JPS6161625B2 - - Google Patents
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- Publication number
- JPS6161625B2 JPS6161625B2 JP7157081A JP7157081A JPS6161625B2 JP S6161625 B2 JPS6161625 B2 JP S6161625B2 JP 7157081 A JP7157081 A JP 7157081A JP 7157081 A JP7157081 A JP 7157081A JP S6161625 B2 JPS6161625 B2 JP S6161625B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- light
- dust
- amount
- window
- 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
Links
- 239000000428 dust Substances 0.000 claims description 61
- 230000003287 optical effect Effects 0.000 claims description 18
- 238000005259 measurement Methods 0.000 claims description 17
- 230000005540 biological transmission Effects 0.000 claims description 8
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 4
- 230000001678 irradiating effect Effects 0.000 claims 2
- 238000010586 diagram Methods 0.000 description 12
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 5
- 229910052799 carbon Inorganic materials 0.000 description 5
- 238000001514 detection method Methods 0.000 description 5
- 230000003247 decreasing effect Effects 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 239000000843 powder Substances 0.000 description 3
- 230000035945 sensitivity Effects 0.000 description 3
- 238000002834 transmittance Methods 0.000 description 3
- 238000002474 experimental method Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000000704 physical effect Effects 0.000 description 2
- 238000000151 deposition Methods 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000010893 paper waste Substances 0.000 description 1
- 239000002994 raw material Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/84—Systems specially adapted for particular applications
- G01N21/86—Investigating moving sheets
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Description
本発明はシート状の物体に含まれて水分量を測
定する装置に関する。
シート状の物体に含まれる水分量を測定する装
置として、抄造紙に含まれる、又は、吸着する水
分を連続して測定する多重散乱・透過方式水分計
がある(特願昭54−63362号)。
第1図は、上記水分計の構成説明図である。第
1図において、上ヘツド1は、照射窓4及び5
と、反射材を被覆した散乱面21と、円板状の板
面に2個の貫通穴を設け、一方の穴に基準光用フ
イルタ14を、他方の穴に測定光用フイルタ15
を埋設支承して、連続した定速回転をする回転セ
クタ13と、円板状の板面に複数の貫通穴171
8…等を設け、その一部に標準サンプル19,2
0…等を埋設支承して、外部から与えられる制御
信号によつて、定期的、又は、必要に応じて、定
められた角度で回転するサンプルホルダ16と、
照射窓4を通る平行光線を作成するランプ7、レ
ンズ8、ミラー9及びレンズ10とを有する。一
方、下ヘツド2は、入射窓6と、反射材を被覆し
た散乱面22と、入射窓6に入射する光を収束す
るレンズ11と、収束された入射光を検出するセ
ンサ12とを有する。
上・下ヘツド1及び2は、シート状の紙3を挾
んで対向状態にあり、ランプ7、レンズ8、照射
窓4、散乱面21及び22、入射窓6、レンズ1
1並びにセンサ12で多重散乱光学系を、ランプ
7、ミラー9、レンズ10、照射窓5、入射窓
6、レンズ11及びセンサ12で透過光学系を
夫々構成している。そして、通常の測定状態にあ
つては、貫通穴17を照射窓4の上に、貫通穴1
8を照射窓5の上に夫々位置させ、照射窓4及び
5から、回転セクタ13による断続光を紙3に照
射し、紙3と相互作用をもつた光、即ち、多重散
乱光学系における測定光Mn及び基準光Rn並びに
透過光学系における測定光Mt及び基準光Rtから
成る時系列信号をセンサ12で検出し、次段の演
算・制御部(図示せず)に送出し、所定の演算を
して紙の水分を測定するようになつている。ま
た、校正状態にあつては、上・下ヘツド1と2の
間に紙3がない状態でサンプルホルダ16を間欠
的に回転させ、照射窓4及び5の上に、標準サン
プル、即ち、零サンプル、スパンサンプル、チエ
ツクサンプ等を順次配設し、各サンプルによる測
定光Mn及びMt並びに基準光Rn及びRtに対応す
る信号を得るようになつている。
このような水分計において、演算・制御部で実
際の演算に用いる信号は、水分信号としてMn信
号(測定光Mnに対応する信号。以下、各光に対
応する信号をRn信号、Mt信号、Rt信号と言う)
とRn信号の比、即ち、Mn/Rn信号を用い、この
信号に含まれる誤差要因、例えば、透過率fの変
動(原料パルプに故紙を含有した抄造紙に多い)
をRn/Rt信号で補償演算を行うようになつてい
る。演算にMn/Rn信号及びRn/Rt信号を用い
るのは、光学系を構成するランプ、センサ等の特
性変動をキヤンセルするためと、Rn,Mn,Rt,
Mtの各信号と紙の光学的特性を左右する変数、
即ち、層数n、透過率f、反射率r及び水分量
MWとの間に、次表に示す感度特性を呈し、
Mn/Rn信号が水分量に対し、また、Rn/Rt信
号が透過率fに対し、夫々感度が大となる特性を
示すためである。
The present invention relates to an apparatus for measuring the amount of water contained in a sheet-like object. As a device for measuring the amount of moisture contained in a sheet-like object, there is a multiple scattering/transmission moisture meter that continuously measures the moisture contained in or adsorbed in papermaking (Japanese Patent Application No. 1983-63362). . FIG. 1 is an explanatory diagram of the structure of the moisture meter. In FIG. 1, the upper head 1 has irradiation windows 4 and 5.
