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JPH076926B2 - Method and apparatus for measuring the amount of water contained in an object - Google Patents
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JPH076926B2 - Method and apparatus for measuring the amount of water contained in an object - Google Patents

Method and apparatus for measuring the amount of water contained in an object

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Publication number
JPH076926B2
JPH076926B2 JP1072163A JP7216389A JPH076926B2 JP H076926 B2 JPH076926 B2 JP H076926B2 JP 1072163 A JP1072163 A JP 1072163A JP 7216389 A JP7216389 A JP 7216389A JP H076926 B2 JPH076926 B2 JP H076926B2
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JP
Japan
Prior art keywords
amount
microwave
wave
measured
sensor
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 - Lifetime
Application number
JP1072163A
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Japanese (ja)
Other versions
JPH02249958A (en
Inventor
宏 東
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Individual
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Individual
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Priority to JP1072163A priority Critical patent/JPH076926B2/en
Publication of JPH02249958A publication Critical patent/JPH02249958A/en
Publication of JPH076926B2 publication Critical patent/JPH076926B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 発明の目的 本発明は物体中に含まれる水分量の計測方法及びその計
測装置に関する。物体には、木材等の吸湿性の固形物、
穀物等の粒状物、加工食品用の粉体物、あるいは織物、
紙等のシート状物等が含まれる。この被測定物体にマイ
クロ波を照射するとき、含まれている水分量に応じて反
射率及び透過率が変化する。本発明は、この中、反射率
が変化する現象を利用して汎用のマイクロ波ドップラセ
ンサを用いて簡便に水分量を計測する計測方法及びその
計測装置を提供することを目的とする。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring the amount of water contained in an object and a measuring apparatus therefor. For objects, hygroscopic solids such as wood,
Granules such as grains, powders for processed foods, or textiles,
Sheet-like materials such as paper are included. When the object to be measured is irradiated with microwaves, the reflectance and the transmittance change according to the amount of water contained. An object of the present invention is to provide a measuring method and a measuring device for easily measuring the water content by using a general-purpose microwave Doppler sensor by utilizing the phenomenon that the reflectance changes.

従来の技術及び解決しようとする問題点 従来、マイクロ波が物体を通過するとき、水分量に応じ
て減衰率すなわち透過率が変化するのを利用して水分量
を計測する方法がすでに実用化されている。
2. Description of the Related Art Conventional Techniques and Problems to Be Solved Conventionally, when microwaves pass through an object, a method of measuring the amount of water by utilizing the fact that the attenuation rate, that is, the transmittance changes according to the amount of water has already been put into practical use. ing.

第6図はその原理を図示したものである。FIG. 6 illustrates the principle.

(1)はマイクロ波発信器、(2)はマイクロ波受信器
であって、一定の間隔(S)を置いて互いに対向配置
し、その間に被測定物体(3)(以下、単に物体と云
う)を置く。発信器(1)より照射されたマイクロ波
(矢印A)は、物体(3)を通過するとき水分に吸収さ
れて減衰し受信器(2)に達する(矢印B)。この減衰
率は一定範囲内で水分量に比例して変化するから、これ
を測定すれば水分量を計測することができる。
(1) is a microwave transmitter, and (2) is a microwave receiver, which are arranged to face each other with a constant space (S) between them, and an object to be measured (3) (hereinafter, simply referred to as an object). ) Is put. The microwave (arrow A) emitted from the transmitter (1) is absorbed by water when passing through the object (3), is attenuated, and reaches the receiver (2) (arrow B). Since this attenuation rate changes in proportion to the water content within a certain range, the water content can be measured by measuring it.

しかしながら、この減衰率を的確に計測することはそれ
ほど簡単ではない。一般に汎用されている発信器と受信
器を用いた場合には、その間隔(S)を一定に保ち、物
体(3)はその間の特定位置に置かなければならない。
もし、物体(3)が少しでもずれたり、間隔(S)が変
化すれば、受信器から得られる受信信号(直流電圧)が
変動し、安定した計測が出来なくなる。これは、照射し
たマイクロ波の一部が物体(3)により反射され、更に
二次的な照射波(点線矢印C)となるが、この二次的な
照射波(C)は、物体(3)の位置により元の照射波
(A)に対して位相のずれが生じて、これらの照射合成
波(AとCの合成波)の強弱が変動し、従って、受信器
(2)の受信信号が変動するからである。また、透過し
たマイクロ波(矢印B)の二次的な反射波(点線矢印
D)も物体(3)の位置により位相のずれが生じ、複合
的に受信器の受信信号に影響を与える。このような変動
をなくするためには、上記の二次的な反射波(点線C及
びD)の影響を受けないように発信器及び受信器に特別
な工夫をこらす必要があり、その結果、特殊な設計の発
信器及び受信器となって、取り付け精度も要求され、高
価な据付式構造とならざるを得なくなっていた。
However, it is not so easy to measure this attenuation rate accurately. When a generally used transmitter and receiver are used, the space (S) must be kept constant and the object (3) must be placed at a specific position between them.
If the object (3) is slightly displaced or the interval (S) changes, the received signal (DC voltage) obtained from the receiver fluctuates, and stable measurement cannot be performed. This is because a part of the irradiated microwave is reflected by the object (3) and becomes a secondary irradiation wave (dotted arrow C). This secondary irradiation wave (C) is generated by the object (3). ), A phase shift occurs with respect to the original irradiation wave (A), and the strength of these irradiation combined waves (combined wave of A and C) fluctuates. Therefore, the reception signal of the receiver (2) is changed. Is fluctuating. Further, the secondary reflected wave (dotted arrow D) of the transmitted microwave (arrow B) also causes a phase shift depending on the position of the object (3), and affects the received signal of the receiver in a complex manner. In order to eliminate such fluctuation, it is necessary to devise a special device for the transmitter and the receiver so as not to be affected by the secondary reflected waves (dotted lines C and D), and as a result, The transmitters and receivers have a special design, and mounting precision is also required, and it is unavoidable that the installation structure is expensive.

