必要はあるが
、断面積は変える必要がない。
Also, since the directivity of this antenna 30 is determined by the length of the tapered part and has nothing to do with its cross-sectional area, it is necessary to change the length of Kf-1 in order to obtain the required directivity, but the cross-sectional area does not need to be changed.

このため、50〜40w@度の設定空間幅があれば、溶
融金属の湯面レベルの計測線可能となる〇ところで、耐
熱性の問題に関して線、アンテナを構成する誘電体材料
に高耐熱性のセラミックスを使えば解決できる。さらに
、アンテナ3紘もともと小形棒形状をしているから、8
4図に示すように、アンテナ5の外周に冷却用の筒4を
配置して冷却用エアー5を吹けば熱対策は完全である。
For this reason, if there is a set space width of 50 to 40 W@degrees, it becomes possible to measure the level of the molten metal.By the way, regarding the issue of heat resistance, the dielectric material that makes up the wire and antenna has high heat resistance. This can be solved using ceramics. Furthermore, since antenna 3 originally has a small bar shape, 8
As shown in FIG. 4, heat countermeasures can be completed by arranging a cooling tube 4 around the outer periphery of the antenna 5 and blowing cooling air 5.

従って、小製連続鋳造モールドのようにアンテナをノズ
ル近傍に配置せざるを得ない場合で4、その―射熱や湯
面からの輻射熱からアンテナを守ることができ、かつノ
ズル面からのマイクロ波の不要反射の影響を防ぐ事がで
きる。
Therefore, in cases where the antenna must be placed near the nozzle, such as in the case of small-scale continuous casting molds, the antenna can be protected from radiation heat and radiant heat from the hot water surface, and microwaves from the nozzle surface can be protected. It is possible to prevent the effects of unnecessary reflections.

lIl!5@は本発明の上記一実施例に係るマイクロ波
溶融金属湯面計の全体のブロック図である。図中6はモ
ールド、7は浸漬ノズルを示している〇そして、11は
マイクロ波発振器、12線方向性結合器、16は送信ア
ンテナ、14は被III定対象物である湯面、15は受
信アンテナ、16社周波数変換器、17は検波器、18
は測定辺21と基準辺22との間の位相差を検出する位
相差検出回路119はカウンタ、20は距離計算回路、
23は周波数変換を行なうための基準発振器である〇こ
こで送信アンテナ1′5及び受信アンテナ15は第3囚
のコーンアンテナを用いている。この実施例では送信ア
ンテナと受信アンテナとをそ牡ぞれ別のものにしている
が、同一のアンテナで両者を兼用させるようにしてもよ
いことはいうまでもない0 以上の構成からなるマイクロ波溶融金属湯面計26にお
いて、マイクロ波発振器11から発生した周波数foの
マイクロ波線方向性結合器12によシ、送信アンテナ1
3を介して被III定対象物14に送信されそこで反射
されて受信アンテナ15に戻る測定辺21と、周波数変
換回路16へ向かう基準辺22とに分離される。基準辺
22では周波数変換器16により、周波数foから基準
発振益23の周波数fs (fo > h )が差し引
か牡、この減算周波数(fa−f+)が検知器17に与
えられる0ここでは勿論周波数foと周波数flとを加
算した周波数(f。
lIl! 5 is an overall block diagram of the microwave molten metal water level gauge according to the above embodiment of the present invention. In the figure, 6 is a mold, 7 is an immersion nozzle, 11 is a microwave oscillator, 12 is a wire directional coupler, 16 is a transmitting antenna, 14 is a hot water surface which is the object to be measured, and 15 is a receiver Antenna, 16 frequency converter, 17 detector, 18
A phase difference detection circuit 119 that detects the phase difference between the measurement side 21 and the reference side 22 is a counter, 20 is a distance calculation circuit,
Reference numeral 23 is a reference oscillator for frequency conversion. Here, the transmitting antenna 1'5 and the receiving antenna 15 are third cone antennas. In this embodiment, the transmitting antenna and the receiving antenna are separate, but it goes without saying that the same antenna may be used for both purposes. In the molten metal level gauge 26, the microwave ray directional coupler 12 of the frequency fo generated from the microwave oscillator 11 is connected to the transmitting antenna 1.
3 to the target object 14 , where it is reflected and returns to the receiving antenna 15 , and a reference side 22 that goes toward the frequency conversion circuit 16 . At the reference side 22, the frequency fs (fo > h) of the reference oscillation gain 23 is subtracted from the frequency fo by the frequency converter 16, and this subtracted frequency (fa-f+) is given to the detector 17. Here, of course, the frequency fo and the frequency fl (f.