, a scattering surface 21 coated with a reflective material, and two through holes are provided in the disk-shaped plate surface, with a reference light filter 14 in one hole and a measurement light filter 15 in the other hole.
A rotary sector 13 that is embedded and supported and rotates continuously at a constant speed, and a plurality of through holes 171 in a disc-shaped plate surface.
8, etc., and standard samples 19, 2 are included in some of them.
0..., etc., and rotates at a predetermined angle periodically or as needed by a control signal given from the outside;
It has a lamp 7, a lens 8, a mirror 9 and a lens 10 for creating parallel light rays passing through the illumination window 4. On the other hand, the lower head 2 has an entrance window 6, a scattering surface 22 coated with a reflective material, a lens 11 that converges the light incident on the entrance window 6, and a sensor 12 that detects the converged incident light. The upper and lower heads 1 and 2 face each other with a sheet of paper 3 in between, and include a lamp 7, a lens 8, an irradiation window 4, scattering surfaces 21 and 22, an entrance window 6, and a lens 1.
1 and sensor 12 constitute a multiple scattering optical system, and lamp 7, mirror 9, lens 10, irradiation window 5, entrance window 6, lens 11 and sensor 12 constitute a transmission optical system. In normal measurement conditions, the through hole 17 is placed above the irradiation window 4 and the through hole 1 is placed above the irradiation window 4.
8 are positioned above the irradiation window 5, and the paper 3 is irradiated with intermittent light from the rotating sector 13 from the irradiation windows 4 and 5, and the light that interacts with the paper 3, that is, the measurement in the multiple scattering optical system. A time series signal consisting of light Mn, reference light Rn, measurement light Mt and reference light Rt in the transmission optical system is detected by the sensor 12, and sent to the next stage calculation/control unit (not shown) to perform predetermined calculations. It is now possible to measure the moisture content of paper. In addition, in the calibration state, the sample holder 16 is rotated intermittently with no paper 3 between the upper and lower heads 1 and 2, and a standard sample, that is, a zero sample, is placed above the irradiation windows 4 and 5. Samples, span samples, check samples, etc. are arranged in sequence, and signals corresponding to measurement lights Mn and Mt and reference lights Rn and Rt from each sample are obtained. In such a moisture meter, the signal used for actual calculation in the calculation/control section is the Mn signal (signal corresponding to measurement light Mn) as a moisture signal.Hereinafter, the signals corresponding to each light are called Rn signal, Mt signal, Rt signal. (called a signal)
The ratio of the Mn and Rn signals, that is, the Mn/Rn signal, is used to calculate the error factors included in this signal, such as fluctuations in transmittance f (common in paper making containing waste paper in the raw material pulp).
Compensation calculations are performed using the Rn/Rt signals. The reason why the Mn/Rn signal and Rn/Rt signal are used in calculations is to cancel characteristic fluctuations of the lamps, sensors, etc. that make up the optical system, and to cancel changes in the characteristics of the lamps, sensors, etc. that make up the optical system, and to
Variables that affect each signal of Mt and the optical properties of paper,
That is, the number of layers n, transmittance f, reflectance r, and water content.