このように、従来、実用化されているマイクロ波の透過
減衰率を利用した方式の水分量計測装置はいずれも使用
法に制限があった。例えば、固形物、粒状物、粉体物等
の場合は抜取られた少量の物しか測定できないとか、連
続計測ができないとか、高価であるにもかかわらず、設
置した場所でしか使用できないとかの制限があり、加工
工程中で連続的に計測しようとする場合において、需要
者の要求を満たすものではなかった。
As described above, the water content measuring devices that have been practically used in the past and that utilize the transmission attenuation factor of microwaves are limited in usage. For example, in the case of solids, granules, powders, etc., it is possible to measure only a small amount of extracted substances, continuous measurement is not possible, or it is expensive but it can only be used at the place where it is installed. However, in the case of continuously measuring in the processing process, it did not meet the demand of the consumer.

一方、マイクロ波の反射波を利用した水分計が市販され
ているのを未だ見聞していないが、水分量により反射波
が変化するのを利用して水分量を検出する方式の水分計
測技術について開示した文献はある。(例、特開昭59-8
7346公報など) マイクロ波ドップラセンサ[第1図に示すようにマイク
ロ波発信器(1)と受信器(2)を一体に組込み、発信
器(1)からのマイクロ波を導波管内で直接に受ける自
己発信波と物体からの反射波(C)との合成波を受信器
(2)で受信し、これを検波(整流し平滑化すること)
して受信信号(直流検出電圧)(V)を得るセンサ]を
用いた方式の場合は、センサの形状寸法、センサと被検
出物体との距離、水分量の多寡などにより、受信器
(2)の位置で自己発信波と反射波(C)との位相のず
れが変化するため、これらの合成波の強さ(振幅)が変
動する。従って、受信器(2)の受信信号(検出電圧)
(V)は必ずしも反射波の強さに対応するものとは限ら
ず、むしろ、形状寸法、距離などの位置関係の影響を受
ける度合いが強くなる。このように、反射波が物体の水
分量に対応したものであっても、受信信号(V)は必ず
しも定まった値とはならず、水分量の検出は想定してい
るほど容易ではない。
On the other hand, we have not yet seen that moisture meters that use reflected waves of microwaves are on the market, but we are not aware of moisture measurement technology that uses the change in reflected waves depending on the amount of moisture to detect the amount of moisture. There are references disclosed. (For example, JP-A-59-8
7346, etc.) Microwave Doppler sensor [As shown in FIG. 1, the microwave transmitter (1) and the receiver (2) are integrated into one body, and the microwave from the transmitter (1) is directly introduced in the waveguide. The composite wave of the self-generated wave received and the reflected wave (C) from the object is received by the receiver (2) and detected (rectified and smoothed).
In the case of a system using a sensor to obtain a received signal (DC detection voltage) (V)], the receiver (2) may vary depending on the shape and size of the sensor, the distance between the sensor and the object to be detected, and the amount of water content. Since the phase shift between the self-generated wave and the reflected wave (C) changes at the position of, the intensity (amplitude) of these combined waves changes. Therefore, the reception signal (detection voltage) of the receiver (2)
(V) does not necessarily correspond to the strength of the reflected wave, but rather, the degree of being affected by the positional relationship such as the shape size and the distance becomes stronger. Thus, even if the reflected wave corresponds to the water content of the object, the received signal (V) does not always have a fixed value, and the detection of the water content is not as easy as expected.

従来開示された反射波利用の水分計測技術は、上記のよ
うなドップラセンサの受信原理についての考察が欠落し
ているものの他、反射波が水分量に応じて減少するとい
う誤解(実際は、反射波は水分量にほゞ比例して増大す
る。)に基づいてなされているものなどであって、一般
的に正確な水分量の検出が期待できるものではなかっ
た。
The previously disclosed moisture measurement technology using reflected waves lacks the consideration of the receiving principle of the Doppler sensor as described above, and the misunderstanding that reflected waves decrease according to the amount of moisture (actually, reflected waves Is increased based on the amount of water, which is generally proportional to the amount of water.) However, in general, accurate detection of the amount of water could not be expected.

反射波を利用する場合には、上記のように物体(3)の
位置による反射波の位相のずれの影響は必然の現象であ
り、これを解消する方式が未だ未解決であったからであ
る。
This is because, when the reflected wave is used, the influence of the phase shift of the reflected wave due to the position of the object (3) is an inevitable phenomenon as described above, and a method for eliminating this is still unsolved.

