JPH0465334B2 - - Google Patents
Info
- Publication number
- JPH0465334B2 JPH0465334B2 JP60067552A JP6755285A JPH0465334B2 JP H0465334 B2 JPH0465334 B2 JP H0465334B2 JP 60067552 A JP60067552 A JP 60067552A JP 6755285 A JP6755285 A JP 6755285A JP H0465334 B2 JPH0465334 B2 JP H0465334B2
- Authority
- JP
- Japan
- Prior art keywords
- pulp
- beating
- degree
- light intensity
- measurement
- 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
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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
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/47—Scattering, i.e. diffuse reflection
- G01N21/49—Scattering, i.e. diffuse reflection within a body or fluid
- G01N21/51—Scattering, i.e. diffuse reflection within a body or fluid inside a container, e.g. in an ampoule
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)
- Paper (AREA)
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は紙パルプ工業に於ける懸濁状パルプの
叩解程度測定方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Industrial Field of Application) The present invention relates to a method for measuring the degree of beating of suspended pulp in the pulp and paper industry.
(従来の技術)
紙の原料であるパルプは、通常幅10〜50μm、
長さ0.5〜3mmの木材繊維であり、かかるパルプ
は抄紙工程でシートにする前に種々の処理が施こ
される。その代表的な処理は、叩解と称される機
械処理であつて、繊維は叩解機によつて圧潰、切
断、膨潤等の処理を受けると共に、外部フイブリ
ル化と称される繊維の開裂が行なわれる。(Conventional technology) Pulp, the raw material for paper, usually has a width of 10 to 50 μm.
It is a wood fiber with a length of 0.5 to 3 mm, and the pulp is subjected to various treatments before being made into sheets in the papermaking process. The typical process is a mechanical process called beating, in which the fibers are crushed, cut, swollen, etc. by a beating machine, and the fibers are cleaved, which is called external fibrillation. .
叩解とはこのような処理を繊維に施すものであ
るが、その程度によつて、得られた紙の性質は極
度に変化する。即ち、紙の性質を決める重要な因
子は叩解処理であり、この処理を夫々どの程度施
こすかによつて同じ原料のパルプでも異なつた性
質の紙が出来、その80%以上が叩解処理によつて
決まるとされている。 Beating is a process in which fibers are subjected to such treatment, and the properties of the resulting paper vary dramatically depending on the degree of beating. In other words, the important factor that determines the properties of paper is the beating process, and depending on the extent to which this process is applied, paper with different properties can be produced even from pulp made from the same raw material, and more than 80% of the paper is due to the beating process. It is said that it will be determined by
このような重要な因子である叩解の程度を表わ
す方法として、従来はカナダ標準ろ水度試験方法
等が用いられ、CSF値として常用され、数値化さ
れているが、これは上記の複雑な繊維の変化をま
とめて1つの数値で示すだけに止り、必ずしもそ
の値だけで、得られる紙の性質を反映するもので
はない。こうして従来から、叩解による繊維の変
化のうち、特に外部フイブリル化の程度を分離し
て測定し得る方法が望まれている。 Conventionally, the Canadian Standard Freeness Test Method has been used as a method to express the degree of beating, which is an important factor, and is commonly used and quantified as the CSF value, but this is difficult to measure due to the complex fibers mentioned above. It merely shows the changes in values as a single numerical value, and that value alone does not necessarily reflect the properties of the paper obtained. Thus, there has been a desire for a method that can separate and measure the degree of external fibrillation among the changes in fibers caused by beating.
このような外部フイブリル化の程度を分離して
測定することを目的として、従来例えば特開昭53
−41506号公報に開示されるような光学測定方法
が提案されている。 For the purpose of separating and measuring the degree of external fibrillation, for example, Japanese Patent Laid-Open No. 53
An optical measurement method as disclosed in Japanese Patent No. -41506 has been proposed.
この測定方法は光源から照射してパルプ懸濁液
試料を透過した光線を、積分球により構成した分
離部により直進光成分と散乱光成分とに分離し
て、それらの強度を測定し、これらの夫々の強度
と、前記試料が水だけの場合の夫々の強度とから
導出される散乱比によりパルプ繊維の外部フイブ
リル化および内部フイブリル化の程度を導出する
ものである。 In this measurement method, a light beam irradiated from a light source and transmitted through a pulp suspension sample is separated into a straight light component and a scattered light component by a separating section composed of an integrating sphere, and the intensity of these components is measured. The degree of external fibrillation and internal fibrillation of pulp fibers is derived from the scattering ratio derived from the respective intensities and the respective intensities when the sample is only water.