MW, exhibits the sensitivity characteristics shown in the table below,
This is because the sensitivity of the Mn/Rn signal increases with respect to the water content, and the sensitivity of the Rn/Rt signal increases with respect to the transmittance f.
【表】
ところで、Mn/Rn信号及びRn/Rt信号は所
望の因子以外による影響を受けないことが理想で
あるが、現実には、Rn,Mn,Rt,Mtの各信号
は、散乱面21や22、照射窓4や5、入射窓6
等に付着するダストの付着面によつて変動し、し
かも、ダストの色(白色、黒色灰色等がある)に
よつて異なる特性を示すので、ダスト雰囲気で測
定精度を維持することが難しかつた。そこで、先
に、本発明者らは、ダスト付着量のみを補償する
方法及び装置を発明した(特願昭55−104766号、
特願昭55−104769号)。上記発明によれば、Mn/
Rn信号(これをK値と言う)とダスト付着量
は、第2図に示す関係を有し、補償演算式は(1)式
となる。なお、(1)式において補償量はDK1・F
(ΔMz)である。
K=Kon−DK1・F(ΔMz) (1)
ΔMz=Rnd/Rtd−Rno/Rto (2)
但し、Kon…測定状態(オンライン)にお
けるK値(Mn/Rn信号)
DK1…実験によつて求めた定数
F(ΔMz)…ダスト付着量を示す
信号
Rnd,Rtd…散乱面等にダストが付
着している時、零サンプルを用いて
得たRn信号及びRt信号の値
Rno,Rto…散乱面等にダストが付
着していない時、零サンプルを用い
て得たRn信号及びRt信号の値
第2図において、縦軸はK値、横軸はダスト付
着量及び校正回数を示す。グラフ(イ)はサンプルホ
ルダ16の零サンプルを用いて得たグラフ、グラ
フ(ロ)は被測定体である紙を流す位置に、零サンプ
ルと同じ物性のシート状物体を配設して得たグラ
フである。
なお、実際に検出ヘツドを据付ける現場におい
て、ダストの付着量は時間と共に比例的に増加す
るので、校正を一定間隔で行う場合、ダストの付
着量は校正回数に対応するので、ダスト付着量は
校正回数に比例する。
グラフ(イ)において、A点は、上・下ヘツドの散
乱面、各窓等にダストが付着していない状態にお
けるK値でKzoとなつている。B点は、一定時間
後の校正(これを第1回目の校正と言う)におけ
る値をプロツトしたもので、ダスト付着量d=
d1、K値=Kz1となつている。同様に、C点は、
第2回目の校正によるもので、ダスト付着量d=
d2、K値=Kz2であり、D点は、第3回目の校正
によるもので、ダスト付着量d=d3、K値=Kz3
である。
一方、グラフ(ロ)におけるA点、B′点、C′点及
びD′点は、グラフ(イ)におけるA点、B点、C点
およびD点に夫々対応している。このように、サ
ンプルを配設する位置によつてK値が異なるの
は、実際に紙を流す位置にシート状のサンプルを
配設した場合、多重散乱の度合が、サンプルホル
ダのサンプルによる場合に比べて極めて大きいた
めであると考えられている。
同様に、Rn/Rt信号(これをM値と言う)に
ついても第2図と同様の特性を示し、M値の補償
演算式は(3)式となる。
M=Mon−DK2・F(ΔMz) (3)
但し、Mon…測定状態(オンライン)にお
けるM値(Rn/Rt信号)
DK2…実験によつて求めた定数
F(ΔMz)…(1)式におけると同じ
ところで、(1)式及び(3)式における定数DK1及び
DK2はダストの色が一定している場所では定数と
みなし得るが、ダストの色が変るとDK1及びDK2
も変る。しかも、検出ヘツドが据付けられる現場
は、紙粉(白色)、紙粉+カーボン(灰色)、カー
ボン(黒色)等が混在する雰囲気が多いので、(1)
式及び(3)式を用いてダストによる影響を完全に補
償することが難しい。
第3図及び第4図は(1)式及び(3)式における補償
量DK1・F(ΔMz)≡ΔKpp及びDK2・F(Δ
Mz)≡ΔMppの特性図である。各図のグラフに
付した符号の添字1は散乱面等に白色ダスト(紙
粉)が付着した時の特性である。同様に、添字2
は灰白色ダスト(紙粉+少量のカーボン)、添字
3は灰黒色ダスト(紙粉+多量のカーボン)、添
字4は黒色ダスト(カーボン)が付着した時の特
性である。これら添字の意味するところは、後述
する第5図においても同様である。
第5図は、第1図の検出ヘツドにおける零サン
プルを用い、Rn信号とRt信号の関係を求めたも
のである。第5図から明らかなように、Rn信号
は白色ダストが付着している場合、増加特性を示
すのに対し、黒色、又は、黒色に近い色のダスト
が付着している場合、減少特性を示す。一方、
Rt信号はダストの色に関係なく減少特性となつ
ている。
上記現象は、照射窓4を透過する光が白色ダス
トの存在によつて散乱光となり、かつ、上・下ヘ
ツドで形成するギヤツプ中を多重散乱してきた光
が照射窓5に付着する白色ダストによつて、より
多く入射窓6に入射するために起るものと考えら
れる。
本発明は、かかる点に鑑みてなされたものであ
り、散乱面(対向面)、照射窓、入射窓等に付着
するダストの量や性状に関係なく精度の良い測定
信号を得るために、ダストの色に対して一定の特
性を有する検出信号を得ると共に、ダストの付着
量による影響を演算によつて補償する装置を提供
することを目的とする。
即ち、本発明による装置は、窓面に凹ノンズを
近接設置して成る照射窓から被測定体に光を照射
し、その被測定体と複数回相互作用をもつた光
を、窓面に近接して凹レンズを設置して成る入射
窓を介して検出する多重散乱光学系と、入射窓に
比して小さい開口部を有する光の透過通路を形成
して成る照射窓から被測定体に光を照射し、その
被測定体を透過した光を検出する透過光学系と、
上・下ヘツドの対向面にダストが付着していない
時、標準サンプルを用いて求めた校正信号及び定
期的、又は、必要に応じて校正動作をかけ、標準
サンプルを用いて求めた校正信号を用いて所定の
演算をして、被測定体の物性に関する信号を得る
手段とを有する。
以下、本発明について詳しく説明する。
第6図は、本発明の一実施例による測定装置の
構成説明図である。第6図に付した符号で、第1
図と同一のものは同一意味を有するので、ここで
の説明を省略する。
第6図における装置の構成の特徴は、窓面に近