このような上記従来の欠点と問題点に鑑みて、本発明
は、一般に汎用されているマイクロ波発信器及び受信器
を一体に組み込んだマイクロ波ドップラセンサを用い
て、簡便に物体中に含まれる水分量を計測することが出
来るように、反射率の変化と上記不安定要因となってい
た反射波の位相のずれとの関係を逆に巧みに利用したも
のであって、これにより、便利な計測方法及び計測装置
を提供し、需要者の要望に応えようとするものである。
In view of the above-mentioned conventional drawbacks and problems, the present invention uses a microwave Doppler sensor integrally incorporating a generally-used microwave transmitter and receiver, and is easily included in an object. In order to be able to measure the amount of water, the relationship between the change in reflectance and the phase shift of the reflected wave, which has been the cause of the above instability, has been skillfully utilized in reverse, which makes it convenient. It is intended to provide a measuring method and a measuring device to meet the demand of consumers.

発明の構成及び作用 以下に、本発明の実施例について図面を参照して詳述す
る。
Configuration and Action of the Invention Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.

その前に栄5、マイクロ波発信器とマイクロ波受信器を
一体に組み込んだマイクロ波ドップラセンサを用いた場
合における、物体からのマイクロ波の反射波と受信信号
(V)との関係を第1図および第2図を参照して述べ
る。
Prior to that, Sakae 5, the relationship between the reflected wave of the microwave from the object and the received signal (V) when the microwave Doppler sensor in which the microwave transmitter and the microwave receiver are integrated is used. It will be described with reference to FIGS.

第1図において、ドップラセンサ(4)は発信器(1)
と受信器(2)を一体に構成したものであって、導波管
(5)内に発信器(1)としてガンダイオード、受信器
(2)としてミキサダイオードを一体に内蔵している。
発信器(1)の入力端子(14)に適当な電圧(たとえ
ば、DC 8V)を印加すると、発信器(1)からマイクロ
波が導波管(5)を経てホーンアンテナ(6)により発
受信面(7)(必ずしも実体面である必要はなく、実体
のない仮想面と考えてもよい。)から一定の方向に発信
される(矢印A)。物体(3)により反射されたマイク
ロ波(矢印C)は発受信面(7)からホーンアンテナ
(6)により収束されて受信器(2)で受信される。受
信器(2)は自己発信波「発信器(1)から発信された
マイクロ波が導波管(5)内で直接に受信器(2)に達
する発信波。以下同じ]と物体からの反射波との合成波
を受信し、これを検波してその振幅に比例した受信信号
(直流検出電圧)(V)を出力する。センサ(4)から
の受信信号は増幅器(8)、A/D変換器(9)を経てデ
ジタル値として演算器(10)へ読み込まれ、内蔵のメモ
リ(11)にデータとして記憶される。増幅器(8)、A/
D変換器(9)、演算器(10)、メモリ(11)及び表示
器(12)は全体として処理器(13)を構成する。演算器
(10)にはマイクロコンピュータを組み込み、データの
値の読み取りとその変動値の変化分の演算処理を行な
い、その結果を表示器(12)に表示する。
In FIG. 1, the Doppler sensor (4) is a transmitter (1).
And a receiver (2) are integrated, and a Gunn diode as a transmitter (1) and a mixer diode as a receiver (2) are integrated in a waveguide (5).
When an appropriate voltage (eg, DC 8V) is applied to the input terminal (14) of the oscillator (1), microwaves are transmitted and received from the oscillator (1) through the waveguide (5) and the horn antenna (6). It is transmitted in a certain direction from the surface (7) (it does not necessarily have to be a physical surface and may be considered as a virtual surface without a physical body) (arrow A). The microwave (arrow C) reflected by the object (3) is converged from the emitting / receiving surface (7) by the horn antenna (6) and received by the receiver (2). The receiver (2) is a self-transmitted wave "a microwave emitted from the transmitter (1) directly reaches the receiver (2) in the waveguide (5). The same applies below." The combined wave with the wave is received, this is detected, and the received signal (DC detection voltage) (V) proportional to its amplitude is output.The received signal from the sensor (4) is the amplifier (8), A / D It is read as a digital value into the arithmetic unit (10) through the converter (9) and stored as data in the built-in memory (11).
The D converter (9), the arithmetic unit (10), the memory (11) and the display unit (12) constitute a processor (13) as a whole. A microcomputer is incorporated in the arithmetic unit (10) to read the data value and perform arithmetic processing for the change in the variation value, and display the result on the display unit (12).

物体(3)の表面はセンサ(4)のホーンアンテナ
(6)の発受信面(7)より距離(X)の間隔をおいて
いる。
The surface of the object (3) is spaced from the emitting / receiving surface (7) of the horn antenna (6) of the sensor (4) by a distance (X).

物体(3)が完全に乾燥したものである場合には、照射
されたマイクロ波は物体特有の反射を除きほとんど反射
されず吸収されるかまたは透過してしまう(点線矢印
B)。このとき、受信器(2)は自己発信波によって励
振され、これを検波して一定の基準信号(直流電圧)
(V0)を出力している。(第2図のグラフの直線(E)
を参照。)この値は発信器(1)の照射マイクロ波の強
さ(出力)、導波管(5)の寸法、受信器(2)の性能
等によって定まる。但し、物体によっては、僅かながら
特有の反射があるから、若干変動することがある。
When the object (3) is completely dry, the irradiated microwaves are hardly reflected except the reflection peculiar to the object and are absorbed or transmitted (dotted line arrow B). At this time, the receiver (2) is excited by the self-oscillation wave, and this is detected to detect a constant reference signal (DC voltage).
(V 0 ) is being output. (Straight line (E) in the graph of Figure 2
See. ) This value is determined by the intensity (output) of the irradiation microwave of the transmitter (1), the size of the waveguide (5), the performance of the receiver (2) and the like. However, depending on the object, there may be a slight reflection, which may cause a slight variation.