(発明が解決しようとする課題)
上述した従来の測定方法では、散乱光成分とし
て、光線の照射方向にして懸濁液の前方位置の散
乱光成分のみを用いるので、後方位置に於いて叩
解程度の差に対応して測定光強度の差が顕著に現
れる場合でも、この差、そしてこれによる高感度
の測定を行うことができない。(Problems to be Solved by the Invention) In the conventional measuring method described above, only the scattered light component at the front position of the suspension in the direction of irradiation of the light beam is used as the scattered light component. Even if there is a noticeable difference in the measurement light intensity corresponding to the difference in , it is not possible to perform high-sensitivity measurement due to this difference.
また、上述の従来技術は、パルプ濃度をパラメ
ータにとつて前記散乱比と叩解程度の関係を導出
しているが、パルプ濃度が未知または変動するパ
ルプ懸濁液の叩解程度を、いかにして測定または
導出するかについては、その技術的手段全く開示
していない。 Furthermore, in the above-mentioned conventional technology, the relationship between the scattering ratio and the degree of beating is derived using the pulp concentration as a parameter, but how can the degree of beating of a pulp suspension in which the pulp concentration is unknown or fluctuate be measured? Or, the technical means for deriving it are not disclosed at all.
本発明は以上の点に鑑みてなされたもので、即
ち濃度が未知または変動するパルプ懸濁液の前述
した外部フイブリル化の程度を他と分離して濃度
と共に、その移送経路に於いて非接触式で高感
度、高精度に測定し得る測定方法を提供すること
を目的とするものである。 The present invention has been made in view of the above points, that is, the degree of external fibrillation of a pulp suspension whose concentration is unknown or fluctuates is separated from other parts, and the degree of external fibrillation, together with the concentration, is transferred in a non-contact manner. The purpose of this invention is to provide a measurement method that can perform measurements with high sensitivity and accuracy using the following formulas.
(課題を解決するための手段)
上述した課題を解決するための手段を説明する
と、本発明の測定方法は、被測定パルプ懸濁液の
移送経路に、光学的測定部と音響的測定部とを構
成し、該光学的測定部はパルプ懸濁液に測定光を
照射する測定光照射装置と、該パルプ懸濁液を経
た測定光を、その前方及び後方位置に於いて測定
可能な測定光強度測定装置とから構成すると共
に、前記音響的測定部は、前記パルプ懸濁液に超
音波を透過させて、その減衰量を測定する超音波
送受信装置により構成し、該音響的測定部に於い
て前記パルプ懸濁液による超音波の減衰量を測定
して、この減衰量とパルプ濃度との対応関係によ
り、パルプ濃度を算出すると共に、前記光学的測
定部に於いて前記前方または後方位置に於ける測
定光強度を測定し、前記音響的測定部に於いて算
出したパルプ懸濁液の濃度に対応する前記測定光
強度と叩解程度との対応関係により、叩解程度を
算出することを要旨とするものである。(Means for Solving the Problems) To explain the means for solving the above-mentioned problems, the measurement method of the present invention includes an optical measurement section and an acoustic measurement section in the transfer path of the pulp suspension to be measured. The optical measurement unit includes a measurement light irradiation device that irradiates the pulp suspension with measurement light, and a measurement light that can measure the measurement light that has passed through the pulp suspension at the front and rear positions. The acoustic measuring section includes an ultrasonic transmitter/receiver that transmits ultrasonic waves through the pulp suspension and measures the amount of attenuation thereof. The amount of attenuation of the ultrasonic waves due to the pulp suspension is measured, and the pulp concentration is calculated based on the correspondence between the amount of attenuation and the pulp concentration. The gist is to calculate the beating degree based on the correspondence between the measuring light intensity corresponding to the concentration of the pulp suspension calculated in the acoustic measuring section and the beating degree. It is something to do.
(作用)
一定のパルプ濃度のパルプ懸濁液に測定光を照
射して、該パルプ懸濁液を経た測定光強度を測定
し、叩解程度との対応関係を調べると、前方位置
及び後方位置に於ける測定光強度は叩解程度に対
応して変化し、その変化方向は逆であること、そ
して叩解程度の変化に対応して測定光強度の変化
が顕著に現れる側は、上記前方位置または後方位
置のいずれか一方側に現れることがわかる。従つ
てパルプ濃度に対応して上記測定光強度と叩解程
度との対応関係を予め測定して求めておけば、上
記光学的測定と共にパルプ濃度の測定を行うこと
により、被測定パルプ懸濁液の叩解程度を、対応
した変化が顕著に現れる上記前方又は後方位置の
測定光強度から算出することができる。(Function) When a measuring light is irradiated onto a pulp suspension having a constant pulp concentration and the intensity of the measuring light passing through the pulp suspension is measured and the relationship with the degree of beating is investigated, it is found that The measurement light intensity changes in accordance with the degree of refining, and the direction of change is the opposite.The side where the change in the measurement light intensity appears conspicuously in response to the change in the degree of refining is the above-mentioned front position or rear position. It can be seen that it appears on either side of the position. Therefore, if the correspondence between the above-mentioned measurement light intensity and the degree of beating is determined in advance in accordance with the pulp concentration, by measuring the pulp concentration together with the above-mentioned optical measurement, it is possible to determine the value of the pulp suspension to be measured. The degree of beating can be calculated from the measured light intensity at the front or rear position where the corresponding change is noticeable.