接設置して成る凹レンズ31を有し、この凹レン
ズ31を介して紙3に光を照射する多重散乱光学
系の照射窓4と、光路にカラー33を有する集光
レンズ32を配設し、入射窓6の開口部より小さ
い開口部を有する透過光学系の照射窓5と、窓面
に近接設置して成る凹ノンズ34を有し、この凹
レンズ34を介してセンサ12に入射光を導く入
射窓6とを有する点にある。
上記構成において、回転セクタ13及びサンプ
ルホルダ16は、第1図におけると同一な動作を
行い、センサ12は、Rn,Mn,Rt,Mtの時系
列信号を検出し、演算・制御部に送出する。この
時のRn信号とRt信号の関係は、付着するダスト
の色によつて第8図に示すように変る。第8図に
おいて、縦軸は、ダスト付着量が零の時のRn信
号を基準にしたRn信号の変化率であり、横軸
は、同じ状況におけるRt信号の変化率である。
グラフC1,C2,C3及びC4は、前記した白色ダス
ト、灰白色ダスト、灰黒色ダスト及び黒色ダスト
を、各窓面、散乱面等に付着して得たグラフであ
る。図に示すように、Rn信号は、窓面、散乱面
等にダストが付着していない時、最大を示し、ダ
ストが付着すると、その色に関係なく減少傾向を
示す。即ち、第5図の特性と異なり、ダストが
上・下ヘツドの対向面に付着すると、Rn信号は
必ず減少する。この現象について以下のように考
えることができる。
照射窓4からの光は、第7図イに示すように、
レンズ8を介して得る平行光線35を、凹レンズ
31によつて2π方向に投光する散乱光となり、
ダストがない状態で理想的な散乱光となる。この
ため、照射窓4の窓面にダストが付着すると、た
とえ、それが白色であつても散乱光は減少する。
また、入射窓6の窓面に近接して凹レンズ34を
設置しているので、第7図ロに示すように、上・
下ヘツド間のギヤツプを散乱してきた散乱光36
の検出が容易で、(センサ12からの視野角が実
質的に拡大される)しかも、入射窓6の真上に位
置する照射窓5の開口部が入射窓6の開口部に比
して小さいので、照射窓5の開口部に反射して入
射する散乱光は、照射窓5の開口部の状態変化
(ダスト付着)による影響をほとんど受けない。
上記理由によつて上・下ヘツドの対向面にダス
トが付着するとRn信号は減少傾向を示す。
このように、Rn信号が散乱面等に付着するダ
ストの色に関係なく、減少傾向を呈することによ
つて、補償量ΔKpp及びΔMppは第9図及び第
10図に示すように、ダストの色に影響されない
補償係数を有する特性となる。第9図及び第10
図は、本発明による装置におけるK値の補償量Δ
Kpp及びM値の補償量ΔMppとダスト付着量信
号ΔMzの関係を示したものであり、データの・
印は白色ダスト、○・は灰白色ダスト、△・印は灰黒
色ダスト、□・は黒色ダストを示す。
なお、上記実施例は、抄造紙の水分計について
説明したが、本発明はこれに限定するものではな
く、フイルムの厚さ測定装置等のシート状の物体
の物理量測定装置を含むものである。
また、上記実施例は、Mn/Rn信号及びRn/
Rt信号を用いて所定の演算を行つているが、本
発明はこれに限定するものではなく、他の信号を
用いて演算を行う装置であつてもよい。
以上詳しく説明したように、本発明による測定
装置によれば、散乱面等に付着するダストの色に
対して一定の特性を有する検出信号を得ると共
に、ダストの付着量を所定の演算をして補償して
いるので、散乱面等に付着するダストの量や性状
に関係なく、精度の良い測定信号を得ることがで
きる。[Table] By the way, it is ideal that the Mn/Rn signal and the Rn/Rt signal are not affected by factors other than desired factors, but in reality, each signal of Rn, Mn, Rt, and Mt is affected by the scattering surface 21. 22, irradiation windows 4 and 5, entrance window 6
It was difficult to maintain measurement accuracy in a dusty atmosphere because the characteristics varied depending on the surface of the dust adhering to the surface, and also showed different characteristics depending on the color of the dust (white, black, gray, etc.). . Therefore, the present inventors previously invented a method and device for compensating only the amount of dust adhesion (Japanese Patent Application No. 104766/1983).
(Special Application No. 104769, 1982). According to the above invention, Mn/
The Rn signal (this is called the K value) and the amount of dust adhesion have the relationship shown in FIG. 2, and the compensation calculation formula is equation (1). In addition, in equation (1), the amount of compensation is DK 1・F
