METHOD AND APPARATUS FOR DETERMINING THE FLOW VELOCITY OF A MOLTEN, RADIATION-EMITTING MATERIAL

Abstract: The invention is related to a method and an apparatus for measuring the flow velocity of a flow, stream or jet of molten radiation emitting material, in particular a freely falling jet of molten glass. The intensity of the radiation emitted from a limit­ ed section (2, 3) of the material flow is detected by means of two radiation detectors (S1, S2) at two separate locations mu­ tually spaced apart by a given distance (L) along the flow path of the material flow. All pulse-like amplitude variations having an amplitude exceeding a given magnitude are discriminated from the output signals of the two radiation detectors. These pulse-like amplitude variations originate from randomly occur­ ring, local, discrete, short variations in the intensity of the ra­ diation emitted by the material flow caused by randomly occur­ ring inhomogeneities in the material, for instance in the form of air bubbles in a jet of molten glass. The time interval between a pulse-like amplitude variation in the output signal from the up-­ stream detector (S1) caused by an inhomogeneity in the mate­ rial flow (1) and the occurrence of a pulse-like amplitude varia­ tion in the output signal from the down-stream detector (S2) caused by the same inhomogeneity in the material flow, is measured and used as a measure of the time taken by the mate­ rial flow to travel between the detector locations, for calculat­ ing the flow velocity of the material flow. Also the volumetric flow rate of the material flow can be determined by measuring also the diameter of the material flow with the aid of a linear array of photodiodes and calculating the volumetric flow rate on the basis of measured values of the flow velocity and the diameter.

Description: Method and Apparatus for Determining the Flow Velocity of a Molten, Radiation-Emitting Material The present invention relates to a method and a corresponding apparatus for measuring the flow velocity of a flow, stream or jet of a molten, radiation-emitting material. The invention has been made primarily for measuring the flow velocity of a freely falling jet of molten glass, but it can be used also for other molten, radiation-emitting materials, as ceramic or mineral materials and metals. A development of the invention concerns also measuring the volumetric or mass flow rate of a stream, flow or jet of molten radiation-emitting material by measuring the flow velocity as well as the diameter of the stream, flow or jet and calculating the volumetric flow rate on the basis of these measured data. As will be understood, when measuring the flow velocity of a molten material, there must be no mechanical contact with the material. Methods for measuring the velocity of movement of elongate solid objects, such as for instance wire, strip, paper-webs and the like, without mechanical contact with the object are previously known. In these known methods the moving object is provided with regularly spaced marks and a measuremnt is taken of the time taken for these marks to travel between two mutually spaced locations along the path of the moving object is measured. In this instance, these marks may comprise coloured dots on or locally heated sections of the object, such locally heated sections being provided by periodically irradiating the object by means of short radiation pulses from an IR radiation source. However, this method can not, of course, be used for measuring the flow velocity of a molten material which is itself radiative. It is also previously known to meausre the flow velocity of a liquid containing gas bubbles, by directing a light beam through the liquid flow at two mutually spaced locations, and by detecting the passage of gas bubbles in the liquid at these locations, so as to determine the travel time of the gas bubbles and thus the travel time of the liquid between said two locations. As will be understood, it is also impossible to use this method for determining the flow velocity of a molten material which is itself radiative, such as, for Instance, a freely falling jet of molten glass. In reality, there is no satisfactory known method for determining with sufficient accuracy the flow velocity of a stream, flow or jet of a molten radiative material, as for instance a freely falling jet of molten glass. The present invention relates to a novel and very satisfactory and advantageous method for this purpose. The method according to the invention is based on the discovery that a stream, flow or jet of a molten radiation-emitting material, such as molten glass in particular, emits radiation of such a character that when detecting radiation emitted from a limited section of the material flow, for instance by means of a suitable radiation detector, although the major part of the output signal from said detector will have a noice-character, the signal will also contain pulse-like, extremely large amplitude variations, which appear randomly in the signal. These short and large amplitude-variations in the output signal of the detector must find correspondence in local, discrete and randomly occurring variations in the intensity of the radiation emitted by the material, which variations are most probably caused by local, discrete, randomly occurring inhomogeneities in the material. In molten glass, these inhomogeneities probably