Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0136897B2 - - Google Patents
[go: Go Back, main page]

JPH0136897B2 - - Google Patents

Info

Publication number
JPH0136897B2
JPH0136897B2 JP7353983A JP7353983A JPH0136897B2 JP H0136897 B2 JPH0136897 B2 JP H0136897B2 JP 7353983 A JP7353983 A JP 7353983A JP 7353983 A JP7353983 A JP 7353983A JP H0136897 B2 JPH0136897 B2 JP H0136897B2
Authority
JP
Japan
Prior art keywords
horn
measured
transmitting
receiving
microwave
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
Application number
JP7353983A
Other languages
Japanese (ja)
Other versions
JPS59197842A (en
Inventor
Seiichiro Kyobe
Hirotoshi Ishikawa
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.)
Yokogawa Electric Corp
Original Assignee
Yokogawa Electric Corp
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 Yokogawa Electric Corp filed Critical Yokogawa Electric Corp
Priority to JP7353983A priority Critical patent/JPS59197842A/en
Publication of JPS59197842A publication Critical patent/JPS59197842A/en
Publication of JPH0136897B2 publication Critical patent/JPH0136897B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N22/00Investigating or analysing materials by the use of microwaves or radio waves, i.e. electromagnetic waves with a wavelength of one millimetre or more
    • G01N22/04Investigating moisture content

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (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)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Measurement Of Resistance Or Impedance (AREA)

Description

【発明の詳細な説明】 本発明は、マイクロ波水分計の改良に関する。
一般に、マイクロ波帯では、水分のマイクロ波吸
収が極めて大きい。このため、水分のマイクロ波
吸収を利用し、マイクロ波の減衰量から被測定物
の水分量を測定することが従来から広く行なわれ
ていた。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in microwave moisture meters.
Generally, in the microwave band, microwave absorption of water is extremely large. For this reason, it has been widely practiced in the past to utilize the microwave absorption of moisture and to measure the moisture content of the object to be measured from the amount of attenuation of the microwaves.

第1図は、このような従来のマイクロ波水分計
を説明する従来例構成説明図であり、図中、1は
マイクロ波信号を発生するマイクロ波源たる発信
器、2は一方向にのみマイクロ波を通し逆方向に
はマイクロ波を殆んど通さないアイソレータ、3
は第1導波管(若しくは同軸ケーブル、以下単に
「導波管」という)4を介してアイソレータ2に
接続された送信ホーン、5は送信ホーン3と所定
距離lを隔てて配設される受信ホーン、7は第2
導波管6を介して受信ホーン5に接続された送信
ホーン、8は送受信ホーン3,5間の距離と同一
の所定距離lを送信ホーン7との間に隔てて配設
される受信ホーン、9は送信ホーン3,7と受信
ホーン5,8の間に配置された例えばシト状の紙
などでなる被測定物、11は例えばクリスタルダ
イオード等でなり第3導波管10を介して受信ホ
ーン8の出力を検出する検出部、12は検出部1
1の出力を受け所定の演算処理を施こして被測定
物中の水分量を算出する演算部である。
FIG. 1 is a diagram illustrating the configuration of a conventional microwave moisture meter. An isolator that allows almost no microwave to pass through the microwave in the opposite direction, 3
5 is a transmitter horn connected to the isolator 2 via a first waveguide (or coaxial cable, hereinafter simply referred to as "waveguide") 4, and 5 is a receiver disposed at a predetermined distance l from the transmitter horn 3. Horn, 7 is second
A transmitting horn 8 is connected to the receiving horn 5 via a waveguide 6, and a receiving horn 8 is disposed at a predetermined distance l, which is the same as the distance between the transmitting and receiving horns 3 and 5, from the transmitting horn 7. Reference numeral 9 denotes an object to be measured made of, for example, a sheet of paper, placed between the transmitting horns 3, 7 and the receiving horns 5, 8; 11, made of, for example, a crystal diode; 8 is a detection unit that detects the output, 12 is a detection unit 1
This is a calculation unit that receives the output of No. 1 and performs predetermined calculation processing to calculate the amount of water in the object to be measured.