十f1)を検波器17に与えてもよい。10f1) may be applied to the detector 17.

測定辺21では送受値アンテナ13.15と被測定対象
物14との距離Rが変化すれば、検波器17に到達する
までの径路も変化する0従って、横波器17で基準辺2
2及び測定辺21からの信号をiキシングをしてからバ
ンドパスフィルタを通せば、両辺間の位相差は測定し易
いflの周波数上の情報として、径路24及び25の間
に現われるO この径路24及び25の間0位相差を位相差検出回路1
8により測定すれば、第6図囚に示すように、送受信ア
ンテナ13.15から被測定対象物14までの距@Rに
より、λ4単位に不連続変化を生じて′gi帰する位相
差−が測定できる〇カウンタ19は位相差検出器18の
出力が2に→0に復帰するときにカウントアツプし、0
→2Kに復帰する時にはカウントダウンを行なう回路で
あるから、第6図(B)のような距離Rが大きくなるに
従ってカウント数nも増加する。
On the measuring side 21, if the distance R between the transmitting/receiving value antenna 13.15 and the object to be measured 14 changes, the path to reach the detector 17 also changes.
If the signals from 2 and measurement side 21 are subjected to i-xing and then passed through a bandpass filter, the phase difference between both sides appears between paths 24 and 25 as information on the frequency of fl, which is easy to measure. Phase difference detection circuit 1 detects 0 phase difference between 24 and 25.
8, as shown in Figure 6, the distance @R from the transmitting/receiving antenna 13.15 to the object to be measured 14 causes a discontinuous change in units of λ4, and the phase difference due to Measurement possible The counter 19 counts up when the output of the phase difference detector 18 returns from 2 to 0.
→ Since the circuit performs a countdown when returning to 2K, the count number n also increases as the distance R increases as shown in FIG. 6(B).

従って、距離計算回路20によシ次式の演算を行なえば
湯面距離Rが得られる。
Therefore, if the distance calculation circuit 20 calculates the following equation, the hot water level distance R can be obtained.

上式の右辺の1!n3項L・は、測定開始点の値で定数
項であるから測定誤差には影響しない。第21Jlは位
相比較方式による項であり、周波数10G&のマイクロ
波を使用すれば±a I w O測定精度が得られる。
1 on the right side of the above equation! The n3 term L. is the value at the measurement starting point and is a constant term, so it does not affect the measurement error. The 21st Jl is a term based on the phase comparison method, and if microwaves with a frequency of 10G& are used, ±a I w O measurement accuracy can be obtained.

そして、第1項においてλ(マイクロ波の波長)は5桁
の精度で測定することができるので、周波910G&の
マイクロ波で測定すれば、±0.1−の測定精度が得ら
れる。1147図に距離計算回路20の出力を実際の湯
面距離との関係で示す。この図からも明らかなように直
線性の優れた出力が得られている。
In the first term, λ (wavelength of the microwave) can be measured with an accuracy of 5 digits, so if the measurement is performed using a microwave with a frequency of 910G&, a measurement accuracy of ±0.1- can be obtained. Figure 1147 shows the output of the distance calculation circuit 20 in relation to the actual hot water level distance. As is clear from this figure, an output with excellent linearity is obtained.