一方、パルプ懸濁液に超音波を透過させて、そ
の減衰量を測定し、パルプ濃度との対応関係を調
べると、このパルプ濃度と超音波減衰量とは、叩
解程度に関わらず略一つの直線の対応関係となる
ことがわかる。従つてパルプの種類等に対応し
て、パルプ濃度と超音波減衰量との対応関係を予
め測定しておけば、パルプ懸濁液のパルプ濃度を
超音波減衰量から算出することができる。 On the other hand, when ultrasonic waves are transmitted through a pulp suspension, the attenuation amount is measured, and the relationship between the ultrasonic wave attenuation amount and the pulp concentration is examined, it is found that the pulp concentration and the ultrasonic attenuation amount are approximately the same regardless of the degree of beating. It can be seen that there is a linear correspondence relationship. Therefore, if the correspondence between the pulp concentration and the ultrasonic attenuation amount is measured in advance according to the type of pulp, etc., the pulp concentration of the pulp suspension can be calculated from the ultrasonic attenuation amount.
以上のことから、前者の測定を行う光学的測定
部と後者の測定を行う音響的測定部をパルプ懸濁
液の移送経路に設置して、音響的測定部に於ける
後者の測定によりパルプ濃度を測定し、これをフ
イードバツクして光学的測定部に於ける前者の測
定を行うことにより、移送経路を流れるパルプ懸
濁液の叩解程度を算出することができる。 Based on the above, an optical measuring section that measures the former and an acoustic measuring section that measures the latter are installed in the transport path of the pulp suspension, and the latter measurement in the acoustic measuring section measures the pulp concentration. The degree of beating of the pulp suspension flowing through the transfer path can be calculated by measuring the former and feeding it back to measure the former in the optical measuring section.
(実施例) 次に本発明の実施例を図について説明する。(Example) Next, embodiments of the present invention will be described with reference to the drawings.
符号1は被測定パルプ懸濁液Lにレーザ光等の
測定光を照射する測定光照射装置であり、2は照
射されて懸濁液Lを経た測定光の強度を測定する
測定光強度測定装置である。これらの装置1,2
から光学的測定部Aを構成する。前記測定装置2
は測定光の照射方向に対して、懸濁液Lの前方位
置a及び後方位置bに於いて測定し得るように構
成する。この測定装置2の具体例を説明すると、
第1図に示すものは、懸濁液Lから適宜距離隔て
た円周上に於いて、該懸濁液Lの前方位置aから
後方位置bに至る複数位置に光強度センサ3を配
設して、夫々の光強度センサ3により前記位置
a,bの複数位置に於ける測定光強度を測定する
ものである。この具体例のように複数位置に於け
る測定光強度を測定する他の例として、図示はし
ていないが、単一の光強度センサを移動させて前
記前方位置aから後方位置bに至る連続位置ある
いは複数位置に於いて測定するようにすることも
できる。尚、測定光強度の測定位置は、前方位置
aまたは後方位置b毎に夫々適宜1点を最小構成
とするが、それよりも多くの点に於いて測定し得
るように構成することにより後述の測定の自由度
を大きくすることができる。符号4は前記被測定
懸濁液を収容する透明な収容部であり、この収容
部4は独立した容器として構成しても良いし、第
2図及び第8図に示すように移送経路Cの一部に
構成しても、流動している懸濁液を測定するよう
にすることもできる。 Reference numeral 1 is a measurement light irradiation device that irradiates measurement light such as a laser beam onto the pulp suspension L to be measured, and 2 is a measurement light intensity measurement device that measures the intensity of the measurement light that has been irradiated and passed through the suspension L. It is. These devices 1, 2
The optical measurement section A is constructed from the following. The measuring device 2
is configured to be able to measure at the front position a and the rear position b of the suspension L with respect to the irradiation direction of the measurement light. To explain a specific example of this measuring device 2,
In the device shown in FIG. 1, light intensity sensors 3 are arranged at a plurality of positions on the circumference at appropriate distances from the suspension L, from the front position a to the rear position b of the suspension L. The measurement light intensity at a plurality of positions a and b is measured by each light intensity sensor 3. As another example of measuring light intensity at multiple positions as in this specific example, although not shown, a single light intensity sensor is moved continuously from the front position a to the rear position b. Measurements can also be made at one or more locations. Note that the minimum measurement position for the measurement light intensity is one point for each front position a or rear position b, but it may be configured so that measurements can be made at more points than that, as described below. The degree of freedom in measurement can be increased. Reference numeral 4 denotes a transparent storage section that stores the suspension to be measured, and this storage section 4 may be configured as an independent container, or as shown in FIGS. 2 and 8, It can also be constructed in part or for measuring a flowing suspension.
