US 4,220,499 AGrant
Method for Determining the Relative Quantity of Shives in a Stream of Fibrous Particles
Issue Date:1980-09-02
•4 Claims
•4 Drawing Sheets
Abstract
Relative shive incidence in a production flow line of paper pulp is continuously sampled and measured by means of a continuous flow, fiber induction device located within the production line to extract a diluted sample of fiber flow therein. The diluted sample is directed through a windowed conduit section for photodetection of particles therein. Particle caused pulses are discriminated by amplitude relative to a reference scale to distinguish shive particles from acceptable fiber particles. Two pulse trains are developed simultaneously: one pulse train for shive pulses and the other pulse train for particle flow including shives. Both pulse trains are rate determined by counting the number of pulses in a fixed interim of time identical to both. The two pulse rates are then combined to develop a dimensionless ratio of shive incidence or percentage within the total fiber stream.
Metadata
Assignee
- Westvaco Corporation
Inventors
- Horatio Hughes, Jr.
- Robert A. Schilling
Application Information
Application Number:US 9485902
Filing Date:1978-10-04
Priority Date:1977-07-01
Art Unit:173
Classifications
IPC:
G01N 110G01N 1502
Field of Search:
16235623532425073364DIG. 10;49;198;262;238;243;50102;208;335;44292 PC71 CP222 PC422 R;63471;555
Patent Drawings (4 sheets)
Description
Background of the Invention
1. Field of the Invention
The present invention relates to the art of qualitatively measuring the properties of wood pulp in a dilute stock slurry. More specifically, the present invention relates to a method and apparatus for photometrically identifying the percentage of shives in a stock flow stream.
2. Description of the Prior Art
As a broad generalization, the process of pulping wood for papermaking comprises a series of chemical and mechanical steps to disintegrate the natural state of wood into individual or small bundles of cellulose fiber. However, since wood is not a homogenous material, the standardized or uniform process of an industrialized pulp flow stream does not have the same result on all elements of a tree.
One particular notable natural wood anomaly is the occurrence of fiber bundles bound together by transverse ray cells. A singular, consolidated bundle grouping is known to the papermaker as a "shive". Such transversely bound bundles are extremely tenacious in their resistance to defiberizing processes.
Although wood pulp is normally screened one or more times along the process stream, it is impossible to segregate all shives having 4-8 mm length and 100 to 140 .mu.m width from acceptable fiber bundles of less than half the shive size. Nevertheless, it is important to the papermaker that the presence of shives be maintained below a certain percentage quantity in the stock due to their consequential deleterious effect on a paper web.
The generally practiced industry technique for monitoring the relative presence of shives in a pump stream is to periodically count, manually, the individual shive incidence in a standard area, randomly selected, sample of paper made from the pulp. This practice, of course, is extremely time consuming and occasions a large delay interim between the time that pulp lands upon the papermachine and knowledgeable recognition of the relative shive incidence. Consequently, it is not unusual that machine operators will be plagued with web breaks and unacceptable paper quality due to excess shives long before the cause of the trouble is known.
Recently, work has begun on the development of more timely techniques for shive monitoring. One published report of such work is found in the October, 1975 journal of the Technical Association Of The Pulp and Paper Industry (TAPPI, Volume 58, No. 10, page 120. This report describes an optical detector which passes two perpendicularly disposed light beams in a common plane transversely through a windowed conduit carrying a pulp sample stream. Respective photodetector responses to the shading effect of fibers crossing the beam paths are measured to yield a length, width and thickness determination for each fiber. By means of internally programmed limits, the events of a passing shive may be immediately identified and counted. The frequency of such shive counts is compared to the consistency and flow rate of the sample which must be carefully controlled.
Although the aforedescribed optical shive counter manufactured by Tellusond of Stockholm, Sweden, is extremely accurate, it is still a laboratory device which requires the isolation of a pulp sample from the production flow stream for accurate consistency and flow rate control.
Stock consistencies in a production flow stream are maintained in the range of 1 to 4% based on dry fiber weight. However, the Tellusond shive counter requires a batch quantity stock sample accurately measured to 0.01 g/l and a 10 minute processing period for each batch. These circumstances dictate an instrument preparation procedure which includes withdrawal of an adequate stock quantity of substantially unknown consistency from the production line, analyzing the sample for total fiber content and accurately mixing a sufficient stock quantity to an accurately known consistency. This procedure may be mechanized for an automatic sampling and measuring cycle but the necessary support apparatus is elaborate and subject to considerable maintenance.