上述の実施例では湯面とアンテナとの距離すなわち湯面
距離Rを求める場合について説明したが、湯面距離の変
位ΔRを求めるには距離計算回路20において次式の計
算をすればよいC n・λ  λ・e ΔB、−−+ −−L・        (2)2  
4π 以上の説明から明らかなように、本発明に係るマイクa
波溶融金属湯面計によれば、カウンタ19演算回路中に
挿入した事によシ広範囲にわたって高n度に測定する事
ができ、さらに送受信用アンテナをコーン形状にした事
によって、アンテナの設fIL場所が得られないような
狭い場所であっても、当該場所での測定が可能になって
いる0
In the above-described embodiment, the case where the distance between the hot water surface and the antenna, that is, the hot water surface distance R is calculated, was explained. However, in order to calculate the displacement ΔR of the hot water surface distance, the distance calculation circuit 20 should calculate the following formula C n・λ λ・e ΔB, −−+ −−L・ (2) 2
4π As is clear from the above explanation, the microphone a according to the present invention
According to the wave molten metal level gauge, by inserting it into the calculation circuit of the counter 19, it is possible to measure at a high degree over a wide range.Furthermore, by making the transmitting and receiving antenna cone-shaped, the antenna design Even in narrow spaces where space is not available, measurements can be taken at the location.

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

第1図拡小−ンアンテナの説明図、第2図はノ(ラボナ
アンテナの説明図、第3図は本発明の一実M1例に係る
湯面計のアンテナの説明図、第4脂は本発明の他の実施
例に係る湯面計のアンテナの説明図、第5図は本発明の
上記一実施例に係る湯面側の全体のブロック図、第6図
(A) (B+は第5−のカウンタの動作説明1、第7
図は第5図の湯面計の出力特性図である。 1・・・ホーンアンテナ、2・・・パラボナアンテナ、
3・・・コーンアンテナ、4・・・冷却用筒、5・・・
冷却用エアー、11・・・マイクロ波発振器、12・・
・方向性結合器、13・・・送信アンテナ、14・・・
被測定対象物、15・・・受信アンテナ、16・・・周
波数変換器、17・・・検波器、18・・・位相差検出
器、19・・・カウンタ、20・・・距離計算回路、2
1・・・マイクロ波の測定辺、22・・・マイクロ波の
基準辺、23・・・基準発振回路、26・・・マイクロ
波溶融金楓湯面針。 代理人 弁理士 佐 藤 正 年 第3図 3a 第4図 第5図 竺6図 を桿77;JIAIしくt17(mm)手続補正書(自
発) 特許庁長官殿        昭和56年9月2日1、
事件の表示 特願昭 56−1204+51号 2・発明の名称 !イクー波aim金属湯画計 3、補正をする者 事件との関係   畳許出願人 名 称(412)日本鋼管株式会社 4、代理人 6、補正の対象 ′S川用d;:i ’ 、+i7 (1)明細書O特許請求の範囲を別紙のとお抄補正する
。 伐) 明細書を次のとおp補正する。 以上 基準辺と測定辺とからなるマイクロ波ブリッジと、移相
量が2πを越える度にそ0回数を積算するカクンタとを
備え、測定辺上O被側定対象物の7距離又はその変位を
位相比較方式によp測定する→イクロ波溶融金属湯面計
において、マイクロ波の送受信用アンテナに誘電体棒ア
ンテナを用φた事を特徴とするマイクロ波溶融金属湯函
計。
Fig. 1 is an explanatory diagram of an enlarged antenna, Fig. 2 is an explanatory diagram of a rabona antenna, Fig. 3 is an explanatory diagram of an antenna of a water level gauge according to the M1 example of the present invention, An explanatory diagram of an antenna of a water level gauge according to another embodiment of the present invention, FIG. 5 is a block diagram of the entire hot water level side according to the above embodiment of the present invention, and FIG. 5- Counter operation explanation 1, 7th
The figure is an output characteristic diagram of the hot water level gauge shown in FIG. 1...Horn antenna, 2...Parabona antenna,
3... Cone antenna, 4... Cooling tube, 5...
Cooling air, 11...Microwave oscillator, 12...
・Directional coupler, 13... Transmission antenna, 14...
Object to be measured, 15... Receiving antenna, 16... Frequency converter, 17... Detector, 18... Phase difference detector, 19... Counter, 20... Distance calculation circuit, 2
DESCRIPTION OF SYMBOLS 1...Microwave measurement side, 22...Microwave reference side, 23...Reference oscillation circuit, 26...Microwave melted maple surface needle. Agent Patent Attorney Tadashi Sato Figure 3, Figure 4, Figure 5, Figure 6, Figure 77;
Display of the case Patent application No. 56-1204+51 No. 2・Name of the invention! Ikuha aim metal hot water plan 3, relationship with the case of the person making the amendment Name of the applicant for the tatami license (412) Nippon Kokan Co., Ltd. 4, agent 6, subject of amendment 'S River use d;:i', +i7 ( 1) Amend the specification O and claims by adding a separate sheet. ) Amend the statement as follows. Equipped with a microwave bridge consisting of a reference side and a measurement side, and a kakunta that adds up the number of times each time the amount of phase shift exceeds 2π, it is possible to calculate the distance of 7 distances of a fixed object on the measurement side or its displacement. A microwave molten metal water level gauge measuring p by a phase comparison method, characterized in that a dielectric rod antenna is used as a microwave transmitting and receiving antenna.