しかして第1図に示す構成に於いて、まずパル
プ繊維のモデルとして、繊維の径並びに長さを異
ならせたレーヨン繊維につき、前方位置aから後
方位置bに至る測定光強度の分布を測定すると第
3図a,bに示す如くなる。aは試料に入射する
測定光の光量を大とした場合、bは光量を小とし
た場合で、夫々後方、前方位置b,aに特徴が表
われており、かかる結果から測定光強度に及ぼす
繊維形態の影響は繊維の長さよりも、むしろ径の
大小に支配されることがわかる。このことから、
このような光学的測定により、繊維の径方向の変
化が測定し得ることがわかる。 However, in the configuration shown in Fig. 1, first, as a model of pulp fiber, the distribution of the measurement light intensity from the front position a to the rear position b is measured for rayon fibers with different fiber diameters and lengths. The result is as shown in FIGS. 3a and 3b. ``a'' is the case when the light intensity of the measurement light incident on the sample is increased, and ``b'' is the case when the light intensity is decreased.Characteristics appear at the rear and front positions b and a, respectively, and from these results, it is possible to determine the effect on the measurement light intensity. It can be seen that the influence of fiber morphology is dominated by the size of the diameter rather than the length of the fiber. From this,
It can be seen that such optical measurements can measure changes in the fiber's radial direction.
次いで広葉樹晒クラフトパルプを叩解し、CSF
が340、412、580(ml)の夫々に対して、パルプ濃
度が2、1、0.5(%)のパルプ懸濁液に対する前
述した測定光強度の分布を測定すると、第4図
a,b,cに示す如くなる。かかる測定結果か
ら、一定のパルプ濃度に於いては、CSFの変化に
より測定光強度に差が生じ、例えばCSFが少なく
なり、即ち叩解が進むにつれて後方位置bに於い
ては測定光強度が大きくなり、前方位置aに於い
ては逆に小さくなることがわかる。そこで以上の
夫々のCSFのパルプを原料として抄紙し、紙の物
性の一つを示す比破裂度を測定した結果は図中の
表に示す通りであり、即ち測定光強度の変化に対
応して強度が変化していることがわかる。このこ
とから一定のパルプ濃度に於いては、かかるパル
プ濃度に対応した叩解程度と測定光強度との対応
関係を予め測定して求めておくことにより、測定
した測定光強度から叩解程度を算出し得ることが
わかる。 Next, the hardwood bleached kraft pulp is beaten and CSF
When the distribution of the above-mentioned measurement light intensity is measured for pulp suspensions with pulp concentrations of 2, 1, and 0.5 (%) for 340, 412, and 580 (ml), respectively, the results are as follows in Figure 4 a, b, It becomes as shown in c. These measurement results show that at a constant pulp concentration, a difference occurs in the measurement light intensity due to a change in CSF. For example, as CSF decreases, that is, as beating progresses, the measurement light intensity increases at rear position b. , it can be seen that, on the contrary, it becomes smaller at the front position a. Therefore, paper was made using the above-mentioned CSF pulps as raw materials, and the specific rupture degree, which is one of the physical properties of paper, was measured.The results are shown in the table in the figure. It can be seen that the intensity is changing. Therefore, at a certain pulp concentration, by measuring and finding the correspondence between the degree of beating corresponding to the pulp concentration and the measured light intensity in advance, the degree of beating can be calculated from the measured light intensity. I know what I'm getting.
次にこのように算出されるパルプの叩解程度
は、前述した繊維の切断、圧潰、膨潤又は開裂の
どの因子を表わしているかを考察する。まず前述
した通り、レーヨン繊維による測定では、繊維の
長さの変化に対する測定光強度の変化は僅かであ
ることから、パルプに於いても繊維の切断の程度
は本発明に於ける叩解程度には含まれないと類推
し得る。第5図は叩解時のパルプ濃度を10%と30
%で行つた場合のパルプ懸濁液についての測定光
強度の、CSFに対する変化を示すもので、かかる
測定光強度はパルプ濃度が10%と30%のもので異
なることがわかる。ところでパルプ濃度30%程度
の条件で叩解したパルプは、いわゆる高濃度叩解
と称され、これは10%程度のパルプ濃度で叩解し
たパルプとは明らかに異なつた性質を示すもので
あり、即ち繊維の開裂が烈しく、著しい外部フイ
ブリル化を生じているものであり、従来の叩解程
度を示すCSFでは同一値を示すにも係らず、光学
的測定に於いては明確に識別可能である。 Next, it will be considered which factor of the above-mentioned cutting, crushing, swelling, or splitting of the fibers represents the degree of beating of the pulp calculated in this way. First of all, as mentioned above, in measurements using rayon fibers, the change in the measurement light intensity due to changes in fiber length is slight, so even in pulp, the degree of fiber cutting is smaller than the degree of beating in the present invention. It can be inferred that it is not included. Figure 5 shows the pulp density at the time of beating of 10% and 30%.