物体(3)が水分を含んでいるときは物体の誘電率が水
分量にほゞ比例して大きくなる。このため、照射された
マイクロ波は一部が物体(3)の表面および表面の浅い
層で反射され(矢印C)、深い部分では吸収されてしま
う。この反射波により受信器(2)は自己発信波と反射
波の合成波で励振される。この反射波は一定の範囲内で
物体の表層部分に含まれる水分量にほぼ比例して強くな
る。誘電率の異なる物質間の境界層に於けるマイクロ波
の反射率は誘電率の違いの大きいほど大きくなるからで
ある。
When the object (3) contains water, the dielectric constant of the object increases in proportion to the amount of water. Therefore, a part of the irradiated microwave is reflected by the surface of the object (3) and the shallow layer of the surface (arrow C), and is absorbed in the deep part. Due to this reflected wave, the receiver (2) is excited by a composite wave of the self-generated wave and the reflected wave. This reflected wave becomes strong in proportion to the amount of water contained in the surface layer of the object within a certain range. This is because the microwave reflectance in the boundary layer between substances having different permittivities increases as the difference in permittivity increases.

自己発信波は距離(X)に関係なく受信器(2)に一定
の強さで達するが、反射波は距離(X)により自己発信
波に対して位相のずれが変化するため、受信器(2)の
検出部で自己発信波と反射波とが共鳴して(同じ位相と
なって)合成波が強まる位置と、打消されて(逆の位相
となって)合成波が弱まる位置とがある。従って、受信
器(2)からの受信信号(V)は距離(X)により高く
なったり低くなったりする。
The self-transmitted wave reaches the receiver (2) with a constant intensity regardless of the distance (X), but the reflected wave changes in phase with respect to the self-transmitted wave depending on the distance (X). In the detection unit of 2), there are a position where the self-transmitted wave and the reflected wave resonate (become in the same phase) to strengthen the composite wave, and a position where they are canceled (become the opposite phase) to weaken the composite wave. . Therefore, the received signal (V) from the receiver (2) becomes higher or lower depending on the distance (X).

この関係の一例をグラフで示したのが第2図の波形曲線
(F)である。縦軸に受信器(2)からの受信信号(直
流電圧)(V)、横軸に距離(X)をとる。グラフの波
形曲線(F)の山部(M1、M3・・)が共鳴部(自己発信
波と反射波とが同じ位相となる位置)、谷部(M2、M4
・)が打消部(逆の位相となる位置)である。距離
(X)が大きくなると反射波の捕捉率が低下して曲線
(F)の振幅は次第に減衰する。なお、この曲線の二周
期分の長さ(L)が原理的にマイクロ波の波長と一致す
る。
An example of this relationship is shown in the graph as the waveform curve (F) in FIG. The vertical axis represents the received signal (DC voltage) (V) from the receiver (2), and the horizontal axis represents the distance (X). The peaks (M 1 , M 3 ··) of the waveform curve (F) in the graph are the resonance part (the position where the self-generated wave and the reflected wave have the same phase) and the valleys (M 2 , M 4 ·).
・) Is the canceling portion (position with opposite phase). As the distance (X) increases, the capture rate of the reflected wave decreases and the amplitude of the curve (F) gradually decreases. In addition, the length (L) of two cycles of this curve agrees with the wavelength of the microwave in principle.

この波形曲線(F)の隣接する山部と谷部の振幅は反射
波の強さに比例し、また、基準信号(V0)にも比例して
大きくなる。つまり基準信号(V0)と反射率の積にほぼ
比例して大きくなるが、水分量が多くなると反射波もほ
ゞ比例して高くなるから、この振幅も水分量にほゞ比例
して大きくなる。
The amplitudes of the adjacent peaks and valleys of this waveform curve (F) are proportional to the intensity of the reflected wave and also to the reference signal (V 0 ). In other words, it increases almost in proportion to the product of the reference signal (V 0 ) and the reflectance, but when the amount of water increases, the reflected wave also increases almost in proportion, so this amplitude also increases almost in proportion to the amount of water. Become.

直線(E)は自己発信波のみによって受信器(2)が励
振されて出力する基準信号(電圧)(V0)を示し、距離
(X)とは無関係である。
The straight line (E) shows the reference signal (voltage) (V 0 ) output by the receiver (2) being excited only by the self-generated wave, and is independent of the distance (X).

従って、例えば、一定の距離の位置(M1)で受信信号を
測定して得られる値(V1)と基準信号(V0)の差(ΔV
=V1−V0)を計算すれば、この値を水分量のパラメータ
(Y)とすることができる。基準信号(V0)は発信出
力、温度、受信器の性能等の影響をうけるから、(Y=
ΔV/V0)の値の方が安定したパラメータとなる。
Therefore, for example, the difference (ΔV) between the value (V 1 ) obtained by measuring the received signal at the position (M 1 ) at a constant distance and the reference signal (V 0 ).
If = V 1 -V 0) calculate, it is possible to this value and water content of the parameter (Y). Since the reference signal (V 0 ) is affected by the transmission output, temperature, receiver performance, etc., (Y =
The value of ΔV / V 0 ) is a more stable parameter.

測定位置は一定の距離の位置(M1)が最も効果的である
が、位置(M2)、(M3)・・でもよい。
The measurement position is most effective at a position at a fixed distance (M 1 ), but it may be at positions (M 2 ), (M 3 ) ...