U.S. Pat. No. 3,461,030 to M. A. Keyes describes a different type of wood pulp slurry measuring device which relies upon the dielectric quality of cellulose to impose a voltage variation between two electrodes as fibers suspended in a known electrolyte are passed therebetween. Similar to the Tellusond optical device, the Keyes instrument integrates a cross-sectional area measurement of an individual fiber with a transit time measurement to derive a volumetric conclusion. Consistency of the slurry is obtained by combining the fiber volume conclusion with a simultaneous slurry volume measurement. Although the Keyes instrument is disclosed in the context of a consistency measuring instrument, it is conceivable that it may be adapted to shive measurement simply because it obtains a quantitative measure of individual fiber or particle volume. Nevertheless, the inventor did not disclose a recognition of this capacity or how such an adaptation may be devised.
In light of such aforedescribed prior art, there heretofore remained a need for an instrument that will continuously measure the relative presence of shives in a mill production stock flow stream. The specification of this need by the pulp and papermaking industry is further complicated by the absence of a satisfactory pulp sampling technique that is simple, continuous and relatively maintenance free.
Cellulose fibers have an unusually high affinity for adhesion to each other and to foreign surfaces. Any surface exposed to a pulp stream is quickly coated with a layered growth of fiber. This growth continues until other forces such as gravity or fluid shear exceed the adhesion strength of the fiber bond thereby causing a breaking off of an accumulated quantity. Consequently, maintenance of a continuous flow stream of pulp is a scalar and velocity design problem. Relatively small pipelines will be quickly plugged by fiber accumulations if not self-cleaned by an appropriately high flow velocity. For these reasons it is difficult to continuously extract from a large production line a small but representative sample of pulp for testing purposes. Accordingly, it is also an objective of the present invention to teach a method and apparatus for continuously extracting a low quantity pulp sample that is representative of the primary flow stream but will not plug.
Brief Summary of the Invention
The present invention accomplishes these and other objectives by means of a continuous pulp sample extraction device which directs a fiber-free water stream across an open gap within a large production flow stream of pulp into a sample extraction conduit. Pressure on the fiber free water stream is significantly higher than the production line pressure to maintain a relatively low energy loss across the open gap. Principles of fluid flow induction draw pulp fiber from the production stream in the proximity of the gap to be carried along the extraction conduit. Although consistency dilution occurs, the sample extraction flow stream is sustained at a substantially constant flow rate, therefore, the quantity of pulp extracted at any given moment may be directly related to the momentary production stream consistency.
For purposes of shive monitoring the sample extraction flow stream is adjusted to provide an approximate 0.05% pulp consistency although this value is not particularly critical. A consistency of 0.1% or less is suitable.
The dilute sample is then conducted past a photometric window between a light source and a single photodetector having an approximate 1/2 inch (1.25 cm) flow channel gap therebetween.
Voltage measuring devices signify both the event of a passing fiber or shive and the relative size thereof due to the particle shadow on the detector. The magnitude of voltage response to such passing shadows is directly related to the size of the shadow and hence, the size of the particle. Since shives are significantly larger than acceptable fiber bundles, the detector voltage responses may be segregated accordingly by appropriate signal discriminating devices.
Simultaneously, signals proportional to the absolute or total particle flow rate are ratioed with the total shive flow rate to yield a signal that is directly proportional to the shive density in the sample stream.
Accurate knowledge of sample consistency is irrelevant since the invention relates a first counted number of particles to a second counted number of shives, the first number being inclusive of the second number. Consequently, the absolute quantity of these numbers in the sense of consistency or dry pulp quantity per unit slurry volume is unnecessary to conclude the desired objective of shive density.
Accordingly, a continuous indication of shive density may be reported in such form as to automatically actuate appropriate alarms when the density exceeds acceptable limits. Moreover, the point in the production flow stream at which the sample is extracted may be selectively chosen sufficiently far upstream of the papermachine headbox so as to provide adequate time for evasive or corrective action before a high shive density increment of pulp enters the headbox.
Brief Description of the Drawing
Relative to the drawing wherein like reference characters designate like or similar elements throughout the several figures:
FIG. 1 is a piping schematic for the present pulp sampling system;
FIG. 2 is a longitudinal section view of the photodetecting window section of the continuous flow sample stream;
FIG. 3 is a cross-sectional view of the sample stream window taken along cut lines III--III of FIG. 2;
FIG. 4 is a signal flow schematic for the electronic portion of the meter;
FIG. 5 schematically illustrates an alternative portion of the basic FIG. 4 signal management system.