%, the measured light intensity for pulp suspensions is shown to change with respect to CSF, and it can be seen that the measured light intensity differs between pulp concentrations of 10% and 30%. By the way, pulp that has been beaten at a pulp concentration of about 30% is called high-concentration beaten pulp, and this shows properties that are clearly different from pulp that has been beaten at a pulp concentration of about 10%. The cleavage is severe and significant external fibrillation has occurred, and although they show the same value in conventional CSF, which indicates the degree of beating, they can be clearly identified in optical measurements.
これらのことから本発明に於いては、叩解程度
として、外部フイブリル化の程度を主体として測
定し得るものと見做すことができる。 From these facts, in the present invention, it can be considered that the degree of beating can be measured mainly based on the degree of external fibrillation.
本発明は前述の通り、パルプ懸濁液を経た測定
光強度の変化により、予めの測定により求められ
ている叩解程度と測定光強度との対応関係を用い
て、叩解程度を算出するものであるから、かかる
叩解程度の算出に際しては何らかの方法で測定光
強度の変化を求める必要がある。この変化を求め
る方法としては例えば、前方位置aあるいは後
方位置bのいずれかの側に於ける適宜位置(例え
ば図示例の測定条件の場合には、測定光強度の差
が最も顕著な角度150゜の位置)に於ける測定光強
度の値から求める、前方位置aあるいは後方位
置bのいずれかの側に於ける測定光強度分布を積
分して、積分値から求める、前方位置aあるい
は後方位置bのいずれかの側に於ける適宜の2つ
の位置に於ける測定光強度の比の値から求める方
法等の適宜の方法によつて求めることができる。
即ちこれら、、の方法は、夫々測定光強
度、積分値、比の値と叩解程度との対応関係を予
め測定して、マイクロコンピユータ等に於ける記
憶素子にデータとして用意しておくことにより、
測定時のこれらの値から容易に叩解程度の算出す
ることができる。尚、叩解度の差異に因る測定光
強度の差は、第4図の実施例に於いては測定光強
度のピークとなる角度140゜〜150゜の後方位置に於
いて顕著であるが、前述したレーヨン繊維に於け
る測定結果と同様に、測定光の光量を調節した
り、あるいは光強度センサ3のゲインを調節する
等により、測定光強度の差が顕著に表われる位置
を前方位置aまたは後方位置bのいずれの側とす
ることもでき、また前記光量やゲインが一定の場
合にも、被測定パルプ懸濁液の濃度に応じて、測
定光強度の差が顕著に表われる位置が前方位置a
になつたり、後方位置bになつたりするので、こ
れらの各条件に応じて前方位置aまたは後方位置
bの適宜の位置の測定光強度を用いることによ
り、高感度で高精度に叩解程度を算出することが
できる。例えば、測定対象たるパルプ懸濁液の濃
度が予めの測定等により分かつていて、これが変
化しない場合には、測定光強度の差が顕著に表わ
れる位置が予め分かるので、このような場合には
測定光強度測定装置2、かかる位置のみに於いて
測定光強度を測定し得る構成とすることができ
る。しかしながら、本発明では前方位置a及び後
方位置bの複数の位置で測定光強度を測定し得る
構成としているので、パルプ懸濁液の性状に応じ
て測定位置を適切に選択することができ、測定の
自由度を大きくすることができ、以つて精度のよ
り高い測定を行なうことができる。 As described above, the present invention calculates the degree of beating by using the correspondence between the degree of beating determined by previous measurements and the measured light intensity based on the change in the measured light intensity after passing through the pulp suspension. Therefore, when calculating the degree of beating, it is necessary to find a change in the measurement light intensity by some method. A method for determining this change is, for example, at an appropriate position on either side of the front position a or the rear position b (for example, in the case of the measurement conditions shown in the figure, at an angle of 150° where the difference in measurement light intensity is most significant). The front position a or the rear position b is determined from the integral value by integrating the measured light intensity distribution on either side of the front position a or the rear position b, which is determined from the value of the measured light intensity at the position of It can be determined by any appropriate method such as a method of determining from the value of the ratio of the measured light intensities at two appropriate positions on either side.
That is, in these methods, the correspondence between the measured light intensity, integral value, ratio value, and degree of beating is measured in advance and prepared as data in a memory element in a microcomputer or the like.