consist of air bubbles in the molten glass, since it has been found that said pulse-like intensity variations in the radiation also appear with glass-materials with great purity. For other molten radiation-emitting materials, such as ceramic and mineral materials, similar gas or air bubbles are probably present and will give cause to similar, pulse-like, randomly occurring intensity variations in the emitted radiation. In molten metals there are also in most cases local, discrete inhomogeneities, for instance in the form of slag particles, which can give rise to similar pulse-like, randomly occurring intensity variations in the radiation emitted by the material. The invention is based on the assumption that these pulse-like, randomly occurring intensity variations in the radiation emitted by the material can be used to determine the flow velocity of the material, by detecting the radiation emitted from a limited section of the material flow at two mutually spaced locations along its flow path, and by measuring the time interval between the occurrence of such a pulse-like intensity variation at an upstream location and the occurrence of the same pulse-like intensity variation at a down-stream location. However, the fact that these variations in intensity occur completely randomly, and consequently with a varying mutual spacing in time, creates a serious problem when applying this measuring principle. In order to measure the flow velocity of the material correctly, however, it must be possible to determine the time interval between detections of exactly the same intensity variation at the two mutually spaced locations along the path of the flow. This is not easily achieved, as the intensity variations occur completely randomly and one intensity variation can not readily be distinguished from another intensity variation. One possible solution to this problem is proposed in Swedish patent application No. 800884-0. This proposed solution is based on the concept of measuring these time intervals only with respect to those variations in intensity which occur in the location of the upstream detector after a period of time has lapsed in which, no intensity varia +inns occurred, this time period positively exceeding the time taken for the flow of material to pass between the two detecting locations. This ensures, satisfactorily, that only the correct time-interval, and therewith the correct flow veloci-i correct flow velocity of the material, will be measured. The present invention relates to another method of solving the same problem. The method and corresponding apparatus according to the invention for determining the flow velocity of a stream, jet or flow of molten, radiation-emitting material have the characterizing features set-forth in following claims 1-4 and 7-9 respectively. A further embodiment of the invention relates to a method and corresponding apparatus for determining the volumetric flow rate if a stream, jet or flow of radiationemitting material having the characterizing features setforth in following claims 5-6 and 10-12 respectively. The invention will now be described in more detail with reference to the accompanying drawings, in which Fig. 1 illustrates schematically and by way of example the typical configuration of an output signal from a photodetector receiving radiation emitted from a limited section of a jet of molten glass; Fig. 2 illustrates schematically apparatus con- structed in accordance with the invention for measuring the flow velocity of a jet of molten glass; Fig. 3 is a diagram illustrating the principle on which the invention is based. Fig. 4 illustrates schematically apparatus according to another embodiment of the invention for measuring the diameter of a stream, flow or jet of molten radiationemitting material for determining the volumetric flow rate of the material; and Fig. 5 is a diagram illustrating the principles of operation of the apparatus illustrated in Figure 4. Fig. 2 illustrates schematically an embodiment of an apparatus according to the invention for measuring the flow velocity of a freely falling jet 1 of molten glass. The apparatus comprises two radiation detectors S1 and S2, which are spaced apart at a predetermined mutual distance L along the glass jet 1 and are arranged to receive, through a suitable optical system not shown in detail, radiation from two limited sections of the glass jet. Inthe drawing these two limited sections of the glass jet are schematically illustrated by hroken-line rectangles 2 and 3, respectively. Thus, these rectangles can be regarded as "viewing windows" for the radiation detectors S1 and S2, respectively. Each of the detectors provides an electric output signal having, in principle, the form illustrated by way of example in Fig. 1. Although the major part of this signal has the nature of a noise signal, it also comprises a plurality of randomly occurring, pulse-like, large amplitude variations P. These amplitude variations P are caused by randomly occurring, intensity variations of short duration in the radiation emitted by the glass jet 1. In turn, these intensity variations are most probably caused by randomly occurring air bubbles 4 in the glass material. When an air bubble passes the viewing window 2 or 3, it causes a pulse-like amplitude variation P in the output signal from the associated detector S1 or S2, respectively, the magnitude of this