上記構成からなる従来例において、発振器1か
ら送出されたマイクロ波は、アイソレータ2およ
び第1導波管4を経て送信ホーン3から被測定物
9に投射される。また、被測定物9を透過して水
分子による減衰を受けたマイクロ波は、受信ホー
ン5で受信されてのち第2導波管6を経て、送信
ホーン7から再び被測定物9に投射される。該被
測定物を透過して再度水分子による減衰を受けた
マイクロ波は、受信ホーン8で受信されてのち第
3導波管10を経て検出部11で検出される。該
検出部の出力に基ずき、演算部12内で施こされ
る演算処理により、被測定物9中の水分量が求め
られるようになる。
In the conventional example having the above configuration, the microwave transmitted from the oscillator 1 is projected onto the object to be measured 9 from the transmission horn 3 via the isolator 2 and the first waveguide 4. Further, the microwave that has passed through the object to be measured 9 and has been attenuated by water molecules is received by the receiving horn 5, passes through the second waveguide 6, and is projected onto the object to be measured 9 again from the transmitting horn 7. Ru. The microwaves that have passed through the object to be measured and are attenuated by water molecules again are received by the reception horn 8 and then passed through the third waveguide 10 and detected by the detection unit 11. Based on the output of the detection section, the amount of water in the object to be measured 9 can be determined by arithmetic processing performed in the calculation section 12.

然し乍ら、上記従来例においては、被測定物9
がシート状であるため被測定物のばたつきが生じ
易く、このようなばたつきによつて生ずる定在波
のため、パスライン特性が大きな測定誤差要因に
なるという欠点があつた。
However, in the above conventional example, the object to be measured 9
Since it is in the form of a sheet, the object to be measured tends to fluctuate, and the standing waves generated by such fluttering have the disadvantage that the pass line characteristics become a major source of measurement error.

本発明はかかる欠点に鑑みてなされたものであ
り、その目的は、マイクロ波を使用して被測定物
中の水分量を測定するマイクロ波水分計におい
て、シート状被測定物のばたつきの影響を大きく
受けることなく、被測定物中の水分量を高精度に
測定できるマイクロ波水分計を提供することにあ
る。
The present invention has been made in view of these drawbacks, and its purpose is to reduce the effects of flapping of a sheet-like object to be measured in a microwave moisture meter that uses microwaves to measure the amount of moisture in an object to be measured. It is an object of the present invention to provide a microwave moisture meter capable of measuring the amount of moisture in a measured object with high precision without being subjected to large effects.

本発明の特徴は、マイクロ波を使用して被測定
物中の水分量を測定するマイクロ波水分計におい
て、第1送・受信ホーンの間隔をl1とし第2送・
受信ホーンの間隔をl2とするとき、l2−l1≒nλ+
λ/4(但し、n;自然数、λ;波長)が成立する
ように、第1および第2の送・受信ホーンを配置
したことにある。
The feature of the present invention is that in a microwave moisture meter that measures the amount of moisture in a measured object using microwaves, the interval between the first transmitting and receiving horns is l1 , and the distance between the first transmitting and receiving horns is l1.
When the distance between the receiving horns is l 2 , l 2 −l 1 ≒nλ+
The first and second transmitting/receiving horns are arranged so that λ/4 (where n: natural number, λ: wavelength) holds.

以下、本発明について図を用いて詳細に説明す
る。第2図は本発明実施例の構成説明図であり、
図中、第1図と同一記号は同一意味をもたせて使
用しここでの重複説明は省略する。また、送信ホ
ーン3と受信ホーン5の距離がl1であり、送信ホ
ーン7と受信ホーン8の距離がl2であり、且つ下
式(1)が成立するような位置に各送受信ホーン3,
5,7,8が配設されている。l3=l2−l1≒nλ±
λ/4(但し、n;自然数、λ;波長)………(1)
尚、第2図には図示しないが、各送受信ホーン
3,5,7,8を夫々上・下動させるための上下
動微調整機構が設けられることが多い。
Hereinafter, the present invention will be explained in detail using figures. FIG. 2 is an explanatory diagram of the configuration of an embodiment of the present invention,
In the figure, the same symbols as in FIG. 1 are used with the same meaning, and repeated explanation will be omitted here. Further, each transmitting/ receiving horn 3 ,
5, 7, and 8 are arranged. l 3 =l 2 −l 1 ≒nλ±
λ/4 (where n: natural number, λ: wavelength)……(1)
Although not shown in FIG. 2, a fine vertical adjustment mechanism is often provided for moving each transmitting/receiving horn 3, 5, 7, 8 up and down, respectively.