The degree of beating can be easily calculated from these values at the time of measurement. Incidentally, in the embodiment shown in FIG. 4, the difference in the measurement light intensity due to the difference in the degree of beating is noticeable at the rear position at an angle of 140° to 150°, where the measurement light intensity peaks. Similar to the measurement results for the rayon fibers described above, by adjusting the light intensity of the measurement light or the gain of the light intensity sensor 3, the position where the difference in measurement light intensity is noticeable is determined as the front position a. Alternatively, it can be on either side of the rear position b.Also, even when the light amount and gain are constant, there is a position where the difference in measurement light intensity appears significantly depending on the concentration of the pulp suspension to be measured. Front position a
The degree of beating can be calculated with high sensitivity and accuracy by using the measured light intensity at an appropriate position of front position a or rear position b depending on each of these conditions. can do. For example, if the concentration of the pulp suspension to be measured is known through prior measurement and does not change, the position where the difference in measurement light intensity will be noticeable can be known in advance, so in such a case, The measurement light intensity measuring device 2 can be configured to be able to measure the measurement light intensity only at such a position. However, in the present invention, the measurement light intensity can be measured at a plurality of positions such as the front position a and the rear position b, so the measurement position can be appropriately selected depending on the properties of the pulp suspension. It is possible to increase the degree of freedom of the measurement, and therefore, it is possible to perform measurements with higher accuracy.
次に第8図の符号Bは上記パルプ懸濁液の移送
経路Cに、上記光学的測定部Aに相前後して設け
ている音響的測定部を示すもので、この音響的測
定部Bは移送されるパルプ懸濁液に超音波を透過
させて、その減衰量を測定する超音波送受信装置
5,6を設けた構成である。 Next, reference numeral B in FIG. 8 indicates an acoustic measuring section which is provided in the transport path C of the pulp suspension, one after another to the optical measuring section A, and this acoustic measuring section B is The structure includes ultrasonic transmitting/receiving devices 5 and 6 that transmit ultrasonic waves through the pulp suspension being transferred and measure the amount of attenuation of the ultrasonic waves.
しかして、第6図は上記音響的測定部Bに於い
て2MHzの周波数の超音波に対する広葉樹晒パル
プの、パルプ濃度の変化に対応する減衰量を測定
した結果を示すものである。かかる測定結果よ
り、パルプ濃度が0〜2.5%程度の範囲では、パ
ルプ濃度と超音波減衰量とは、叩解程度によらず
ほぼ1つの直線状の対応関係を有することがわか
る。従つてパルプの種類等に対応して、かかるパ
ルプ濃度と超音波減衰量との対応関係を予め測定
して求めておくことにより、測定した超音波減衰
量からパルプ濃度を算出し得ることがわかる。こ
のようにしてパルプ懸濁液の移送経路Cに設置し
た音響的測定Bに於いてパルプ濃度を算出すると
共に、前記光学的測定部Aに於いて、前述した通
りパルプ濃度に対応した叩解程度と測定光強度と
の対応関係から叩解程度を算出することができ
る。 FIG. 6 shows the results of measuring the amount of attenuation corresponding to the change in pulp density of the bleached hardwood pulp against ultrasonic waves at a frequency of 2 MHz in the acoustic measuring section B. From these measurement results, it can be seen that in a pulp concentration range of about 0 to 2.5%, the pulp concentration and the ultrasonic attenuation amount have a substantially linear correspondence regardless of the degree of beating. Therefore, it can be seen that by measuring and finding the correspondence between the pulp concentration and the ultrasonic attenuation in advance according to the type of pulp, etc., it is possible to calculate the pulp concentration from the measured ultrasonic attenuation. . In this way, the pulp concentration is calculated in the acoustic measurement unit B installed in the transport path C of the pulp suspension, and at the same time, in the optical measurement unit A, the degree of beating corresponding to the pulp concentration is determined as described above. The degree of beating can be calculated from the correspondence with the measured light intensity.
次に以上の動作をより具体的に説明する。第7
図a,b,cはパルプ濃度0.5〜2.5%、CSF600〜
200(ml)のパルプ懸濁液について行なつた測定結
果を模式的に示すもので、叩解程度の差による測
定光強度の差は、角度150゜の後方位置bに最も顕
著に表われるものである。そしてこれら全ての図
に於いて実線は所定のパルプ濃度、叩解程度に於
ける分布、即ち基準状態に於ける測定光強度分布
を示すものである。aの破線は基準状態からパル
プ濃度だけが変化した場合即ちパルプ濃度が上昇
した場合の測定光強度分布を示すもので、前方、
後方位置a,bの測定光強度が互いに逆方向に大
幅に変化している。かかるパルプ濃度の変化は前
述したように音響的測定部Bに於いて測定するこ
とができるので、パルプ濃度と測定光強度との対
応関係を予めの測定により求めておくことによ
り、パルプ濃度の変化に起因する測定光強度の変
化を算出することができる。次にbの破線は定常
状態から叩解程度だけが変化した場合、即ち叩解
程度が進んだ場合の測定光強度分布を示すもの
で、後方位置bの測定光強度だけが上昇してい
る。パルプ濃度が一定の場合には、かかる測定光
強度の変化により、前述したように予め測定して
求めた叩解程度と測定光強度との対応関係を用い
て、叩解程度を算出することができる。更に、c
の曲線,並びには、曲線で示す基準状態
から、夫々濃度は変化せず叩解程度のみが進んだ
場合、叩解程度は変化せず濃度のみが上昇した場
合、並びに濃度の上昇と共に叩解程度が進んだ場
合の測定光強度分布を示すものである。このよう
にパルプ状態が曲線の状態から曲線の状態に
移行すると、前方、後方位置a,bの測定光強度
が共に互いに逆方向に変化する。しかして曲線
の状態では後方位置bに於ける測定光強度の変化
には、パルプ濃度並びに叩解程度の変化による変
化分の両方が含まれるので、これらを分離しなけ
ればならないが、本発明は前述した通り、音響的
測定部Bに於けるパルプ濃度の測定により、パル
プ濃度の変化に起因する測定光強度の変化を算出
し得るので、これらの分離を容易に行なうことが
できる。こうして本発明は未知の濃度のパルプ懸
濁液の叩解程度をも測定することができる。 Next, the above operation will be explained in more detail. 7th
Figures a, b, and c are pulp concentration 0.5 to 2.5%, CSF600 to