amplitude variation being dependent inter alia on the size of the bubble and its distance from the external surface of the glass jet 1. It will be realized that the time of travel of a given air bubble from the upstream viewing window 2 to the downstream viewing window 3 will be equal to the time taken for the glass jet 1 to travel the distance L, wherefore it can be used for determining the flow velocity of the glass jet in accordance with the expression V = L/T where V is the flow velocity and T is the travel time of the air bubble. Each of the output signals from the two detectors S1 and S2 are applied to a respective amplifying and signal processing circuit F1 and F2. Each circuit F1 and F2, respectively, discriminates from the output signal of the associated radiation detector any pulse-like amplitude variations P having an amplitude exceeding a predetermined amplitude level, for instance the amplitude level A in Fig. 1, and provides on its output a corresponding signal pulse P' for each such amplitude variation P. These signal pulses P' from the amplifier F1 are applied to the start input and to the stop-input respectively of a time measuring circuit R, which may comprise a digital counter driven from a clock pulse generator C. Thus, the time measuring circuit R is started by an air bubble 4 in the glass jet 1 passing the viewing window 2 of the upstream detector S1, and is stopped again as soon thereafter as an air bubble 4 passes the viewing window 3 of the downstream detector S2. When the time-measuring circuit R has in this way measured a time interval, it sends a ready signal to a calculating unit D, for instance comprising a micor-processor, which receives the measured value from the output of the time measuring circuit and at the same time resets said circuit. The time measuring circuit R is subsequently restarted as soon as an air bubble 4 passes the viewing window 2 for the upstream t detector S1. In order to ensure that the time interval measured by the time measuring circuit R actually corresponds to the travel time of the glass jet 1 over the distance L between the detectors S1 and S2, it is obviously necessary that the time measuring circuit R is started and stopped under the influence of precisely one and the same air bubble 4 in the glass jet 1. As will be understood,this will only be the case if there are no bubbles 4 present in the space between the viewing windows 2 and 3 at the time when a bubble passes the upstream window 2 and starts the time measuring circuit R. However, since the air bubbles 4 are completely randomly located in the glass jet 1, in the majority of cases bubbles 4 will be present, in practice, between the windows 2 and 3 when the timing circuit R is started by a bubble 4 passing the window 2. In these instances, the timing circuit R will be stopped prematurely by one of the bubbles already present between said windows 2 and 3, and hence the time interval measured by the timing circuit R will be too hsort. It may also be that the time interval measured by the timing circuit R is too long, for example when the bubble 4 which passes the upstream window 2 and initiates the timing circuit R does not, for some reason or other, pass the downstream window 3, e.g. because of irregular flow in the glass jet 1, and therewith does not influence the downstream detector SZ. In this case, the time-measuring circuit R will be stopped by a later, subsequent bubble 4 and the time interval measured will be too long. Despite these difficulties, however, it is possible by means of the calculating unit D, when practicing the invention, to obtain correct information concerning the "correct" time interval, i.e. the time taken for an air bubble 4, and therewith the glass jet 1, to travel the distance L between the viewing windows 2 and 3. According to the invention this is effected in that the calculating unit D receives from the time-measuring circuit R, and stores a large number of time intervals, for example 100 time intervals, measured in the manner described above. The calculating unit D is designed or programmed to sort or classify these measured time intervals with respect to their values, and to determine the most frequently occurring value of these measured time intervals received by and stored in the calculating unit. Thus the calculating unit D sets up a histogram of the kind illustrated in Fig. 3, in which histogram the horizontal axis represents the values of the measured time intervals in classes or groups each having a width of Xps, and the vertical axis represents the number of measured time intervals N within each class or group. It is found that this histogram displays a single distinct peak or maximum for the class or group within which the correct time interval is located, i.e. the class or group having the center value Yus in Fig. 3. Since the bubbles 4 appear completely randomly within the glass jet 1, the "erroneously" measured time intervals will be spread out along the time axis, mainly as too short time intervals, whereas all the correct measured time intervals will be placed at one and the same location along the time axis. This analysis of the measured time intervals received from the time measuring circuit 3 is performed automatically by the micro-processor in the calculating unit D, when this has received a predetermined number of measured time intervals, for instance 100. It has been