以下、上記構成からなる本発明実施例の動作に
ついて説明する。第2図において、発振器1から
送出されたマイクロ波は、アイソレータ2および
第1導波管4を経て送信ホーン3から被測定物9
に投射される。また、被測定物9を透過して水分
子による減衰を受けたマイクロ波は、受信ホーン
5で受信されてのち第2導波管6を経て送信ホー
ン7に至る。該マイクロ波は、送信ホーン7から
再び被測定物9に投射されて透過し、該被測定物
中の水分子によつて再度減衰される。その後、受
信ホーン8で受信され第3導波管10を経て、検
出部11で検出される。
The operation of the embodiment of the present invention having the above configuration will be described below. In FIG. 2, microwaves sent out from an oscillator 1 pass through an isolator 2 and a first waveguide 4, and then from a transmission horn 3 to an object under test 9.
is projected on. Furthermore, the microwaves transmitted through the object to be measured 9 and attenuated by water molecules are received by the receiving horn 5 and then reach the transmitting horn 7 via the second waveguide 6 . The microwave is projected again from the transmission horn 7 to the object to be measured 9 and transmitted therethrough, and is attenuated again by water molecules in the object to be measured. Thereafter, the signal is received by the reception horn 8, passes through the third waveguide 10, and is detected by the detection section 11.

ところで、第1図に示した従来例において、線
路に沿つた電圧波形は、波動方程式により下式(2)
のように導びかれる。
By the way, in the conventional example shown in Fig. 1, the voltage waveform along the line is expressed by the following equation (2) using the wave equation.
be guided as follows.

V=V+e-jx+ΓV+ejx ………(2) 但し、Γ;反射率、V+;電圧を表わす
サイン波の波高値、β;位相、
x;基準位置からの距離 上式(2)から電圧振幅|V|は下式(3)のように導
びかれる。
V=V + e -jx + ΓV + e jx ………(2) However, Γ: Reflectance, V + : Peak value of sine wave representing voltage, β: Phase,
x: Distance from the reference position From the above equation (2), the voltage amplitude |V| is derived as shown in the below equation (3).

|V|=|V+||(1+Γej2x/ejx| =|V+||1+Γej2x| =|V+|{(1+Γcos2βx)2+Γ2sin22βx}
1/2 =|V+|{(1+Γ)2−2Γ(1−
cos2βx)}1/2 =|V+|{(1+Γ)2−4Γsin2βx}1/2
………(3) 上式(3)から電圧振幅|V|の極大値|Vnax
と極小値|Vnio|を求め、それらの比をとると下
式(4)が得られる。
|V|=|V + ||(1+Γe j2x /e jx | =|V + ||1+Γe j2x | =|V + |{(1+Γcos2βx) 22 sin 2 2βx}
1/2 = |V + |{(1+Γ) 2 −2Γ(1−
cos2βx)} 1/2 = |V + |{(1+Γ) 2 −4Γsin 2 βx} 1/2
………(3) From the above formula (3), the maximum value of voltage amplitude |V| |V nax |
By finding the minimum value |V nio | and taking their ratio, the following equation (4) is obtained.