This diagram schematically shows the measurement results for 200 (ml) of pulp suspension, and the difference in measured light intensity due to the difference in degree of beating is most noticeable at rear position b at an angle of 150°. be. In all of these figures, the solid line indicates the distribution at a predetermined pulp concentration and degree of beating, that is, the measured light intensity distribution in the standard state. The broken line in a shows the measured light intensity distribution when only the pulp concentration changes from the reference state, that is, when the pulp concentration increases;
The measured light intensities at rear positions a and b change significantly in opposite directions. As mentioned above, such changes in pulp concentration can be measured in the acoustic measuring section B, so by determining the correspondence between pulp concentration and measurement light intensity through prior measurement, changes in pulp concentration can be measured. It is possible to calculate the change in the measured light intensity caused by the change in the measured light intensity. Next, the broken line b shows the measured light intensity distribution when only the degree of beating changes from the steady state, that is, when the degree of beating progresses, and only the measured light intensity at the rear position b increases. When the pulp concentration is constant, the degree of beating can be calculated based on the change in the measured light intensity using the correspondence between the degree of beating measured in advance and the measured light intensity as described above. Furthermore, c
From the reference state shown by the curve and the curve, respectively, cases in which the concentration did not change and only the degree of beating progressed, cases in which the degree of beating did not change and only the concentration increased, and cases in which the degree of beating progressed as the concentration increased. This shows the measured light intensity distribution in the case of When the pulp state shifts from a curved state to a curved state in this way, the measured light intensities at the front and rear positions a and b both change in opposite directions. However, in the curved state, the change in the measured light intensity at the rear position b includes both the pulp concentration and the change due to the degree of beating, so these must be separated. As described above, by measuring the pulp concentration in the acoustic measuring section B, it is possible to calculate the change in the measurement light intensity due to the change in the pulp concentration, so that these can be easily separated. Thus, the present invention can also measure the degree of beating of pulp suspensions of unknown concentration.
(発明の効果)
本発明は以上の通り、音響的測定部に於いて測
定したパルプ濃度を、光学的測定部に於ける叩解
程度の測定にフイードバツクすることにより、移
送経路を流れるパルプ懸濁液の叩解程度を、その
パルプ濃度が未知であつたり変動する場合でも算
出することができ、こうして外部フイブリル化を
主体とした叩解程度を移送経路に於いて非接触式
で高感度、高精度に測定することができ、従つて
製紙工程の各種処理工程に於ける制御並びに品質
の管理を良好に行えるという効果がある。(Effects of the Invention) As described above, the present invention feeds back the pulp concentration measured in the acoustic measurement section to the measurement of the degree of beating in the optical measurement section, thereby controlling the pulp suspension flowing through the transfer path. It is possible to calculate the degree of beating of pulp even if the pulp concentration is unknown or fluctuates, and in this way, the degree of beating mainly due to external fibrillation can be measured in a non-contact manner with high sensitivity and precision in the transfer route. Therefore, there is an effect that control and quality management in various processing steps of the paper manufacturing process can be performed well.
第1図並びに第2図は本発明方法の測定系を示
す説明図、第3図a,bは本発明方法の測定系を
用いたモデル繊維(レーヨン)の光学特性実測
図、第4図a,b,cは本発明方法の測定系を用
いたLBKPの光学特性実測図、第5図はパルプ濃
度を変化させた場合の光学的特性図、第6図はパ
ルプ濃度に対する超音波減衰特性図、第7図a,
b,cは叩解程度とパルプ濃度が変化した場合の
光学特性の状態変化を示すモデル説明図、第8図
は本発明の他の構成の説明図である。
符号A……光学的測定部、B……音響的測定
部、C……移送経路、L……パルプ懸濁液、1…
…測定光照射装置、2……測定光強度測定装置、
3……光強度センサ、4……収容部、5……超音
波送信装置、6……超音波受信装置。
Figures 1 and 2 are explanatory diagrams showing the measurement system of the method of the present invention, Figures 3a and b are actual measurement diagrams of optical properties of a model fiber (rayon) using the measurement system of the method of the present invention, and Figure 4a , b, c are actual measurement diagrams of the optical characteristics of LBKP using the measurement system of the method of the present invention, Figure 5 is a diagram of optical characteristics when the pulp concentration is changed, and Figure 6 is a diagram of ultrasonic attenuation characteristics with respect to pulp concentration. , Figure 7a,
b and c are explanatory diagrams of a model showing changes in the state of optical properties when the degree of beating and pulp concentration are changed, and FIG. 8 is an explanatory diagram of another configuration of the present invention. Symbols A...Optical measurement section, B...Acoustic measurement section, C...Transfer route, L...Pulp suspension, 1...