found that such a distinct peak or maximum in the histogram is obtained, if the amount of randomly occurring bubbles 4 in the glass jet 1 is such that the distance between two mutually sequential bubbles, which both pass viewing windows 2 and 3 and give rise to signal pulses P' from the amplifiers F1 and F2, is greater than the distance L between the windows 2 and 3 in at least 8 to 10 % of all cases. The calculating unit D could, per se, use the center value Y for the largest class of measured time intervals according to Fig. 3 as the wanted value of the travel time of the glass jet 1 over the distance L between the windows 2 and 3, and consequently calculate the flow velocity of t the jet on the basis of this value in accordance with the expression given in the foregoing. However, greater accuracy is achieved, when the calculating unit D is designed and programmed in such a way that after having determined the value Y in the manner described above on the basis of a first plurality of measured time intervals, for instance 100, it accepts thereafter only such measured time intervals received from the time measuring circuit R as those which have values within a limited range on both sides of the value Y, ie. within the range Y+Z %. The calculating unit D thereafter collects a predetermined number for instance 100, of such accepted measured time intervals and calculates the mean value of these accepted measured time intervals. This mean value is then regarded as the correct value of the travel time of the glass jet 1 over the distance L between the viewing windows 2 and 3. Preferably, this mean value is updated, by calculating a new mean value for each new accepted measured time interval received from the time measuring circuit R, so that the mean value is always calculated on the basis of, for example, the last hundred accepted measured time intervals received. Further, the value Y is changed continuously, so as to be equal to the mean value last calculated, whereby the only measured time intervals arriving from the time measuring circuit R which will be accepted are those which have values within the range +Z % on both sides of the last calculated mean value. In this way the measuring process will automatically follow the variations in the flow velocity of the glass jet 1. Should the calculating unit not receive any acceptable measured time intervals from the time measuring circuit R during a predetermined period of time, the calculating unit D will restart the process from the beginning, and establish a new histogram according to Fig. 3 in the manner described above, in order to find a correct value of Y. This may, for instance, be necessary in connection with very rapid changes in the flow velocity of the glass jet. As mentioned above, it is sufficient if the number of "accept-ed", i.e. correct, measured time intervals from the time measuring circuit R is at least about 8 to 10 % of the total number of measured time intervals. This can be achieved by an appropriate selection of the distance L between the viewing windows 2 and 3, the size of the viewing windows and the magnitude of the threshold amplitude level A in the amplifiers F1 and F2 in relation to the number of air bubbles 4 present in the glass jet, and to the velocity of the glass jet, in such a manner that the mutual spacing in time between mutually sequential signal pulses P-' in each of the output signals from respective amplifiers F1 and F2 exceeds the travel time of the glass jet between the viewing windows 2 and 3 in at least about 8 to 10 % of all cases. It will be realized that if the distance between the viewing windows 2 and 3 is made smaller, then the spacing in time between mutually sequential signal pulses P' will increase relative to the time taken for the glass jet 1 to travel between the viewing windows. In a similar way, a reduction of the size of the viewing windows 2 and 3 will reduce the number of bubbles 4 passing these windows and influencing the detectors S1 and S2, wherefore the mutual spacing in time between mutually sequential signal pulses P' will increase for an unchanged total number of bubbles in the glass jet 1 and an unchanged flow veloctiy of the jet. In similar way, a larger threshold amplitude level A in the amplifiers F1 and F2 will reduce the number of signal pulses P' and consequently increase the mutual spacing in time between mutually sequential signal pulses P' for an unchanged total number of bubbles 4 in the glass jet and an unchanged flow velocity of the jet. As mentioned in the foregoing, an apparatus according to the invention can be further developed to determine not only the flow velocity of the material but also its volumetric flow rate, which is of interest in many fields of application, such as glass-fiber production, for example where it is important to be able to measure the volumetric rate of flow of the freely falling jet of molted glass down to the spinners. For this purpose it is necessary to determine the diameter of the#jet, in addition to its flow velocity. The diameter of the glass jet can advantageously be measured by means of such an apparatus as that illustrated schematically in Fig. 4. This apparatus comprises a linear array of photodiodes 5, which through a suitable optical system, not shown in detail in the drawing, is arranged to receive radiation emitted by the glass jet 1 along a line 6 which is