(第2図参照) しかしながら、非接触方式による連続測定の場合には距
離(X)がどうしても変動しやすく、一定の位置に保つ
のは困難である。例えば、第2図に示すように、距離
(X)が位置(M1)から(ΔX)だけ揺れると、受信信
号(V)が(ΔV)だけふらついて安定した計測ができ
ない。
(See FIG. 2) However, in the case of continuous measurement by the non-contact method, the distance (X) is apt to fluctuate and it is difficult to keep it at a constant position. For example, as shown in FIG. 2, when the distance (X) fluctuates from the position (M 1 ) by (ΔX), the received signal (V) fluctuates by (ΔV) and stable measurement cannot be performed.

このように、たとえ被測定物体の水分量が一定で反射波
の強さが一定であっても、受信信号(V)は距離(X)
によって大きく変化し、水分量に対応した値にはならな
いことが分かる。
Thus, even if the water content of the object to be measured is constant and the intensity of the reflected wave is constant, the received signal (V) is equal to the distance (X).
It can be seen that the value does not correspond to the water content due to the large change.

この問題を解決し、非接触方式でも連続計測できるよう
にしたのがこの実施例である。
This embodiment solves this problem and enables continuous measurement even in the non-contact method.

第1図において、ドップラセンサ(4)を物体(3)の
表面に対して垂直に周期的に強制的に往復揺動させてみ
る。揺動の振幅は照射マイクロ波の波長の二分の一以上
とし、揺動範囲は、第2図において、例えば位置
(M1)、(M2)を含むような範囲(R)となるようにす
る。具体的には、発信周波数10.525GHzのマイクロ波を
用いた場合には、振幅は20mmあればよい。
In FIG. 1, the Doppler sensor (4) is forcibly reciprocally oscillated periodically perpendicularly to the surface of the object (3). The amplitude of the oscillation is set to ½ or more of the wavelength of the irradiation microwave, and the oscillation range is set to the range (R) including the positions (M 1 ) and (M 2 ) in FIG. 2, for example. To do. Specifically, when a microwave having an oscillation frequency of 10.525 GHz is used, the amplitude may be 20 mm.

センサ(4)が揺動している間に、受信器(2)からの
受信信号(V)を増幅器(8)、A/D変換器(9)を介
して極く短い時間間隔でサンプリングして刻々と演算器
(10)に読取り、多数のデータとしてメモリ(11)に記
憶させる。一周期(T0)の間にサンプリングした多数の
データとオシロスコープで得られる波形を重ね合わせた
のが第3図の波形曲線(G)である。黒点がサンプリン
グした多数のデータの軌跡、実線がオシロスコープで得
られる波形曲線(G)である。この波形曲線(G)はセ
ンサが一往復揺動する間に、第2図の受信信号(V)の
波形を一定の範囲(R)の間でトレースした形で得られ
るから、時刻(T1)、(T4)の受信信号の値(V1)は、
第2図の位置(M1)を通過した時点の値(V1)と一致
し、時刻(T2)、(T3)の受信信号の値(V2)は位置
(M2)を通過した時点の値(V2)と一致する。サンプリ
ングの時間間隔を充分に短くすれば、このサンプリング
したデータの最大値は値(V1)、最小値は値(V2)とみ
なしてよい。そして、この差(ΔV=V1−V2)は反射波
の強さに比例し、従って、水分量にほゞ比例した値とな
るから、これを物体中に含まれる水分量のパラメータ
(Y)とすることができる。
While the sensor (4) is swinging, the received signal (V) from the receiver (2) is sampled at very short time intervals via the amplifier (8) and the A / D converter (9). It is read every second by the arithmetic unit (10) and stored in the memory (11) as a large amount of data. The waveform curve (G) in FIG. 3 is obtained by superimposing a large number of data sampled during one period (T 0 ) and the waveform obtained by the oscilloscope. The black dots are the loci of many sampled data, and the solid line is the waveform curve (G) obtained with an oscilloscope. Since this waveform curve (G) is obtained by tracing the waveform of the reception signal (V) in FIG. 2 within a certain range (R) while the sensor makes one reciprocating oscillation, the time (T 1 ), (T 4 ) received signal value (V 1 ) is
It matches the value (V 1 ) at the time of passing the position (M 1 ) in Fig. 2 , and the value (V 2 ) of the received signal at time (T 2 ) and (T 3 ) passes through the position (M 2 ). It agrees with the value (V 2 ) at the time of doing. If the sampling time interval is sufficiently short, the maximum value of this sampled data may be regarded as the value (V 1 ) and the minimum value thereof may be regarded as the value (V 2 ). Then, this difference (ΔV = V 1 −V 2 ) is proportional to the intensity of the reflected wave, and therefore has a value almost proportional to the amount of water, so that this is a parameter of the amount of water contained in the object (Y ) Can be.

最大値と最小値の和(ΣV=V1+V2)は基準信号(V0
にほゞ比例するから、 Y=ΔV/ΣV ・・・・・(30) を求めると、より安定したパラメータ(Y)を得ること
ができる。
The sum of the maximum and minimum values (ΣV = V 1 + V 2 ) is the reference signal (V 0 ).
Since it is almost proportional to Y = ΔV / ΣV (30), a more stable parameter (Y) can be obtained.

パラメータとしては、この他に測定データの微分値ある
いは積分値を演算して得ることもできる。
In addition to this, the parameter may be obtained by calculating a differential value or an integrated value of the measurement data.