FIG. 6 schematically illustrates a digital signal embodiment of the system; and
FIG. 7 is a comparative performance graph for the subject invention.
Description of the Preferred Embodiment
The mechanical schematic of FIG. 1 illustrates the sample extraction system of the invention which may be inserted through a single aperture 11 in a production stock line pipe or vessel wall 10. The wand 13 of the extractor comprises a small conduit 14 for the delivery of fiber-free water at a relatively constant flow rate to a discharge nozzle 15 which is axially aligned with a square cut opening 16 of extraction conduit 17.
A gap 18 is provided between the tip of nozzle 15 and opening 16. This gap 18 is positioned centrally within the stock line 10 to be swept by a representative flow of the stock therein. Regarding cross-sectional placement of the gap 18 within the production line, the usual instrumentation caveats apply such as avoidance of flow stagnation regions in pipe bends and near the side walls.
Grommet 19 provides a fluid pressure seal of the aperture 18 around the conduits 14 and 17.
There is little criticality in the design parameters of the sample extraction system except that the clear water supply pressure in conduit 15 should be substantially greater than that of the stock line pressure. The system bears resemblance to a conventional jet pump or aspirator except for the gap 18. In the case of jet pumps and aspirators, release of the energy carrying jet stream occurs within the boundary confines of a larger volume induction chamber to provide a localized low pressure zone having communication with the induced fluid. None of the energy carrying induction fluid is lost from the flow system and no intermingling of the induced and induction fluids occurs outside of the induction chamber boundary. In the case of the present invention, intermingling of the induced and induction fluids occurs in the relatively infinite volume of the induced fluid vessel. Moreover, induction fluid may be, and in all probability is, lost from the total flow stream. Although energy efficiency of the present invention is less than that of jet pumps and aspirators, this circumstance is, in absolutes, insignificant or irrelevant to the objective of extracting a low volume sample flow from the 1% to 4% consistency main stream 10 free of pipe plugging concerns.
In a representative actual use of the invention, a 1/4 inch conduit 15 carrying a 1 gpm flow rate at 50 psi discharged a jet stream across a 3/4 inch gap 18 through and transversely of a 4.5% consistency, 0.5 psi pulp flow stream into the bare open end of a 1/4 inch conduit to lift an approximately 0.5 to 1.0% consistency pulp sample through a 10 foot head.
Of course, system designs may be optimized from the perspective of minimum energy loss across the gap 18 and maximum total head and velocity within the extraction tube 17. However, from the specific example described, simple experimentation will usually provide an operative system suitable for the following objectives.
As a further note to the sample extraction system, the described circumstance of jet stream discharge nozzle 15 having the same dimensional size as the sample line 17 capture opening 16 should not be considered as a limiting specification since relatively larger area capture openings 16 are known to operate well and in some circumstances, with greater efficiency. Similarly, divergent capture openings 16 have been successfully utilized. Such divergent opening arrangements are physically configured to a convergent-divergent venturi with the throat region removed to accommodate the mixing gap 18.
The extracted sample flow in conduit 17, if within the broad consistency range of less than 0.1% tolerated by the shive meter, may be delivered directly through a transparent window pipe section 30 between a light source 31 and a photodetector 32. Should consistency of the extracted stock sample prove greater than the suggested maximum, additional dilution water may be added at a mixing point 33.
The window section 30 of the sample line 29 shown by FIGS. 2 and 3 may be simply devised from a short section of 1/2 inch i.d. thermoplastic tubing having a heat formed section 33 with generally parallel opposite side walls 34. To the outer surface of these parallel side walls 34 are bonded light source and detector elements 31 and 32. Prototype instruments used on Optron Inc., 1201 Tappan Circle, Carrollton, Tex. 75006, OP214 LED light emitting diode for the light source 31 and a corresponding Optron Inc. OP603 light responsive diode for the detector 32.
Signal processing circuitry for the invention is schematically represented by FIG. 4 which shows the variable amplitude, direct current signal output of the sensor 32 first received by an amplifier A1 which increases the signal strength to a suitably higher value. National Semiconductors Ltd. of 331 Cornelia St., Plattsburgh, N.Y. manufactures an amplifier model LM 747 suitable for use in the A1 application.
The average d.c. value signal output of amplifier A1 is inverted and further amplified by an amplifier A3 such as the National Semiconductors model LM 751CV to power the light source 31 in such a way that a constant or steady-state average quantity of light is maintained on the sensor 32 notwithstanding water color, internal surface slimeing of the sample tube 29 or ageing of the light source 31.