perpendicular to the direction of flow of the glass jet. It will be appreciated that of the array 5 a number of diodes corresponding to the diameter d of the glass jet 1 will receive radiation from the jet 1, whereas the remaining diodes in the array will receive substantally only background radiation. The diodes in the array 5 are scanned or sensed periodically by means of a SLaililIng circuit 7, from which a series of signal pulses are obtained with each scan, the number of pulses obtained being equal to the number of diodes in the array, and each of which signals has an amplitude corresponding to the amount of radiation received by the respective diode since the immediately preceding scan. Consequently, the output signal of the scanning circuit 7 has the form illustrated by the diagram 1 in Fig. 5. This diagram shows the output signal of the scanning circuit 7 for two mutually sequential scans, and the total scanning time for the array 5 is designated Ta, whereas the pause between two mutually sequential scans is designated To. The scanning or sampling frequency is consequently l/Ta+To and is determined by a control circuit 8, which comprises, for instance, a voltage-controlled oscillator for determining the scanning frequency. The output signal of the scanning circuit 7 is applied to a digitizing circuit 9, which determines which pulses of the signal have an amplitude exceeding a predetermined level, for instance the amplitude level Al in Fig. 5, and which produces a square wave signal of corresponding duration, i.e. having the shape illustrated by the diagram II in Fig. 5. This square wave signal thus has a duration corresponding to that number of diodes in the array 5 which have received radiation exceeding a given level Al. This square wave signal is applied to a time-measuring circuit 10, for instance in the form of a digital counter driven from a clock pulse generator 11, which counter is kept running by the square wave signal from the circuit 9 and which consequently counts a number of clock pulses corresponding to the duration of said square wave signal. The clock pulses from the clock pulse generator 11 are illustrated in the diagram III in Fig. 5. The resulting count in the digital counter of the time measuring circuit 10 will consequently constitute a measure of the diameter d of the glass jet 1, and is supplied from the time measuring circuit 10 to a calculating circuit, which also receives the measured value of the flow velocity of the glass jet 1 and which calculates the volumetric flow rate of the glass jet on the basis of these measured values. The fact that there is no sharply defined border line between those diodes in the array 5 which receive radiation directly from the glass jet 1 and those diodes in the array which should theoretically receive only background radiation, creates a problem, however. This is apparent from the form of the signal illustrated by diagram I In Fig. 5 which shows that the output signals from the Individual diodes increase gradually at the "edges" of the glass jet 1. As a consequence, the number of diodes providing an output signal exceeding the threshold value Al will vary not only with the diameter of the glass jet 1 but also with the radiation intensity of the glass jet, i.e. with the temperature of the jet. An increased temperature of the glass jet will therefore give a larger measured value for the diameter, even if the diameter of the jet is in reality constant. According to the invention this measuring error is compensated for by applying the output signal of the scanning circuit 7 to a switch 12, which is controlled by the square wave signal from the circuit 9 in such a manner that it is closed only for the duration of this square wave signal, whereby only those output signals from the diodes of the array 5 which exceed the threshold level A1 are passed through the switch. These signals are applied to an averaging circuit 13 which determines the mean amplitude value of these signal pulses and supplies a corres#onding signal to a control circuit 14. In the control circuit 14 this mean value signal from the circuit 13 is compared with a reference value Ar and in response to this comparison the control circuit 14 provides a control voltage to the voltage controlled oscillator in the control circuit 8. In response to this control voltage the circuit 8 adjusts the scanning or sampling frequency for the array 5 in such a manner that the mean amplitude of the photodiode signals exceeding the threshold value Al is maintained constant and equal to the reference amplitude Ar. It will be appreciated that this is possible, since the amplitude of the signal pulses from the diodes of the array 5 increases when the scanning or sampling period Ta+To increases, since each diode will then have time to receive a larger amount of radiation between each scan. In this way there is obtained an automatic compensation of the diameter measurement for any variations in the temperature of the glass jet 1, and thus in its radiation intensity. In an apparatus according to the invention for measure ing both the flow velocity and the diameter cf a stream, flow or jet of molten, radiation emitting material the photodiode array 5 is preferably located between the two radiation detectors S1 and S2, whereby the velocity and the diameter will be measured at substantially the same location along the material flow.