|Vnax|/|Vnio|=1+Γ/1−Γ ………(4) 一方、第2図に示した本発明実施例において
は、各送受信ホーン3,5,7,8が上式(1)を満
足するように配置されている。このため、線路に
沿つた電圧波形の振幅|V|として、上式(3)以外
に、上式(3)と位相がλ/4(即ち90゜)隔てられた部
分の信号である下式(5)も検出される。また、被測
定物9は厚紙などであり、各送受信ホーン3,
5,7,8に対しては平行移動するようにして動
く(即ち、各送受信ホーン3,5,7,8に対し
て第2図の紙面上で被測定物9が波うつことなく
平行移動するようにして上下方向に動く)。従つ
て、単に上式(3)と下式(5)の相加平均をとるだけで
導波管6等の距離差に基ずく位相変動を考慮する
ことができ、該平均値(即ち{(3)式+(5)式}/2)の 極大値|Vnax|と極小値|Vnio|を求めてのち、
それらの比をとると下式(6)が得られる。尚、定在
波分布を示す包絡線(図示せず)の谷から谷まで
の距離は1波長λでなく半波長(λ/2)となつ
ている。このため、送受信ホーン3,5間の定在
波と送受信ホーン7,8間の定在波との位相をπ
(即ち、λ/2)ずらしても線路に沿つた電圧波
形は増幅されるだけである。従つて、本願発明に
おいては、被測定物9のバタツキによつて発生し
た定在波の影響を除去するため、送受信ホーン
3,5間の定在波と送受信ホーン7,8間の定在
波との位相をπ/2(即ち、λ/4)ずらしてい
る。
|V nax |/|V nio |=1+Γ/1−Γ ......(4) On the other hand, in the embodiment of the present invention shown in FIG. It is arranged to satisfy 1). Therefore, as the amplitude |V| of the voltage waveform along the line, in addition to the above equation (3), the following equation is used, which is the signal of the part whose phase is separated from the above equation (3) by λ/4 (that is, 90 degrees). (5) is also detected. The object to be measured 9 is cardboard or the like, and each transmitting/receiving horn 3,
5, 7, and 8 (that is, the object to be measured 9 moves parallel to each transmitting/receiving horn 3, 5, 7, and 8 on the paper surface of FIG. 2 without wavering). (move up and down). Therefore, by simply taking the arithmetic average of the above equation (3) and the below equation (5), it is possible to consider the phase fluctuation based on the distance difference of the waveguide 6, etc., and the average value (i.e., {( After finding the maximum value |V nax | and the minimum value |V nio | of equation 3) + equation (5)}/2),
By taking their ratio, the following formula (6) is obtained. Note that the distance from trough to trough of the envelope (not shown) indicating the standing wave distribution is not one wavelength λ but half a wavelength (λ/2). Therefore, the phase of the standing wave between the transmitting and receiving horns 3 and 5 and the standing wave between the transmitting and receiving horns 7 and 8 is set to π
(ie, by λ/2), the voltage waveform along the line is only amplified. Therefore, in the present invention, in order to eliminate the influence of the standing waves generated by the fluttering of the object to be measured 9, the standing waves between the transmitting and receiving horns 3 and 5 and the standing waves between the transmitting and receiving horns 7 and 8 are removed. The phase is shifted by π/2 (that is, λ/4).

また、本願発明においては、被測定物9に接触
することなく被測定物中の水分量を測定すること
が必要であり、しかも、被測定物9は測定中にバ
タつく(上下動する)。従つて、送受信ホーン3,
8と被測定物9との距離をそれぞれ同一にした
り、送受信ホーン7,5と被測定物9との距離を
それぞれ同一にしたりすることは実際上困難であ
り、そのことが本願発明の必須の構成要件となる
ものでもない。
Furthermore, in the present invention, it is necessary to measure the amount of water in the object to be measured without contacting the object to be measured 9, and moreover, the object to be measured 9 flutters (moves up and down) during the measurement. Therefore, the transmitting/receiving horn 3,
In practice, it is difficult to make the distances between 8 and the object to be measured 9 the same, or to make the distances between the transmitting/receiving horns 7 and 5 and the object to be measured 9 the same, and this is an essential feature of the present invention. It is not a configuration requirement either.