このように、マイクロ波センサを周期的に一定の範囲内
で強制的に往復揺動させ、その間にサンプリングした多
数の受信信号のデータの変動値の一周期の間の変化分を
パラメータとすることによって水分量を一周期に一回づ
つ計測することができる。
In this way, the microwave sensor is forcibly reciprocally oscillated within a certain range periodically, and the variation of the variation value of the data of many received signals sampled during that period is used as a parameter. With this, the water content can be measured once per cycle.

この場合、センサを固定し、物体を揺動させても同様の
計測ができる。
In this case, the same measurement can be performed by fixing the sensor and swinging the object.

なお、往復揺動する一周期とその間にサンプリングした
多数のデータを演算処理する時間はコンピュータの演算
速度にもよるが、通常は1秒以内に充分に納まるから、
水分計測の結果を表示する周期は観測者からみれば充分
に短く、実質的には連続的に計測しているものとみなし
うる。
It should be noted that, although one cycle of reciprocating oscillation and the time required to process a large number of data sampled during that period depend on the operation speed of the computer, normally it is sufficiently within one second.
From the observer's point of view, the cycle for displaying the results of moisture measurement is sufficiently short, and it can be considered that the measurement is substantially continuous.

本実施例においては、第2図の位置(M1)、(M2)を含
むようにセンサ(4)の揺動範囲を選びさえすれば、物
体あるいはセンサの多少の揺れや傾きには影響されず、
非接触方式で水分量を連続計測できるところに大きな利
点がある。
In this embodiment, if the swing range of the sensor (4) is selected so as to include the positions (M 1 ) and (M 2 ) shown in FIG. not,
There is a great advantage in that the water content can be continuously measured by the non-contact method.

上記においては、変動値の変化分としてデータの最大値
と最小値を用いたが、これに限ることなく、微分値、積
分値等の電気的に検出できる値を用いることもできる。
例えば、コンデンサと整流器を組み合わせた検波器によ
りアナログ値として検出してもよい。
In the above, the maximum value and the minimum value of the data are used as the variation of the variation value, but the invention is not limited to this, and a value that can be detected electrically such as a differential value or an integrated value may be used.
For example, a detector combining a capacitor and a rectifier may detect the analog value.

第4図は本発明実施の計測装置の一例を示したものであ
って、センサ(4)を収納した箱(15)はロッド(16)
の先端に固定され、ロッドの根元は揺動装置(17)に連
結されている。揺動装置(17)は内蔵のモータ及びクラ
ンク機構(図示せず)によりロッドの軸方向にセンサ箱
(15)を一定周期で一定範囲内で強制的に往復揺動する
ように構成されている。制御箱(19)内には電源(20)
と処理器(13)が納められ、電源(20)はモータと処理
器(13)に接続し、処理器(13)はセンサ(4)に揺動
装置(17)、ロッド(16)を介して接続している。
FIG. 4 shows an example of a measuring device embodying the present invention. The box (15) accommodating the sensor (4) is a rod (16).
Is fixed to the tip of the rod, and the root of the rod is connected to the rocking device (17). The oscillating device (17) is configured to forcibly oscillate the sensor box (15) in the axial direction of the rod within a fixed range in a fixed range by a built-in motor and a crank mechanism (not shown). . Power supply (20) in the control box (19)
And the processor (13) are housed, the power source (20) is connected to the motor and the processor (13), and the processor (13) is connected to the sensor (4) via the rocking device (17) and the rod (16). Connected.

センサ(4)が揺動している間に得られる受信信号は処
理器(13)内の増幅器、A/D変換器を経てデジタル値と
して演算器へ極く短い時間間隔でサンプリングされて刻
々と読み込まれ、内蔵のメモリにデータとして記憶され
る。演算器はサンプリングされた多数のデータの変動値
の一周期の間の変化分の演算処理を行ない、その結果を
表示器(12)に表示する。例えば、一周期(T0)内のデ
ータの最大値(V1)と最小値(V2)の差(Y=ΔV=V1
−V2)に一定の係数(α)を掛けた値(α・ΔV)を、
計測した水分量の値として表示器(12)に表示する。あ
るいは、最大値と最小値の差(ΔV)と和(ΣV=V1
V2)の比(Y=ΔV/ΣV)を表示する。
The received signal obtained while the sensor (4) is oscillating is sampled at a very short time interval as a digital value through the amplifier and A / D converter in the processor (13) and is sampled every second. It is read and stored as data in the built-in memory. The arithmetic unit performs the arithmetic processing of the variation of the variation values of a large number of sampled data during one cycle, and displays the result on the display (12). For example, the difference (Y = ΔV = V 1 ) between the maximum value (V 1 ) and the minimum value (V 2 ) of data in one cycle (T 0 ).
-V 2 ) multiplied by a constant coefficient (α) (α · ΔV),
The value of the measured water content is displayed on the display (12). Alternatively, the difference (ΔV) between the maximum value and the minimum value and the sum (ΣV = V 1 +
The ratio of V 2 ) (Y = ΔV / ΣV) is displayed.

このように構成された装置を用いれば、物体(3)の表
面にセンサ箱(15)を近ずけて揺動装置(17)を設置す
ることにより、非接触方式で水分量を連続計測すること
ができる。この際、多少の物体の揺れや傾きが許容され
るのは前述のとうりである。
By using the device configured as described above, the water content can be continuously measured in a non-contact manner by installing the rocking device (17) on the surface of the object (3) so that the sensor box (15) is close to the sensor box (15). be able to. At this time, it is the same as described above that some shaking and tilting of the object is allowed.