Claims: Claims 1. A method for measuring the flow velocity of a flow, stream or jet of a molten radiation-emitting material, comprising the steps of a) detecting the intensity of the radiation emitted from a limited section of the material flow at two separate detecting locations, which are arranged at a given distance apart along the path of the flow, and generating corresponding electric signals, b) discriminating from said signals from said two detecting locations all pulse-like amplitude variations exceeding a predetermined amplitude, said amplitude variations originating from randomly occurring, local, discrete deviations in the intensity of the radiation of the material flow caused by the presence of local inhomogeneities in the material, c) repeatedly determining the time interval between the occurrence of one such amplitude variation in the signal from the upstream detecting location and the subsequent amplitude variation occurring nearest in time in the signal from the down-stream detecting location, d) establishing on the basis of a selected number of thus determined time intervals which value is the one which occurs most frequently for these time intervals, and e) considering said most frequently occurring value as the lime taken for the material flow to travel between said two detecting locations, and using said most frequently occurring value together with said given distance between the two detecting locations to calculate the flow velocity of the material flow. 2, A method as claimed in claim 1, characterized by, after having in step d) determined the most frequently occurring value of a plurality of time intervals measured according to step c), selecting from the continuously measured time intervals according to step c) only such time intervals as those which have a value lying within a given limited range on both sides of said most frequently occurring value, arid determining the mean value of a plurality of such selected time intervals, and using said mean value as a measure of the time taken for the material flow to travel between said two detecting locations when making the calculation according to step e). 3. A method as claimed in claim 2, characterized by, after having determined said mean value a first time on the basis of a given number of said selected time intervals, updating said mean value by again calculating for each new selected time interval a mean value of said given number of the latest selected time intervals, whereafter only such time intervals are selected as those which have values within said given value range on both sides of the last calculated mean value. 4. A method as claimed in any one of claims 1 - 3, characterized by so adapting the magnitude of said limited sections of the material flow and said distance between the detecting locations and said given magnitude of said amplitude variations to the occurrence of said inhomogeneities present in the material and to the flow velocity of the material flow that the mutual spacing in time between mutually sequential amplitude variations exceeding said given magnitude in said signals from said detecting locations exceeds the travel time of the material flow between said detecting locations in at least about 8 to 10 % of all cases. 5. A method for measuring the volumetric flow rate of a flow, stream or jet of a molten, radiation-emitting material, characterized by, in addition to measuring the flow velocity of the material flow by means of the method according to any one of claims 1-4, also measuring the diameter of the material flow and calculating the volumetric flow rate on the basis of said measured values for the flow velocity and the diameter. 6. A method as claimed in claim 5, characterized in that the diameter of the material flow is measured by a) using a linear photodiode array for detecting the radiation emitted by the material flow along a line perpendicular to the flow direction of the material flow, b) scanning said photodiode array periodically with - respect to the quantity of radiation received by each individual photodiode since an immediately preceding scan, c) determining after each such scan the number of photodiodes which have received a quantity of radiation exceeding a given value and using this number of diodes together with the mutual spacing between the diodes as a measure of the diameter of the material flow, d) also determining after each such scan the mean value of the radiation quantities received by said number of photodiodes, and e) controlling the periodicity of said scans of the photodiode array in such a way that said mean value is caused to correspond to a given reference value. 