更に、導波管4,6,10はマイクロ波水分計
の製造時に固定されるものであり、修理や現場で
の改造など例外的な場合を除き導波管4,6,1
0の位置は通常変動しないものである。仮に、被
測定物9の水分量測定中に導波管4,6,10の
位置が変動したとしても該変動量は極微少であ
り、被測定物9の水分量を測定する上で問題とな
るようなものではない。しかも、このような極微
少の位置変動はオフセツトとして生ずるにすぎ
ず、被測定物9の水分量を測定する上でノイズと
なり易い被測定物9のバタツキ(上下動)とは根
本的に異なるものである。従つて、導波管4,
6,10の位置変動(ひいては位相変動)は原則
として生じない。また、上述の如く例外的もしく
は極微少生ずる導波管4,6,10の位置変動
(ひいては位相変動)まで考慮して定在波にずれ
を生じさせる補償などを行う必要はない。
Furthermore, the waveguides 4, 6, and 10 are fixed during manufacturing of the microwave moisture meter, and the waveguides 4, 6, and 1 are fixed except in exceptional cases such as repair or on-site modification.
The position of 0 usually does not change. Even if the positions of the waveguides 4, 6, and 10 were to change during the measurement of the moisture content of the object to be measured 9, the amount of variation would be extremely small and would not pose a problem in measuring the moisture content of the object to be measured 9. It's not like that. Moreover, such minute positional fluctuations only occur as offsets, and are fundamentally different from the fluttering (vertical movement) of the object to be measured 9, which tends to become noise when measuring the moisture content of the object to be measured 9. It is. Therefore, the waveguide 4,
In principle, positional fluctuations (and thus phase fluctuations) of 6 and 10 do not occur. Further, as mentioned above, there is no need to take into consideration exceptional or minute positional fluctuations (and even phase fluctuations) of the waveguides 4, 6, and 10 to compensate for deviations in the standing waves.

|V|=|V+|{(1+Γ)2−4Γsin2(βx+
90゜)}1/2 =|V+|{(1+Γ)2−4Γcos2βx}1/2
………(5) 上式(4)および(6)において、0<Γ<1であるこ
とから、1+Γ/1−Γ>√1+2が成立する。また
、 上式(4)は前記従来例において被測定物9のパスラ
インが変化した場合の出力信号の振れ幅を示して
おり、上式(6)は本発明実施例において被測定物9
のパスラインが変化した場合の出力信号の振れ幅
を示している。即ち、線路に沿つた電圧波形(定
在波)の振幅は被測定物9のパスラインが変動し
た場合の出力信号と1対1に対応するため、電圧
振幅の極大値と極小値との比は被測定物9のパス
ラインが変動した場合の検出信号の振れ幅に対応
している。従つて、上式(4)と上式(6)の比較から、
第1図に示した従来例に比し第2図に示した本発
明実施例の方が被測定物9のパスライン特性がよ
いことが分る。
|V|=|V + |{(1+Γ) 2 −4Γsin 2 (βx+
90゜)} 1/2 =|V + |{(1+Γ) 2 −4Γcos 2 βx} 1/2
………(Five) In the above equations (4) and (6), since 0<Γ<1, 1+Γ/1-Γ>√1+ 2 holds true. In addition, the above equation (4) shows the amplitude of the output signal when the path line of the device under test 9 changes in the conventional example, and the above equation (6) shows the amplitude of the output signal when the path line of the device under test 9 changes in the embodiment of the present invention.
It shows the amplitude of the output signal when the path line changes. In other words, since the amplitude of the voltage waveform (standing wave) along the line corresponds one-to-one to the output signal when the path line of the device under test 9 fluctuates, the ratio between the maximum value and the minimum value of the voltage amplitude is corresponds to the amplitude of the detection signal when the path line of the object to be measured 9 changes. Therefore, from the comparison of the above equation (4) and the above equation (6),
It can be seen that the pass line characteristic of the object 9 to be measured is better in the embodiment of the present invention shown in FIG. 2 than in the conventional example shown in FIG.