Capicitance C filters the total signal from amplifier A1 to pass only pulse constituents due to shadows across the sensor 32 when particles in the slurry pass between the source 31 and sensor 32.
Amplifier A2 further magnifies the filtered pulse signal for amplitude discrimination by comparative amplifiers CP1 and CP2. These amplitude comparison devices are of a type such as the National Semiconductors model LM 319D which compare each incoming pulse from amplifier A2 with a predetermined reference value r1 and r2, respectively, and emit a corresponding pulse only if the incoming pulse equals or exceeds the reference value. In the present invention, the reference value of r1 is set four to five times greater than the values of r2 so that CP1 will transmit only those high amplitude pulses which signify the passage of a shive. Simultaneously, the value of r2 is set so that CP2 will transmit pulses representative of both fiber and shives.
Respective outputs from the comparative amplifiers CP1 and CP2 are conducted to pulse generators PG1 and PG2 such as the Signetics Corp., Wolf Rd. and Arques Ave., Sunnyvale, Calif., 555 timer which emits a constant amplitude, constant width, square wave pulse in response to each variable width, pulse received. These sqaure wave pulses are repetitively averaged over brief intervals, 50 seconds for example, by amplifiers A4 and A5 such as the Analog Devices Inc., Rte. 1, Industrial Park, P.O. Box 280, Norwood, Mass. 02062, AD 504 J which provides an analog responsive voltage variation proportional to the instant pulse receipt rate. At this juncture, the variable voltage signal of amplifiers A4 and A5 may be assigned a dimensional proportionality such as volts per shive per second in the case of A4 or volts per particle per second in the case of A5. These dimensions correspond to the fact that the momentary flow rate of both shives and total particles is being determined by an absolute event count over a brief time interval. The voltage of amplifiers A4 and A5 directly corresponds to the magnitude of the event count.
These voltage signals from the amplfiers A4 and A5 may be directly combined in a division function by ratio circuit R such as an Analog Devices Inc., supra, AD530 which delivers a DC voltage signal proportional to the shive flow rate divided by the particle flow rate, a dimensionless value of the stated objective.
This dimensionless ratio signal may be further amplified by A6 to proportionately actuate an appropriately calibrated meter 40 or chart recorder 41.
Similarly, the ratio signal may be processed by a voltage comparison circuit CP3 similar to those of CP1 and CP2 which actuates an alarm 42 when the ratio signal value rises above an acceptable reference magnitude r3.
A digital signal management technique suitable for the present invention is represented by FIG. 6. As in the FIG. 4 analog system, comparative amplifiers CP1 and CP2 issue a pulse for each shive and particle, respectively. Responsive to a particle pulse train of n fiber pulses received by digital counter DC 2, a gate pulse g.p. is issued to digital counter DC1 which is simultaneously counting the receipt of shive pulses. The beginning and end of gate pulse g.p. are used to start and stop the counting function of DC1.
At the end of each gate interval, the accumulated shive count in DC1, which represents the number of shives per n fiber particles, is transferred to a latch and display module DD1. Receipt of the shive count by DD1 initiates transmission of a reset signal to the counters DC1 and DC2 from a reset generator RG thereby resuming the particle and shive pulse counting interims.
This FIG. 6 digital embodiment of the invention provides the papermaker with a digital display of the objective dimensionless shive ratio.
Another signal management technique adaptable to the invention relates to a logarithmic scale of relative shive incidence. A logarithmic standard for acceptable pulp is subjective in that a plurality of pulp grade ranges are established above a worst-condition reference grade. Such a standard may begin with a sample of the highest shive incidence pulp a particular mill is known to produce. A standard handsheet is formed from this first sample and retained for future reference.
A portion of the first sample is diluted with shive-free pulp at some convenient ratio, 1:1 for example, to obtain a second sample from which a second, reference handsheet is formed and retained.
This process is repeated until a handsheet is formed which represents the lowest shive incidence pulp the mill is known to produce.
Although any dilution ratio may be used, the 1:1 ratio example represents a logarithmic system to the base 2 wherein each grade above the reference has half the absolute number of shives as the next grade lower. Distinctive about the log base 2 scale is that the human eye can consistently discern and accurately classify a handsheet from an unknown sample by mere visual comparison with the retained reference samples. Moreover, the degree of accuracy obtained is sufficient for most papermaking purposes.