7. An apparatus for measuring the flow velocity of a flow, stream or jet of a molten radiation-emitting material comprising a) two radiation detectors (S1, S2) arranged to receive radiation emitted from a limited section (2, 3) of the material flow (1) at two different locations spaced apart by a given distance (L) along the flow path of said material flow, and to produce electric output signals corresponding to the intensity of said received radiation; b) for each radiation detector a signal-processing circuit (F1, F2) for discriminating from the output signal of said radiation detector only those pulse-like amplitude variations (P) which exceed a given smallest amplitude (A), and to produce corresponding signal pulses (P') on its output; c) a time measuring circuit (R) arranged to be started by one such signal pulse (Pl)originating from the upstream detector (1) and to be stopped by the nearest following signal pulse (P') in time originating from the downstream detector (S2) and to generate a measurrnng result represents ing the time interval between said signal pulses, and to then be restarted by a signal pulse (P') originating from the upstream detector (S1); d) a calculating unit (D) arranged to receive said measuring result from the time-measuring circuit (R) and to establish on the basis of a multiplicity of such measuring results the most frequently occurring value (Y) thereof, and to use the value as a measurement of the time taken for the material flow (1) to travel between the two detection locations, for calculating the flow velocity of said material flow. 8. An apparatus as claimed in claim 7, wherein said calculating unit (D) is arranged to accept, after having determined the most frequently occurring value (Y) of a multiplicity of measured time intervals received from said time-measuring circuit (R), only measured time intervals having values within a given value range (+Z%) on both sides of said most frequently occurring value, and to determine the mean value of a given number of such accepted measuring results and to use said mean value in said calculation of the flow velocity. 9. An apparatus as claimed in claim 8, wherein said calculating unit (D) is arranged repeatedly to update said mean value by calculating for each new accepted measured time interval received from said time-measuring circuit (R) a new mean value on the basis of said given number of accepted measuring results last received, and to accept only such measured time intervals having values within said given value range on both sides of the last calculated mean value. 10. An apparatus as claimed in claims 7 - 9 for determining also the volumetric flow rate of the material flow, characterIzed by means (5-14) for measuring the diameter (d) of the material flow (1), said calculating unit (D) being arranged to calculate the volumetric flow rate of the material flow on the basis of said measured values re preser. ng the flo-.. velocity and the diameter of the material flow. 11. An apparatus as claimed in claim 10, characterized in that said means for measuring the diameter (d) of the material flow (1) comprise a linear array of photodiodes (5) arranged to receive radiation emitted by the material flow (1) along a line (6) perpendicular to the direction of flow, means (7) for scanning this array of photodiodes (5) periodically with respect to the amount of radiation received by each individual diode in the array since the preceding scan, means (9, 10, 11) for determining after each scan the number of diodes having received an amount of radiation exceeding a given level (Al) and for giving to said calculating unit (D) a measurement value representing said number of diodes, the calculating unit being arranged to utilize said measurement value as a measure of the diameter (d) of the material flow (1) in the calculation of the volumetric flow rate of the material flow, means (13) for determining the mean value of the radiation quantities received by said number of diodes, means (14) for comparing said mean value with a reference value (Ar), and means (8) responsive to said comparison for controlling the periodicity of said scanning of said photodiode array (5) in a manner such that said mean value is caused to correspond to said reference value. 12. An apparatus as claimed in claim 11, characterized in that said photodiode array (5) is arranged to receive radiation emitted by said material flow (1) at a location between said two locations (2, 3) where said radiation detectors (S1, S2) receive radiation emitted by the material flow.

Inventors: HOLMGREN, PER, RANSHEIM, ANDERS P., THOMSEN, ARNE
Applicants: GULLFIBER AB
Application year: 1983
Main classification: G01P5
IPC codes: G01F1, G01P5