...Measurement light irradiation device, 2...Measurement light intensity measurement device,
3...Light intensity sensor, 4...Accommodating section, 5...Ultrasonic transmitter, 6...Ultrasonic receiver.
Claims (1)
光照射装置と、該懸濁液を経た測定光強度を、そ
の前方及び後方位置に於いて測定可能な測定光強
度測定装置とから光学的測定部を構成し、該光学
的測定部に於いて前記前方または後方位置に於け
る測定光強度を測定し、前記懸濁液の濃度に対応
する前記測定光強度と叩解程度との対応関係によ
り、叩解程度を算出することを特徴とする懸濁状
パルプの叩解程度測定方法。 2 被測定パルプ懸濁液の移送経路に、該パルプ
懸濁液に測定光を照射する測定光照射装置と、該
懸濁液を経た測定光強度を、その前方及び後方位
置に於いて測定可能な測定光強度測定装置とを設
けた光学的測定部と、前記懸濁液に超音波を透過
させて、その減衰量を測定する超音波送受信装置
を設けた音響的測定部とを構成し、前記音響的測
定部に於いて前記懸濁液による超音波の減衰量を
測定して、この減衰量とパルプ濃度との対応関係
により、パルプ濃度を算出すると共に、前記光学
的測定部に於いて前記前方または後方位置に於け
る測定光強度を測定し、前記音響的測定部に於い
て算出した懸濁液の濃度に対応する前記測定光強
度と叩解程度との対応関係により、叩解程度を算
出することを特徴とする懸濁状パルプの叩解程度
測定方法。[Claims] 1. A measurement light irradiation device that irradiates measurement light onto a pulp suspension to be measured, and a measurement light intensity that can measure the measurement light intensity that has passed through the suspension at positions in front and behind the measurement light irradiation device. A measurement device constitutes an optical measurement section, and the optical measurement section measures the measurement light intensity at the front or rear position, and measures the measurement light intensity corresponding to the concentration of the suspension and the beating. A method for measuring the degree of beating of suspended pulp, characterized in that the degree of beating is calculated based on a correspondence relationship with the degree of beating. 2. A measurement light irradiation device that irradiates measurement light onto the pulp suspension to be measured, and a measurement light irradiation device that irradiates the measurement light onto the pulp suspension to be measured, and is capable of measuring the intensity of the measurement light that has passed through the suspension at positions in front and behind the measurement light irradiation device. an optical measuring section equipped with a measuring light intensity measuring device; and an acoustic measuring section equipped with an ultrasonic transmitting and receiving device that transmits ultrasonic waves through the suspension and measures the attenuation amount thereof, The attenuation of the ultrasonic waves due to the suspension is measured in the acoustic measuring section, and the pulp concentration is calculated based on the correspondence between the attenuation and the pulp concentration, and the optical measuring section Measure the measured light intensity at the front or rear position, and calculate the degree of beating based on the correspondence between the measured light intensity corresponding to the concentration of the suspension calculated in the acoustic measuring section and the degree of beating. A method for measuring the degree of beating of suspended pulp.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60067552A JPS61226641A (en) | 1985-03-30 | 1985-03-30 | Beating degree measuring method for suspended pump |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60067552A JPS61226641A (en) | 1985-03-30 | 1985-03-30 | Beating degree measuring method for suspended pump |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61226641A JPS61226641A (en) | 1986-10-08 |
| JPH0465334B2 true JPH0465334B2 (en) | 1992-10-19 |
Family
ID=13348238
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60067552A Granted JPS61226641A (en) | 1985-03-30 | 1985-03-30 | Beating degree measuring method for suspended pump |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61226641A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7075865B2 (en) * | 2018-10-17 | 2022-05-26 | 株式会社日立製作所 | Optical analyzers, optical analysis methods, and optical analysis systems |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4839095A (en) * | 1971-09-20 | 1973-06-08 | ||
| JPS5341506A (en) * | 1976-09-29 | 1978-04-15 | Nippon Kamiparupu Kenkiyuushiy | Process and apparatus for optically measuring degree of beating by paper manufacture |
-
1985
- 1985-03-30 JP JP60067552A patent/JPS61226641A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61226641A (en) | 1986-10-08 |
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