Claims (1)

【特許請求の範囲】[Claims] 基準辺と測定辺とからなるマイクロ波ブリッジと、移相
量が2胃を越える匿にその回数を積算するカウンタとを
備え、測定辺上の被測定対象物の距離又はその変位を位
相比較方式によ17 Ill定するマイクロ波溶融金属
湯面計において、マイクロ波の送受信用アンテナにコー
ンアンテナを用い窺事を特徴とするiイクロ波溶融金属
湯面計〇
Equipped with a microwave bridge consisting of a reference side and a measurement side, and a counter that adds up the number of times the amount of phase shift exceeds two stomachs, the distance of the object to be measured on the measurement side or its displacement is determined using a phase comparison method. 17 Microwave molten metal level gauge characterized in that a cone antenna is used as an antenna for transmitting and receiving microwaves.
JP56120631A 1981-08-03 1981-08-03 Molten metal level gauge by microwave Pending JPS5822922A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56120631A JPS5822922A (en) 1981-08-03 1981-08-03 Molten metal level gauge by microwave

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56120631A JPS5822922A (en) 1981-08-03 1981-08-03 Molten metal level gauge by microwave

Publications (1)

Publication Number Publication Date
JPS5822922A true JPS5822922A (en) 1983-02-10

Family

ID=14790999

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56120631A Pending JPS5822922A (en) 1981-08-03 1981-08-03 Molten metal level gauge by microwave

Country Status (1)

Country Link
JP (1) JPS5822922A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0669673A1 (en) * 1994-02-23 1995-08-30 VEGA Grieshaber KG Antenna device for a radar level gauge
US5610527A (en) * 1993-07-12 1997-03-11 Kabushiki Kaisha Toshiba Phase difference microwave densitometer and method which detects a number of phase rotations through a reference point
US6155112A (en) * 1996-10-04 2000-12-05 Endress + Hauser Gmbh + Co. Filling level measuring device operating with microwaves
JPWO2012176243A1 (en) * 2011-06-24 2015-02-23 株式会社ニレコ Molten metal level measuring apparatus and molten metal level measuring method

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5112115B2 (en) * 1972-03-25 1976-04-16
JPS55164380A (en) * 1979-06-04 1980-12-22 Burijiendo Puroseshizu Ltd Microwave transmitter receiver

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5112115B2 (en) * 1972-03-25 1976-04-16
JPS55164380A (en) * 1979-06-04 1980-12-22 Burijiendo Puroseshizu Ltd Microwave transmitter receiver

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5610527A (en) * 1993-07-12 1997-03-11 Kabushiki Kaisha Toshiba Phase difference microwave densitometer and method which detects a number of phase rotations through a reference point
US5969254A (en) * 1993-07-12 1999-10-19 Kabushiki Kaisha Toshiba Phase difference measuring apparatus and method
EP0669673A1 (en) * 1994-02-23 1995-08-30 VEGA Grieshaber KG Antenna device for a radar level gauge
US6155112A (en) * 1996-10-04 2000-12-05 Endress + Hauser Gmbh + Co. Filling level measuring device operating with microwaves
US6276199B1 (en) 1996-10-04 2001-08-21 Endress + Hauser Gmbh + Co. Method for producing filling level measuring device operating with microwaves
JPWO2012176243A1 (en) * 2011-06-24 2015-02-23 株式会社ニレコ Molten metal level measuring apparatus and molten metal level measuring method
US9322696B2 (en) 2011-06-24 2016-04-26 Nireco Corporation Apparatus for measuring level of molten metal and method for measuring level of molten metal

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