Abstract:
A method and apparatus for the continuous determination of the flow rate and/or total weight of dry particles, measuring the speed imposed to a movable member by dry particles falling thereon.

Description:
FIELD OF THE INVENTION 
     The instant invention relates to a. method for determining the weight flow rate of dry particles while falling, almost without interruption, from ahigh location, and its further addition in order to obtain the final weight. Besides, one of the operating embodiments is disclosed through which measurement of parameters not easily attained through other methods is obtained. 
     BACKGROUND OF THE INVENTION 
     The method and steps thereof are based on a practical and economical need in those places lacking platform scales (since they are fixed and expensive) or, where continuous measurement of the weight flow rate of dry particles is required, without accumulating the material into bins or hoppers. 
     The apparatus is specially adapted for weighing grain such as wheat, soy, corn, etc, thus solving a concern of agricultural producers since by means of the use of the present method and apparatus, which allows the &#34;in situ&#34; weighing of the produced grain at a very low cost without requiring expensive storage facilities. 
     The advantages of the invention are: 
     Ease of transportation and assembly. Low weight. 
     Low cost 
     Accumulation of dry particles is not required, therefore dimensions are not dependent on the total amount to be weighted. 
     Operation: Classic physics explains the operation. The second Newton Law applied to rotating bodies states that: &#34;The Sum of Torques on an axis is equal to the product between the inertia momentum of the rotating body and its angular acceleration&#34;. Therefore, whenever a torque exists applied to a rotating body, the latter rotates with variable angular speed, proportional to said torque. In other words, if the resulting momentum is zero, the angular acceleration is also zero, and the movable body maintains constant its angular speed. 
     The measuring method and apparatus of the invention is based on the above principle. On one side, the driving torque caused by the dry particles falling on the vanes of the rotating wheel exists. If an antagonist torque directly proportional to the angular speed of the wheel is applied, a speed develops such that both torques are equal and, since are of different sign, the resulting force is null; therefore, at this point, the angular speed is constant as explained above. (Further, it is to be noted that in any practical system, there is a third torque, that caused by friction. This fact is taken into account by the electronic calculation system in order to compensate its influence). 
     Since the rotating speed of the wheel is a function of the driving torque, and this, in turn, depends on the instantaneous weight flow rate of the dry particles falling on the vanes, by measuring the instantaneous angular speed, the value of the weight flow rate of dry particles passing through the wheel at that moment may be obtained. 
     The antagonist momentum proportional to the angular speed is attained by means of an eddy current electromagnetic brake. 
     The subsystem for angular speed measuring, calculation and totalization the weight flow rate and display of results is comprised by a circuit the main element of which is a high scale integration electronic microcomputer. 
     The physical-mathematical development supporting the above follows: 
     Applying the second Newton Law to rotations 
     ΣCi=Ixα 
     wherein Ci represents the different actuating torques; I the inertia momentum of the movable element and α the angular speed. C m  being the driving torque caused by the grain falling; C r  that produced by friction on bearings, and C f  the braking torque produced by eddy currents, in this particular case, 
     
         C.sub.m -cr-C.sub.f =I×α 
    
     If ω is the angular speed, thus ##EQU1## then, 
     
         C.sub.m -C.sub.r =C.sub.f 
    
     Therefore, since the antagonist torque provided by the eddy current brake is C f  =K f  ×K f  being the proportionality constant depending on the element dimensions and magnetic induction of its magnets; the friction torque may be considered independent from the rotating speed for these rates; and due to the vane turbine and wheel theory, it may be considered with sufficient approximation, that ##EQU2## wherein Q p  is the dry particles weight flow rate, g is the gravity acceleration, N te  is the inlet tangent speed, N ts  the outlet tangent speed and Γ is the wheel effective radius; therefore ##EQU3## through mathematical calculation, and taking into account that ##EQU4## it is concluded that ω=f(Q p ) 
     Therefore, measuring the instantaneous angular speed of the wheel (this measure being obtained readily), the value corresponding to the weight flow rate of dry particles falling at that moment may be computed, with the aid of a computer and, by means of a simple integration, the total weight of dry particles passing through the vane wheel may be also calculated. 
     Since the braking constant Ks depends, among other parameters, on the resistivity of the disk material used in its construction, this, in turn, varies as a function of the temperature (room temperature as well as the temperature created by operation), according to the precision level desired, a temperature electronic measuring system and its automatic compensation in calculations carried out by the micro-controller is included. 
     The device described is one of the embodiments in which this process may be used, as shown in the attached drawings, as a non-limiting example. 
     The apparatus or equipment comprises four basic sub-systems: 
     1. Dry particles channelizing sub-system 
     2. Vane wheel rotating under dry particles falling influence. 
     3. Braking system proportional to the angular speed attained by the vane wheel. 
     4. Electronic system for reading parameters, calculation and display of the result. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a front view of the measurement equipment, showing its simple and robust construction. 
     FIG. 2 is a section of the device taken along line A--A of FIG. 1. 
     FIG. 3 is a schematic view of one of the embodiments of the eddy current brake, which has been used due to its ready construction and adjustment. 
     FIG. 4 is a block diagram of the electronic system, with completely standard components and easily available in the market. 
     FIG. 5 is a software flow diagram to be recorded in the &#34;micro-controller chip&#34;, which controls all operations of the device. 
     In the drawings, the same reference letters correspond to the same constituting elements. 
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     As may be seen in FIG. 1, the equipment is constituted by a housing --a-- containing the vane wheel --b--, such wheel rotating under the power provided by dry particles falling, the dry particles being channelized thereto through bin --c--, the spreader --d-- and a &#34;levelling&#34; hole &#34;e&#34;. Once on the vane, dry particles transfer power to the apparatus and fall freely through the outlet bore &#34;f&#34;. At one end of the single shaft &#34;g&#34;, fixed tc the housing by tight ball bearings --h-- there is a copper disk --i--, rotating solidary to said shaft, and is crossed at the edge by the magnetic field provided by permanent magnet --j-- used for causing the antagonist torque proportional to rotation, due to the interaction between currents induced in the disk and the inductor magnetic field, called &#34;eddy current brake&#34;, shown in a greater detail in FIG. 3, wherein the movement calibrating the radial distance of magnets (indicated by double arrow --k--) may be seen, which allows initial adjustment of the braking constant value. 
     The disk is also used for providing the angular speed signal, taken by an optical or magnetic sensor --l-- acting as generator of angular steps, such signal being sent to the electronic microcomputer which processes the signal for obtaining the flow rate value, final weight value, or both (after temperature compensation, if required), and showing the results on a digital display. FIG. 4 shows the block diagram of this part of the apparatus and FIG. 5 shows the flow diagram corresponding to the software to be followed by the micro-controller (which is recorded at its non-volatile memory), once the apparatus is started up. 
     The function allowing the dry particle weight flow rate is obtained through practical tests, this providing a proper adaptation to mechanical and electronic tolerances, inherent of any actual system.