(ΔMz). K=Kon−DK 1・F(ΔMz) (1) ΔMz=Rn d /Rt d −Rno/Rto (2) However, Kon...K value (Mn/Rn signal) in measurement state (online) DK 1 ...Experiment Constant F (ΔMz) determined by... Signal indicating the amount of dust adhesion Rn d , Rt d ... Value Rno of Rn signal and Rt signal obtained using zero sample when dust is attached to the scattering surface etc. , Rto... Values of Rn signal and Rt signal obtained using zero sample when no dust is attached to the scattering surface, etc. In Figure 2, the vertical axis is the K value, and the horizontal axis is the amount of dust attached and the number of calibrations. show. Graph (a) is a graph obtained using the zero sample in sample holder 16, and graph (b) is obtained by placing a sheet-like object with the same physical properties as the zero sample at the position where the paper to be measured is flowed. It is a graph. In addition, at the site where the detection head is actually installed, the amount of attached dust increases proportionally with time, so when calibration is performed at regular intervals, the amount of attached dust corresponds to the number of times of calibration, so the amount of attached dust is Proportional to the number of calibrations. In the graph (a), point A is Kzo, which is the K value when no dust is attached to the scattering surfaces of the upper and lower heads, each window, etc. Point B is a plot of the value after the calibration after a certain period of time (this is called the first calibration), and the amount of dust adhesion d=
d 1 and K value=Kz 1 . Similarly, point C is
Due to the second calibration, dust adhesion amount d=
d 2 , K value = Kz 2 , D point is due to the third calibration, dust adhesion amount d = d 3 , K value = Kz 3
It is. On the other hand, points A, B', C', and D' in graph (b) correspond to points A, B, C, and D in graph (a), respectively. The reason why the K value differs depending on the position where the sample is placed is that when a sheet-like sample is placed at the position where the paper is actually flowed, the degree of multiple scattering is due to the sample in the sample holder. This is thought to be because it is extremely large in comparison. Similarly, the Rn/Rt signal (referred to as the M value) also exhibits the same characteristics as shown in FIG. 2, and the compensation calculation formula for the M value is equation (3). M=Mon−DK 2・F(ΔMz) (3) However, Mon...M value (Rn/Rt signal) in measurement state (online) DK 2 ...Constant F(ΔMz) found by experiment...(1) Same as in equations By the way, constant DK 1 and in equations (1) and (3)
DK 2 can be considered a constant in places where the dust color is constant, but when the dust color changes, DK 1 and DK 2
It also changes. Moreover, the site where the detection head is installed often has an atmosphere containing a mixture of paper dust (white), paper dust + carbon (gray), carbon (black), etc. (1)
It is difficult to completely compensate for the influence of dust using equations and equations (3). Figures 3 and 4 show the compensation amount DK 1・F (ΔMz)≡ΔKpp and DK 2・F (ΔMz) in equations (1) and (3).