第3図は上述の本発明実施例の効果を示すグラ
フであり、図中、縦軸は被測定物を通過したあと
の受信電圧変動を示しており、横軸は被測定物と
受信ホーンとの距離(即ち、被測定物のパスライ
ン)の変動を示している。第3図において、(イ)は
上記(3)式、(5)式、および(3)式+(5)式/2反射率Γが 0.1のときの値を示しており、(ロ)は反射率Γが0.2
のときの値を示している。第3図における上記(3)
式および(3)式+(5)式/2の夫々の特性曲線は、夫々 前記従来例および本発明実施例のパスライン特性
に相当する。従つて、これらを比較することによ
り、本発明実施例によれば被測定物9のパスライ
ン特性が大きく改善されることが分る。
FIG. 3 is a graph showing the effect of the above-described embodiment of the present invention. In the graph, the vertical axis shows the received voltage fluctuation after passing through the object to be measured, and the horizontal axis shows the variation in the received voltage after passing through the object to be measured and the receiving horn. (i.e., the path line of the object to be measured). In Figure 3, (a) shows the values when the above equations (3), (5), and (3) + equation (5)/2 reflectance Γ is 0.1, and (b) shows the values when the reflectance Γ is 0.1. Reflectance Γ is 0.2
It shows the value when . Above (3) in Figure 3
The characteristic curves of equation (3) + equation (5)/2 correspond to the pass line characteristics of the conventional example and the embodiment of the present invention, respectively. Therefore, by comparing these, it can be seen that according to the embodiment of the present invention, the pass line characteristics of the object to be measured 9 are greatly improved.

第4図は、本発明の他の実施例を示す構成説明
図であり、図中、第2図と同一記号は同一意味を
もたせて使用しここでの重複説明は省略する。ま
た、13は送信ホーン3と所定距離l2を隔てて配
置された受信ホーン、14は第2導波管6を介し
て受信ホーン13と接続された送信ホーン、15
は送信ホーン14と所定距離l1を隔てて配置され
た受信ホーン、16は第2導波管6と同様の第4
導波管19を介して受信ホーン15と接続された
送信ホーン、17は送信ホーン16と所定距離l2
を隔てて配置された受信ホーン、18は第2導波
管6と同様の第5導波管20を介して受信ホーン
17と接続された送信ホーンである。第3図にお
いて、発信器1から送出されたマイクロ波は、ア
イソレータ2→第1導波管4→送信ホーン3→被
測定物9を透過→受信ホーン13→第2導波管6
→送信ホーン14→被測定物9を透過→受信ホー
ン15→第4導波管19→送信ホーン16→被測
定物9を透過→受信ホーン17→第5導波管20
→送信ホーン18→被測定物19を透過→受信ホ
ーン8→第3導波管10を経て、検出部11で検
出される。また、検出部11の出力に基づき演算
部12内で施こされる演算処理により、第2図の
実施例の場合と同様にして被測定物9中の水分量
が求められる。尚、本発明は、第2図や第4図の
実施例に限定されるものではなく種々の変形が可
能であり、例えば第4図における送受信ホーンを
8個から12個に増やすなどしてもよい。また、本
願発明と同日付けで出願した特開昭59−197842号
公報記載の発明の原理となつている式と本願発明
の原理となつている式が一致しているが、両者に
おけるl1、l2の意味がそれぞれ異なつているため
両者は同一発明とはならないのである。
FIG. 4 is a configuration explanatory diagram showing another embodiment of the present invention. In the figure, the same symbols as in FIG. 2 are used with the same meanings, and redundant explanation will be omitted here. Further, 13 is a receiving horn arranged at a predetermined distance l2 from the transmitting horn 3, 14 is a transmitting horn connected to the receiving horn 13 via the second waveguide 6, and 15
16 is a receiving horn arranged at a predetermined distance l1 from the transmitting horn 14, and 16 is a fourth waveguide similar to the second waveguide 6.
A transmitting horn 17 is connected to the receiving horn 15 via a waveguide 19, and is connected to the transmitting horn 16 at a predetermined distance l 2
A receiving horn 18 is a transmitting horn connected to the receiving horn 17 via a fifth waveguide 20 similar to the second waveguide 6. In FIG. 3, the microwave transmitted from the transmitter 1 is transmitted through the isolator 2 → the first waveguide 4 → the transmitting horn 3 → the object to be measured 9 → the receiving horn 13 → the second waveguide 6.
→Transmission horn 14→Transmission through the object to be measured 9→Reception horn 15→Fourth waveguide 19→Transmission horn 16→Transmission through the object to be measured 9→Reception horn 17→Fifth waveguide 20
-> Transmission horn 18 -> Passes through the object to be measured 19 -> Receiving horn 8 -> Third waveguide 10 and is detected by the detection unit 11. Further, the amount of water in the object to be measured 9 is determined by arithmetic processing performed in the calculating section 12 based on the output of the detecting section 11 in the same manner as in the embodiment shown in FIG. Note that the present invention is not limited to the embodiments shown in FIGS. 2 and 4, and can be modified in various ways. For example, the number of transmitting/receiving horns in FIG. 4 may be increased from 8 to 12. good. Furthermore, although the formula serving as the principle of the invention described in JP-A-59-197842, which was filed on the same date as the present invention, and the formula serving as the principle of the present invention are the same, l 1 , Since the meanings of l 2 are different in each case, the two are not the same invention.

