This application claims priority under 35 § U.S.C. 119 to Chinese Application No. 02128861.5 filed Aug. 16, 2002, which is hereby incorporated by reference in its entirety for all purposes as if fully set forth herein.
The invention relates to an apparatus for weighing materials online, more particularly, relates to an apparatus for dynamically weighing materials transported on a conveyor.
Now two popular apparatus for online weighing are electronic belt scale and nuclear belt scale.
The common ground of the two apparatus lies in that both of them measure the load of materials on a conveyor belt and the speed of the belt, then get an instantaneous flux through multiplying the load by the speed, and finally obtain the cumulative weight of the material within a period of time through an integral or a summation operation.
The difference of these two apparatus lies in:
The electronic belt scale performs a contacting measurement by means of a pressure sensor, and determines the material load by measuring the weight of the material in a given area of the belt with a given length. If the flux is big, the accuracy of the electronic belt scale is high. But while the speed of the belt's movement is relatively high, the accuracy will decrease obviously. The electronic belt scale always has a huge size and a complicated structure, especially the one with better accuracy. And as it employs the contacting style measurement, the varieties of many factors can make great effect on measurement accuracy, such as change in tension of the belt, change in hardness of the belt and movement deviation of the belt. Therefore electronic belt scales need elaborate maintenance to keep steady accuracy.
The nuclear belt scale performs a non-contacting measurement, determining the material load by measuring the radiation absorption of the material. Nuclear belt scale has many features, such as, small volume, less maintenance and good stability. But under a condition of big flux and high load, due to the power limitation of a radioactive source, the intensity of the radiation having passed through the material and received by a detector is too low, which will influence the accuracy. Additionally, the changes in characteristics of the material, such as, the variety, composition, amount of water included and the change in the shape of a cross-section on the belt may influence the measurement accuracy. Therefore, nuclear belt scale has a low accuracy in general. And a complicated calibration needs to be done to ensure that the nuclear belt scale works well.
Although the nuclear belt scale and the electronic belt scale have their own advantages and disadvantages, they both can not meet the requirements of high precision and high reliability in some industries, such as metallurgy industry, chemical industry, and mining industry. It is an urgent affair to seek an online weighing apparatus with high precision, high stability, easy operation, and easy maintenance.
This invention is directed to a problem that a contacting online weighing apparatus depends too much on the stability of mechanism, and the disadvantages of a non-contacting online weighing apparatus, such as nuclear belt scale. And one object of this invention is to provide an online weighing apparatus which is simple in structure and in non-contacting style.
Another object of this invention is to make this online weighing apparatus not only work well in the case that a bulk density of the material is relatively constant, but also work well in the case that the bulk density changes largely, a high accuracy of the measurement is demanded at the same time and the speed of the belt is changeable.
For the first object, the online weighing apparatus of the present invention comprises: a light-emitting unit for emitting light beams to irradiate on a surface of the material transported on the belt to form bright projections in the same shape as that of the material; a CCD camera for continuously picking up images of the bright projections on the cross-section of the material; an image capture unit that connects to the CCD camera for continuously capturing the images; and a central processing unit that connects to the image capture unit for processing the images captured and computing the weight of the material.
For the second object, a speed sensor and a γ ray emitting and detecting apparatus are added to the invention.
The invention is explained in further detail, and by way of example, with reference to the accompanying drawings wherein:
Throughout the drawings, the same reference numerals indicate similar or corresponding features or functions.
The invention will be described in detail with drawings and the preferred embodiment.
The preferred embodiment of this invention is shown in
The laser source consists of a dot-spot laser 1 and a glass rod 2 to generate a line-spot fan-shaped laser beam 3, and the angle between the laser beam and the conveyor 6 is 45 degree.
The preferred embodiment of the laser source is shown in
A circuit diagram of the preferred embodiment is shown in
The following describes the weighing process of the embodiment of this invention in details with reference to
Before weighing, parameters for optical imaging part of the apparatus must be calibrated. Firstly, under the condition that there is no material on the conveyor, images of the bright projection projected on the conveyor 6 are picked up by the CCD camera, and then the shape and the position of the conveyor surface are determined as a nether contour of the cross-section of the material. When the material passes by on the conveyor, the position (pixel with the least gray) of the bright projection picked up by the camera, represents an upper contour of the cross-section of the material. The computer counts the number n of pixels between the nether and the upper contour of the cross-section. As shown in
If the bulk density of the material changes relatively large and a better accuracy of measurement is demanded, the γ ray emitting and detecting apparatus should be added in the apparatus of this invention. Therefore, the flux density I0 of the γ ray in a case that there is no material should be calibrated before practically measuring.