FIG. 2 is a characteristic diagram of Mz)≡ΔMpp. The suffix 1 attached to the graph in each figure indicates the characteristics when white dust (paper powder) adheres to the scattering surface or the like. Similarly, subscript 2
is a characteristic when gray-white dust (paper powder + a small amount of carbon) is attached, subscript 3 is a gray-black dust (paper powder + a large amount of carbon), and subscript 4 is a characteristic when black dust (carbon) is attached. The meanings of these subscripts are the same in FIG. 5, which will be described later. FIG. 5 shows the relationship between the Rn signal and the Rt signal using zero samples in the detection head of FIG. 1. As is clear from Figure 5, the Rn signal shows an increasing characteristic when white dust is attached, whereas it shows a decreasing characteristic when black or near-black dust is attached. . on the other hand,
The Rt signal has a decreasing characteristic regardless of the color of the dust. The above phenomenon occurs because the light that passes through the irradiation window 4 becomes scattered light due to the presence of white dust, and the light that has been multiple scattered in the gap formed by the upper and lower heads is scattered by the white dust that adheres to the irradiation window 5. Therefore, it is considered that this occurs because more light is incident on the entrance window 6. The present invention has been made in view of this point, and is aimed at obtaining accurate measurement signals regardless of the amount and properties of dust adhering to the scattering surface (opposing surface), irradiation window, entrance window, etc. It is an object of the present invention to provide a device that obtains a detection signal having constant characteristics for each color and compensates for the influence of the amount of attached dust by calculation. That is, the device according to the present invention irradiates light onto an object to be measured from an irradiation window consisting of a concave lens placed close to the window surface, and directs the light that has interacted with the object multiple times close to the window surface. A multiple scattering optical system detects the light through an entrance window with a concave lens installed therein, and an irradiation window that forms a light transmission path with an opening smaller than the entrance window illuminates the object to be measured. a transmission optical system that detects the light transmitted through the object to be measured;
When there is no dust attached to the opposing surfaces of the upper and lower heads, apply the calibration signal obtained using the standard sample and periodically or as necessary, and perform the calibration signal obtained using the standard sample. and means for performing predetermined calculations using the measurement object to obtain a signal related to the physical properties of the object to be measured. The present invention will be explained in detail below. FIG. 6 is an explanatory diagram of the configuration of a measuring device according to an embodiment of the present invention. Number 1 is the number given in Figure 6.
Components that are the same as those in the drawings have the same meaning, so their explanations will be omitted here. The configuration of the apparatus shown in FIG. 6 is characterized by having a concave lens 31 installed close to the window surface, an irradiation window 4 of a multiple scattering optical system that irradiates light onto the paper 3 through this concave lens 31, and an irradiation window 4 in the optical path. A condensing lens 32 having a collar 33 is disposed, an irradiation window 5 of a transmission optical system having an aperture smaller than the aperture of the entrance window 6, and a concave lens 34 disposed close to the window surface. It has an entrance window 6 that guides incident light to the sensor 12 via a concave lens 34. In the above configuration, the rotating sector 13 and sample holder 16 perform the same operations as in FIG. 1, and the sensor 12 detects time-series signals of Rn, Mn, Rt, and Mt and sends them to the calculation/control unit . The relationship between the Rn signal and the Rt signal at this time changes as shown in FIG. 8 depending on the color of the attached dust. In FIG. 8, the vertical axis is the rate of change of the Rn signal with respect to the Rn signal when the amount of dust adhesion is zero, and the horizontal axis is the rate of change of the Rt signal in the same situation.