上記の実施例に示されたパラメータ(Y)に一定の係数
(α)または(β)を掛けた値は物体の表層部分(数mm
以内の深さまで)に含まれる水分量を表わすものである
が、水分が均一に分散している場合には、物体全体に含
まれる水分量(単位体積当りの水分重量)(W)を代表
しているものとみなすことができる。このパラメータ
(Y)と水分量(W)の関係は、物体の素材、水分に含
まれる溶剤の性質によって変わり、必ずしも一定には定
まらない。一例として、(30)式の(Y)と(W)の関
係を一般的にグラフで示したのが第5図である。3本の
検量線は異なった物体の素材について異なった傾きにな
ることを示している。なお、水分量の高い範囲では受信
信号(V)が飽和するから、比例しなくなることを示
す。
The value obtained by multiplying the parameter (Y) shown in the above embodiment by a constant coefficient (α) or (β) is the surface layer part of the object (several mm
It represents the amount of water contained in the whole body, but when the water is uniformly dispersed, it represents the amount of water contained in the whole object (weight of water per unit volume) (W). Can be regarded as The relationship between the parameter (Y) and the water content (W) varies depending on the material of the object and the property of the solvent contained in the water, and is not always fixed. As an example, FIG. 5 is a graph showing the relationship between (Y) and (W) in the equation (30). The three calibration curves show different slopes for different material materials. It should be noted that the received signal (V) is saturated in a range where the amount of water is high, so that it is not proportional.

従って、正確な水分量(W)の絶対値を計測するために
は、物体の素材、密度及び溶解液の薬品の性質等につい
て補正を加え、直線化するために、 W=f(Y) なる関数補正をしなければならない。
Therefore, in order to accurately measure the absolute value of the water content (W), W = f (Y) is set in order to correct the material and density of the object and the property of the chemicals of the solution and to make it linear. Function correction must be done.

なお、上記の水分量を決定する係数(α)、(β)、関
数f(Y)は、マイクロ波ドップラセンサの性能が定ま
り、物体の材質、水溶液の性質等の対象物が定まれば、
表示する水分量の単位を決めて実験的に得られる検量線
から求められる。
It should be noted that the coefficients (α), (β), and the function f (Y) that determine the amount of water are determined by the performance of the microwave Doppler sensor, and when the target material such as the material of the object and the property of the aqueous solution is determined.
It is determined from a calibration curve obtained experimentally by determining the unit of water content to be displayed.

発明の効果 以上、詳述したように、本発明によれば、センサを構成
するマイクロ波発信器及び受信器は一般に汎用されてい
るマイクロ波ドップラセンサをそのまゝ使用し、従来の
方法では計測を阻害していた不安定な要因(自己発信波
と反射波との位相のずれ)を逆に巧みに利用することに
よって、簡便に物体に含まれる水分量を連続計測するこ
とが可能となる。従って、加工工程中で移動している物
体に対しても非接触状態で連続的に計測できる水分量の
計測装置を得ることができる。
Effects of the Invention As described above in detail, according to the present invention, the microwave transmitter and the receiver that constitute the sensor use the microwave Doppler sensor that is generally used as it is, and the measurement is performed by the conventional method. By reversely skillfully utilizing the unstable factor (phase shift between the self-transmitted wave and the reflected wave) that has hindered the above, it becomes possible to easily and continuously measure the amount of water contained in the object. Therefore, it is possible to obtain a water content measuring device capable of continuously measuring an object that is moving during a processing step in a non-contact state.

また、特別な工夫をこらした高価なマイクロ波発信器お
よび受信器を用いる必要もなく、取付精度も厳しく要求
されることはないから、安価で便利な計測装置を提供で
きることになる。
Further, since it is not necessary to use an expensive microwave transmitter and receiver which are specially devised, and the mounting accuracy is not strictly required, it is possible to provide an inexpensive and convenient measuring device.

更に、非接触方式で計測可能としているから、移動中の
物体であっても接触痕をつけたり痛めたりすることはな
い。
Further, since the measurement can be performed by the non-contact method, even a moving object does not make a contact mark or hurt.

このように、本発明は従来にないきわめて有益な効果を
もたらすものである。
As described above, the present invention brings about an extremely beneficial effect which has never been obtained.

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

図面は本発明による水分量の計測方法及びその計測装置
の実施例を示したもので、第1図はマイクロ波ドップラ
センサを用いた場合の構成図、第2図は被測定物体とセ
ンサ間の距離(X)とその受信信号(直流電圧)との関
係を示すグラフ、第3図はその受信信号と時間との関係
を示すグラフ、第4図は計測装置の一例を示す図面、第
5図はパラメータと実際の水分量との関係を示すグラ
フ、第6図は従来の水分量の計測方法を示す図面であ
る。 (1)……マイクロ波発信器(ガンダイオード) (2)……マイクロ波受信器(ミキサダイオード) (3)……被測定物体 (4)……マイクロ波ドップラセンサ (8)……増幅器、(9)……A/D変換器 (10)……演算器、(11)……メモリ (12)……表示器、(13)……処理器 (17)……揺動装置
The drawings show an embodiment of a method for measuring the amount of water and a measuring apparatus therefor according to the present invention. FIG. 1 is a configuration diagram when a microwave Doppler sensor is used, and FIG. A graph showing the relationship between the distance (X) and its reception signal (DC voltage), FIG. 3 is a graph showing the relationship between the reception signal and time, FIG. 4 is a drawing showing an example of a measuring device, FIG. Is a graph showing the relationship between the parameter and the actual water content, and FIG. 6 is a drawing showing a conventional method for measuring the water content. (1) …… Microwave transmitter (Gun diode) (2) …… Microwave receiver (mixer diode) (3) …… Measured object (4) …… Microwave Doppler sensor (8) …… Amplifier, (9) …… A / D converter (10) …… Computer, (11) …… Memory (12) …… Display, (13) …… Processor (17) …… Rotating device