以上詳しく説明したような本発明の実施例によ
れば、上式(1)が成立するように各送受信ホーンを
配置するような構成であるため、前記実施例に比
して被測定物のばたつきによつて生ずる定在波の
影響を受けにくいという利点がある。また、所定
の可動部を設けて各送受信ホーンを機械的にλ/4
上下させることも考えられるが、このような方法
に比しても、本発明実施例によれば、可動部等の
故障を心配する必要がなく製品寿命が長いという
大きな利点がある。
According to the embodiment of the present invention as described in detail above, each transmitter/receiver horn is arranged so that the above formula (1) is satisfied, so that the fluctuation of the object to be measured is less than in the above embodiment. It has the advantage of being less susceptible to the effects of standing waves caused by In addition, a predetermined movable part is provided to mechanically move each transmitting and receiving horn to λ/4
Although it is conceivable to move the product up and down, the embodiment of the present invention has the great advantage that there is no need to worry about failure of movable parts, etc., and the product life is long, even compared to such a method.

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

第1図はマイクロ波水分計の従来例構成説明
図、第2図は本発明実施例の構成説明図、第3図
は本発明実施例使用の効果を示すグラフ、第4図
は本発明の他の実施例の構成説明図である。 1…発振器、2…アイソレータ、3,7,1
4,16,18…送信ホーン、5,9,13,1
5,17…受信ホーン、4,6,10,19,2
0…導波管、9…被測定物、11…検出部、12
…演算部。
Fig. 1 is an explanatory diagram of the configuration of a conventional microwave moisture meter, Fig. 2 is an explanatory diagram of the configuration of an embodiment of the present invention, Fig. 3 is a graph showing the effect of using the embodiment of the present invention, and Fig. 4 is an explanatory diagram of the configuration of the embodiment of the present invention. FIG. 7 is a configuration explanatory diagram of another embodiment. 1... Oscillator, 2... Isolator, 3, 7, 1
4, 16, 18... Transmission horn, 5, 9, 13, 1
5, 17...Reception horn, 4, 6, 10, 19, 2
0... Waveguide, 9... Measured object, 11... Detection section, 12
...Arithmetic section.

Claims (1)