Graphs C 1 , C 2 , C 3 and C 4 are graphs obtained by depositing the above-described white dust, gray-white dust, gray-black dust, and black dust on each window surface, scattering surface, etc. As shown in the figure, the Rn signal is at its maximum when no dust is attached to the window surface, scattering surface, etc., and when dust is attached, it shows a decreasing tendency regardless of its color. That is, unlike the characteristics shown in FIG. 5, when dust adheres to the opposing surfaces of the upper and lower heads, the Rn signal always decreases. This phenomenon can be considered as follows. The light from the irradiation window 4 is as shown in FIG.
The parallel light beam 35 obtained through the lens 8 becomes scattered light projected in the 2π direction by the concave lens 31,
Ideal scattered light without dust. Therefore, if dust adheres to the window surface of the irradiation window 4, scattered light will decrease even if the dust is white.
In addition, since the concave lens 34 is installed close to the window surface of the entrance window 6, as shown in FIG.
Scattered light 36 that has been scattered through the gap between the lower heads
is easy to detect (the viewing angle from the sensor 12 is substantially expanded), and the opening of the irradiation window 5 located directly above the entrance window 6 is smaller than the opening of the entrance window 6. Therefore, the scattered light that is reflected and enters the opening of the irradiation window 5 is hardly affected by changes in the state of the opening of the irradiation window 5 (dust adhesion). For the above reason, when dust adheres to the opposing surfaces of the upper and lower heads, the Rn signal tends to decrease. In this way, the Rn signal exhibits a decreasing tendency regardless of the color of dust adhering to the scattering surface, etc., so that the compensation amounts ΔKpp and ΔMpp depend on the color of the dust, as shown in Figures 9 and 10. This is a characteristic that has a compensation coefficient that is not affected by. Figures 9 and 10
The figure shows the compensation amount Δ of the K value in the device according to the invention.
It shows the relationship between the compensation amount ΔMpp of Kpp and M value and the dust adhesion amount signal ΔMz, and the data
The mark indicates white dust, the mark ○ indicates gray-white dust, the mark △ indicates gray-black dust, and the mark □ indicates black dust. Although the above embodiments have been described with respect to a moisture meter for papermaking, the present invention is not limited to this, but includes devices for measuring physical quantities of sheet-like objects, such as a device for measuring film thickness. Furthermore, in the above embodiment, the Mn/Rn signal and the Rn/
Although predetermined calculations are performed using the Rt signal, the present invention is not limited to this, and may be an apparatus that performs calculations using other signals. As explained in detail above, according to the measuring device according to the present invention, a detection signal having a certain characteristic with respect to the color of dust adhering to a scattering surface etc. is obtained, and the amount of adhering dust is calculated in a predetermined manner. Since the compensation is performed, highly accurate measurement signals can be obtained regardless of the amount and properties of dust adhering to the scattering surface, etc.
第1図は、従来の多重散乱・透過方式水分計の
構成説明図、第2図は、K値−ダスト付着量特性
図、第3図及び第4図は、補償量とダスト付着量
信号の関係図、第5図は、Rn信号とRt信号の関
係図、第6図は、本発明の一実施例による水分計
の構成説明図、第7図は、本発明による水分計の
多重散乱光学系照射窓における散乱光作成説明図
及び入射窓における入射光説明図、第8図は、本
発明による水分計におけるRn信号−Rt信号関係
図、第9図及び第10図は、本発明による水分計
における補償量とダスト付着量信号の関係図であ
る。
1……上ヘツド、2……下ヘツド、3……紙、
4及び5……照射窓、6……入射窓、7……ラン
プ、8,10及び32……レンズ、13……回転
セクタ、16……サンプルホルダ、31及び34
……凹レンズ。
Fig. 1 is an explanatory diagram of the configuration of a conventional multiple scattering/transmission moisture analyzer, Fig. 2 is a K value-dust adhesion characteristic diagram, and Figs. 3 and 4 are compensation amount and dust adhesion amount signals. 5 is a diagram showing the relationship between the Rn signal and the Rt signal, FIG. 6 is an explanatory diagram of the configuration of a moisture meter according to an embodiment of the present invention, and FIG. 7 is a diagram showing the multiple scattering optics of the moisture meter according to the present invention. An explanatory diagram of the creation of scattered light in the system irradiation window and an explanatory diagram of the incident light in the incident window. FIG. 8 is a diagram of the Rn signal-Rt signal relationship in the moisture meter according to the present invention. FIGS. FIG. 3 is a diagram showing the relationship between the compensation amount in the meter and the dust adhesion amount signal. 1...Top head, 2...Bottom head, 3...Paper,
4 and 5...irradiation window, 6...incident window, 7...lamp, 8, 10 and 32...lens, 13...rotating sector, 16...sample holder, 31 and 34
……concave lens.