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】マイクロ波発信器(1)とマイクロ波受信
器(2)を一体に備えて一つの発受信面からマイクロ波
の発信及び受信をするマイクロ波ドップラセンサ(4)
を、被測定物体の表面に向けて近づけ、該センサ(4)
の発受信面と該物体の表面との相対距離(X)を周期的
に強制的に往復変動させ、その間に、被測定物体からの
反射波と自己発信波との合成波を受信した前記受信器
(2)がこれを検波して出力する受信信号(V)の値を
極く短い時間間隔で処理器(13)に刻々と読み込み、そ
の読み込まれた多数のデータから得られる変動値の往復
一周期の間の変化分をパラメータとして、被測定物体中
に含まれる水分量を計測するようにしたことを特徴とす
る物体中に含まれる水分量の計測方法。
1. A microwave Doppler sensor (4) which integrally includes a microwave transmitter (1) and a microwave receiver (2) and transmits and receives microwaves from one emission / reception surface.
Close to the surface of the object to be measured, and the sensor (4)
The reception in which the relative distance (X) between the emitting / receiving surface of the object and the surface of the object is forcibly cyclically fluctuated, and a composite wave of the reflected wave from the object to be measured and the self-oscillating wave is received during that period. The value of the received signal (V) detected and output by the device (2) is read into the processor (13) at very short time intervals, and the round trip of the fluctuation value obtained from the large number of the read data. A method for measuring the amount of water contained in an object, wherein the amount of water contained in the object to be measured is measured using the amount of change during one cycle as a parameter.
【請求項2】マイクロ波発信器(1)とマイクロ波受信
器(2)を一体に備えて一つの発受信面からマイクロ波
の発信及び受信をするマイクロ波ドップラセンサ(4)
と、該センサ(4)をその発受信面に対して垂直方向に
一定の振幅をもって周期的に強制的に往復揺動させる揺
動手段(17)と、その往復揺動の間に、被測定物体から
の反射波と自己発信波との合成波を受信した前記受信器
(2)がこれを検波して出力する受信信号(V)の値を
極く短い時間間隔で刻々と読み込み、その読み込まれた
多数のデータから得られる変動値の往復一周期の間の変
化分をパラメータとして、物体中に含まれる水分量を求
めるように演算処理する処理器(13)とから成り、被測
定物体の表面に向けて前記センサ(4)の発受信面を近
づけ周期的に往復揺動することにより、非接触状態で被
測定物体中に含まれる水分量を計測するように構成した
ことを特徴とする物体中に含まれる水分量の計測装置。
2. A microwave Doppler sensor (4) which integrally includes a microwave transmitter (1) and a microwave receiver (2) and transmits and receives microwaves from one emission / reception surface.
A oscillating means (17) for forcibly and reciprocally oscillating the sensor (4) periodically in a direction perpendicular to the transmitting and receiving surface with a constant amplitude, and a measured object between the oscillating means (17). The receiver (2), which has received the composite wave of the reflected wave from the object and the self-generated wave, detects this and outputs the value of the received signal (V) which is output at very short time intervals, and reads the value. It is composed of a processor (13) that performs arithmetic processing to obtain the amount of water contained in the object, using the amount of change in the fluctuation value obtained from a large number of data during one round trip as a parameter. It is configured to measure the amount of water contained in the object to be measured in a non-contact state by bringing the emitting / receiving surface of the sensor (4) closer to the surface and periodically swinging back and forth. A device for measuring the amount of water contained in an object.
JP1072163A 1989-03-24 1989-03-24 Method and apparatus for measuring the amount of water contained in an object Expired - Lifetime JPH076926B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1072163A JPH076926B2 (en) 1989-03-24 1989-03-24 Method and apparatus for measuring the amount of water contained in an object

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1072163A JPH076926B2 (en) 1989-03-24 1989-03-24 Method and apparatus for measuring the amount of water contained in an object

Publications (2)

Publication Number Publication Date
JPH02249958A JPH02249958A (en) 1990-10-05
JPH076926B2 true JPH076926B2 (en) 1995-01-30

Family

ID=13481307

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JP1072163A Expired - Lifetime JPH076926B2 (en) 1989-03-24 1989-03-24 Method and apparatus for measuring the amount of water contained in an object

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WO2024202893A1 (en) * 2023-03-24 2024-10-03 ソニーグループ株式会社 Data processing device and data processing method

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JP2016165328A (en) * 2015-03-09 2016-09-15 富士通株式会社 Washing / drying machine, washing / drying machine control device, dryness detection device, and drying machine
JP2021015074A (en) * 2019-07-13 2021-02-12 マイクロメジャー株式会社 Noncontact moisture meter and moisture content measurement method

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JPS5987346A (en) * 1982-11-11 1984-05-19 Inoue Japax Res Inc Detecting apparatus of moisture

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WO2024202893A1 (en) * 2023-03-24 2024-10-03 ソニーグループ株式会社 Data processing device and data processing method

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JPH02249958A (en) 1990-10-05

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