【特許請求の範囲】 1 マイクロ波を使用して被測定物中の水分量を
測定するマイクロ波水分計において、発信器から
送出されるマイクロ波を被測定物に投射する第1
送信ホーンと、該被測定物を透過したマイクロ波
を受信する第1受信ホーンと、該第1受信ホーン
に接続されると共に前記被測定物に再度マイクロ
波を投射する第2送信ホーンと、該被測定物を透
過したマイクロ波を受信する第2受信ホーンとか
らなる2対の送・受信ホーンを数組具備し、前記
第1送・受信ホーンの間隔をl1とし、前記第2
送・受信ホーンの間隔をl2とするとき、l2−l1
nλ+λ/4(但し、n:自然数、λ;波長)が成立 するように、前記第1および第2の送・受信ホー
ンを配置することを特徴とするマイクロ波水分
計。 2 前記数組の送・受信ホーンは1組であること
を特徴とする特許請求範囲第1項記載のマイクロ
波水分計。 3 前記数組の送・受信ホーンは2組であること
を特徴とする特許請求範囲第1項記載のマイクロ
波水分計。
[Claims] 1. In a microwave moisture meter that uses microwaves to measure the amount of moisture in an object to be measured, a first device that projects microwaves sent from a transmitter onto the object to be measured
a transmitting horn, a first receiving horn that receives the microwaves transmitted through the object to be measured, a second transmitting horn that is connected to the first receiving horn and projects the microwaves again to the object to be measured; Several pairs of transmitting/receiving horns are provided, each consisting of a second receiving horn that receives the microwave transmitted through the object to be measured, the distance between the first transmitting/receiving horn being l 1 , and the second receiving horn receiving the microwave transmitted through the object to be measured.
When the distance between the transmitting and receiving horns is l 2 , l 2l 1
A microwave moisture meter characterized in that the first and second transmitting/receiving horns are arranged so that nλ+λ/4 (where n: natural number, λ: wavelength) holds. 2. The microwave moisture meter according to claim 1, wherein the several sets of transmitting/receiving horns are one set. 3. The microwave moisture meter according to claim 1, wherein the several sets of transmitting/receiving horns are two sets.
JP7353983A 1983-04-26 1983-04-26 Microwave moisture meter Granted JPS59197842A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7353983A JPS59197842A (en) 1983-04-26 1983-04-26 Microwave moisture meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7353983A JPS59197842A (en) 1983-04-26 1983-04-26 Microwave moisture meter

Publications (2)

Publication Number Publication Date
JPS59197842A JPS59197842A (en) 1984-11-09
JPH0136897B2 true JPH0136897B2 (en) 1989-08-03

Family

ID=13521135

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7353983A Granted JPS59197842A (en) 1983-04-26 1983-04-26 Microwave moisture meter

Country Status (1)

Country Link
JP (1) JPS59197842A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02205758A (en) * 1989-02-03 1990-08-15 Kawasaki Kiko Kk Method and apparatus for measuring moisture using microwave
EP0487582B1 (en) * 1989-08-15 2000-05-03 Commonwealth Scientific And Industrial Research Organisation Moisture content by microwave phase shift and mass/area
ATE192576T1 (en) * 1989-08-15 2000-05-15 Commw Scient Ind Res Org DETERMINATION OF MOISTURE CONTENT BY MICROWAVE PHASE SHIFT AND SURFACE DENSITY

Also Published As

Publication number Publication date
JPS59197842A (en) 1984-11-09

Similar Documents

Publication Publication Date Title
JPH0120375B2 (en)
US4452081A (en) Measurement of velocity and tissue temperature by ultrasound
CA2007190C (en) Laser optical ultrasound detection
US4650330A (en) Surface condition measurement apparatus
CA2500191A1 (en) Apparatus and method for microwave determination of at least one physical parameter of a substance
JPH06504126A (en) Moisture sensor for web that is not affected by temperature and its measurement method
US3913012A (en) Microwave moisture measuring system with reflection suppressing means
GB2046432A (en) Apparatus for determining the thickness moisture content or other parameter of a film or coating
JPH0136897B2 (en)
JPH0758178B2 (en) Ultrasonic seam detector
JPH0136898B2 (en)
JPH08285767A (en) Moisture meter
KR100448440B1 (en) Speed measurement apparatus and method of hot steel
JPS5972047A (en) Method for measuring moisture of powdered body
EP1055114A1 (en) Method and device for measuring the amount of coating on a moving substrate
US4790656A (en) Dual homodyne detection system to measure asymmetric spectrum by using angle mirrors
CN114910922B (en) Atmospheric refractive index compensation laser ranging device and method based on three-color laser
JPS6342357Y2 (en)
SU985752A1 (en) Device for sheet material reflection factor
SU1242781A1 (en) Method of detecting cracks in sheet dielectrics
JPS6069503A (en) Measuring method of shape of steel plate end part
SU643817A1 (en) Ice thickness measuring method
JPH0511498Y2 (en)
US20030132387A1 (en) Method and device for measuring the amount of coating on a moving substrate
SU934327A1 (en) Microwave flaw detector