Claims (1)
形の光学系および透過形の光学系を構成すると共
に、該上・下ヘツドで形成される間隙にシート状
の物体を配設し該物体に中の水分によつて吸収さ
れる波長領域の光である測定光と吸収されない波
長領域の光である基準光とを該物体に照射し、該
物体と相互作用をもつた前記測定光及び基準光を
前記2つの光学系に共通の受光部で検出し、該測
定光及び基準光に夫々対応して前記受光部から出
力される測定信号および基準信号を用いる演算に
よつて前記物体に含有されている水分量を測定す
る装置において、窓面に凹レンズを近接設置し入
射する光を発散させながら前記物体に照射するよ
うに前記多重散乱形光学系の照射部を構成すると
共に、前記受光部の入射窓に比して小さい開口部
をもつた照射窓を有するように前記透過形光学系
の照射部を構成し、前記上・下ヘツドの対向面に
ダストが付着していないとき標準サンプルを用い
て求めた校正信号、および定期的又は必要に応じ
て校正動作をかけ前記標準サンプルを用いて求め
た校正信号を使用し前記測定信号および基準信号
を用いる演算で前記ダスト付着量の影響を除去し
て前記水分量に関する信号を得る手段とを具備す
ることを特徴とするシート状物体中の水分量測定
装置。1. An upper head and a lower head are arranged facing each other to constitute a multiple scattering type optical system and a transmission type optical system, and a sheet-like object is arranged in the gap formed by the upper and lower heads, and a sheet-like object is arranged in the gap formed by the upper and lower heads. The object is irradiated with measurement light that is light in a wavelength range that is absorbed by moisture in the object and reference light that is light in a wavelength range that is not absorbed, and the measurement light and the reference light that interact with the object. is detected by a light receiving section common to the two optical systems, and is detected by a calculation using a measurement signal and a reference signal output from the light receiving section corresponding to the measurement light and reference light, respectively. In an apparatus for measuring the amount of water in a body, the irradiating section of the multiple scattering optical system is configured such that a concave lens is installed close to the window surface to irradiate the object while diverging the incident light, and the irradiating section of the multiple scattering optical system is configured to The irradiation section of the transmissive optical system is configured to have an irradiation window with an opening smaller than the window, and when no dust is attached to the opposing surfaces of the upper and lower heads, a standard sample is used. Using the obtained calibration signal and the calibration signal obtained using the standard sample through which a calibration operation is performed periodically or as necessary, the influence of the amount of dust adhesion is removed by calculation using the measurement signal and reference signal. A device for measuring the amount of moisture in a sheet-like object, comprising means for obtaining a signal related to the amount of moisture.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7157081A JPS57186155A (en) | 1981-05-13 | 1981-05-13 | Measuring apparatus of characteristic of sheet-shaped body |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7157081A JPS57186155A (en) | 1981-05-13 | 1981-05-13 | Measuring apparatus of characteristic of sheet-shaped body |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57186155A JPS57186155A (en) | 1982-11-16 |
| JPS6161625B2 true JPS6161625B2 (en) | 1986-12-26 |
Family
ID=13464489
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7157081A Granted JPS57186155A (en) | 1981-05-13 | 1981-05-13 | Measuring apparatus of characteristic of sheet-shaped body |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57186155A (en) |
-
1981
- 1981-05-13 JP JP7157081A patent/JPS57186155A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57186155A (en) | 1982-11-16 |
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