Relating the present invention to such a shive incidence standard simply involves insertion of a log circuit L of the desired base in the signal flow stream following the ratio circuit R as represented by the dotted line arrow in FIG. 4. Such circuits are standard modular components of the type manufactured by Analog Devices Inc., supra, as catalog number AD755.
By converting the arithmetic ratio of shive incidence in a stock flow stream to the logarithm of that ratio, the total response scale of the instrument is greatly reduced and thereby more meaningful for production line consideration.
Another obvious variation of this theme, shown by FIG. 5, is to convert the output signal of both A5 and A6 to proportional log functions by circuit modules L1 and L2 such as the Analog Devices AD756P similar to L above and merely subtract, by means of a simple summing circuit .epsilon., one signal from the other. The resulting difference is the same logarithm of the arithmetic ratio described above.
The graph of FIG. 7 represents typical performance of the invention as applied to a mill production stock stream. The graph ordinate scales laboratory determinations of shive incidence in a given pulp sample by skilled personnel. The graph abscissa scales the response of the subject invention to the same pulp sample. Comparison with the ideal correspondence rate illustrated by the dashed line testifies to the invention accuracy over a widely varying range of shive incidence.
In summary, therefore, the invention provides a direct, continuous sampling technique for extracting a representative fraction of a production flow stream for test purposes.
The shive meter, per se, detects and counts particles passing the window zone 33 by virtue of the shadow cast thereby on the photodetector cell 32. Simultaneously, shadows due to shives which are at least four times as great as shadows due to acceptable fiber bundles are discriminated exclusively on the basis of shadow size in a single light plane without regard to total volume.
Signal management techniques filter and screen the composite signal from the photodetector to separate base level d.c. from the pulse values caused by passing particle shadows. Whether the particle source of the passing shadow was a shive or a fiber bundle is determined by the relative amplitude of the consequent pulse. Total particle pulses are inventoried along one signal line whereas shive particle caused pulses, simultaneously included with the total inventory, are separately inventoried along another, parallel signal line.
The number of pulses in each signal line is counted over a fixed time interval identical to both lines. Thereby, corresponding pulse rates are provided. Division of one pulse rate by the other provides a dimensionless ratio between the two as a quantified indication of the relative shive incidence in the flow stream.
Note will be taken that this approach to the objective is independent of stock consistency beyond the point that two or more particles will cast a single shadow on the detector. This circumstance occurs with consistencies of greater than 0.1%. Therefore, so long as the sample consistency is less than 0.1%, consistency or flow rate variations are immaterial.
Claims
Having fully described our invention, we claim:
1. A method of determining the relative quantity of shives in a flowing primary stream of fibrous particles comprising the steps of: continuously extracting a representative sample flow stream of fibrous particles within said flow stream; adjusting the consistency of said sample flow stream during said extraction to 0.1% or less; conducting said consistency adjusted sample stream past a photodetector; obtaining a composite first signal flow from said photodetector comprising a variable amplitude pulse continuum wherein each pulse represents the passage of individual fibrous particles past said photodetector, the magnitude of such amplitude variations being directly proportional to the size of said fibrous particles; obtaining a second signal flow of pulses from said first signal flow wherein each pulse in said second signal flow represents a pulse in said first signal flow having an amplitude greater than a reference amplitude; setting said reference amplitude to a value representing the minimum size of a shive particle; generating first and second time rate analog signals from each of said first and second signals by counting the number of pulses respectively therein within a common time interval; and, combining said first and second time rate analog signals to obtain a ratio therebetween and emitting a signal proportional to the ratio.
2. A method as described by claim 1 wherein said sample extracting step comprises the steps of continuously inducting fiber from said flowing stream by jetting a relatively high pressure, low volume stream of fiber-free water across an unconfined gap within said particle stream into a sample extraction conduit opening.
3. A method as described by claim 1 wherein said composite first signal flow also comprises an average d.c. value proportional to a steady-state quantity of light received by said photodetector, said method comprising the step of regulating the emissive intensity of a light source for said photodetector to maintain said average d.c. value.
4. A method as described by claim 1 wherein said ratio between said first and second time rate analog signals is obtained from an arithmetic difference between corresponding log functions of said respective time rate signals.
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|---|---|---|---|
| US3461030 | 1969-08-01 | Keyes | |
| US3626166 | 1970-04-01 | Berg | |
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| US3724957 | 1973-04-01 | Tamate et al. | |
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| US4018089 | 1977-04-01 | Dzula et al. | |
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| US4037966 | 1977-07-01 | Hill | |
| US4066492 | 1978-01-01 | Hill |
Non-Patent Literature (2)
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