While practically measuring, the CCD camera 10 picks up images with a constant frequency, and sending the images to the computer via the image capture card. Supposing during a time interval T, N times of sampling are performed, the number of pixels between the nether and the upper contour of the cross-section of the ith sampling is denoted as ni, and the cross-section area of the ith sampling is denoted as Si. Si is calculated according to the pre-calibrated factor A by this equation: Si=A ni. The angle between the axis 8 and the plane of the fan-shaped beam 3, and the angle between the fan-shaped beam 3 and the conveyor 6 are both pertinent to the pre-calibrated factor A. If either of these two angles changes, the factor A must be calibrated again. Supposing the speed of the conveyor at the ith sampling is vi, during the time interval T, the volume V of the material passed by the conveyor can be calculated by this equation:
If the bulk density of the material is approximately a constant p, the mass M of the material passed by the conveyor during the time interval T is: M=ρV, the weight
wherein g is acceleration of gravity.
When the bulk density changes little or a common accuracy of measurement is demanded, the bulk density p of the material could be treated as a constant and be determined by calibration.
When the bulk density changes largely and a better accuracy of measurement is demanded, the γ ray emitting and detecting apparatus comprising the γ ray source 4, the γ ray detector 9 and the γ ray signal processing circuit 12 should be added to the apparatus of this invention. According to the attenuation law, the mass thickness of the material can be measured at the point where γ ray penetrates the material. Supposing the flux density of the γ ray is I when there is material on the conveyor under the condition of practical measurement. The mass thickness ρd of the material can be calculated according to the pre-calibrated I0 by the equation: ρd=K(LnI0−LnI), wherein the unit of ρd is usually g/cm2, and the constant factor K can be determined by calibration. When the computer analyses the images, the mean bulk thickness d of the material at the point of γ ray penetrating can be computed, so the bulk density ρ of the material is: ρ=ρd/d=K(LnI0−LnI)/d, therefore the precise weight of the material passed by the measuring point during an interval can be calculated by: W=Mg=ρVg.
Obviously, other light sources rather than laser source, and other forms of beams rather than fan-shaped beams can be employed in the volume measurement.
Through the detailed description in combination with the drawings, it is clear that as an non-contacting online weighing apparatus, the present invention asks for little demand on the mechanism stability of the conveyor belt, has a simple structure, and performs a stable measurement; this apparatus determines the bulk volume of the material by the CCD camera picking up the images of the cross-section of the material; and the optional γ ray source and γ ray detector system can be chosen to make the apparatus adapt to the condition that the bulk shape and the bulk density of the material vary greatly and obtain a better accuracy; and the optional speed sensor thereof makes the apparatus adapt to the condition that the speed of belt is not constant; and as the optional γ ray source is a point source with a low activity, easy to be shielded and with good radiation safety. These advantages of the invention make the apparatus have a wide use in chemical industry, metallurgical industry, mining industry and many other fields.
While the invention has been described in conjunction with specific embodiments, it is evident that many alternatives, modifications and variations will be apparent to those skilled in the art in light of the foregoing description. Accordingly, it is intended to embrace all such alternatives, modifications and variations as fall within the spirit and scope of the appended claims.
Number | Date | Country | Kind |
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02 1 28861 | Aug 2002 | CN | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/CN03/00680 | 8/14/2003 | WO | 00 | 2/16/2005 |
Publishing Document | Publishing Date | Country | Kind |
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WO2004/017030 | 2/26/2004 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
3278747 | Ohmart | Oct 1966 | A |
3545610 | Kelly et al. | Dec 1970 | A |
3796873 | Ledgett | Mar 1974 | A |
4147618 | Richardson et al. | Apr 1979 | A |
4238956 | Sniezek et al. | Dec 1980 | A |
4356874 | Blincow et al. | Nov 1982 | A |
4720808 | Repsch | Jan 1988 | A |
5099118 | Francis | Mar 1992 | A |
5184733 | Arnarson et al. | Feb 1993 | A |
5291422 | Esztergar | Mar 1994 | A |
5319160 | Nambu | Jun 1994 | A |
5561274 | Brandorff | Oct 1996 | A |
5585603 | Vogeley, Jr. | Dec 1996 | A |
5753866 | Ikeda et al. | May 1998 | A |
Number | Date | Country |
---|---|---|
03-41306 | Feb 1991 | JP |
9029693 | Feb 1997 | JP |
2000230809 | Aug 2000 | JP |
2002005637 | Jan 2002 | JP |
Number | Date | Country | |
---|---|---|---|
20050241862 A1 | Nov 2005 | US |