Abstract:
A piece of the magnetic material to be tested is coupled to the device by primary and secondary windings. The material is then exposed to varying polarities of a controlled electrical current, such as a ramped current, through the primary winding causing the magnetic flux of the material to vary with respect to the controlled current; and creating varying voltage levels across the secondary winding. When this process has been completed the data is made available to a computer which now has data for the current levels transmitted through the primary winding and the corresponding voltage levels across the secondary winding. The computer can then utilize this data to provide a variety of magnetic property values of the magnetic material.

Description:
BACKGROUND OF THE INVENTION 
     This invention relates, in general, to testing apparatus and methods and, more particularly, to an apparatus and method for testing magnetic materials. 
     Traditionally, flux measurements have been conducted with a ballistic galvanometer that deflects a light beam. This is a slow, cumbersome, and inaccurate method. 
     Another method is using Hall Effect sensors along with a permanent magnet. ln this process a sample is moved at a constant speed through the magnetic field while measurements are taken with the Hall Effect device. This method is slow and inaccurate and the results of this method can be influenced by temperature. 
     An improvement of the Hall Effect device uses solid state devices, see DeMott, lntegrating Flux Meter With Digital Read Out, 6 I.E.E.E. Trans. On Mag., 269 (1970). This device is derived by coupling a solid-state voltage-to-frequency converter to a digital converter. This device, however, is unable to make the variety of measurements often desired and has a narrow range of operating conditions. 
     Further, the I.E.E.E. standard has no storage for the text results and has little or no control over the rate of rise of the current pulses used. 
     SUMMARY OF THE INVENTION 
     Accordingly, it is an object of the present invention to provide an apparatus and method of testing magnetic materials that will overcome the deficiencies described above. 
     A further object of the present invention is to provide an apparatus and method of testing magnetic materials that provided an increased frequency response. 
     Another object of the present invention is to provide an apparatus and method of testing magnetic materials that is versatile in its ability to test a variety of magnetic properties. 
     Still another object of the present invention is to provide an apparatus and method of testing magnetic materials that has a high dynamic range. 
     Yet another object of the present invention is to provide an apparatus and method of testing magnetic materials that has increased speed and accuracy. 
     A further object of the present invention is to provide an apparatus and method of testing magnetic material that has accurate control over the rate of rise and fall of the current pulses used. 
     The above and other objects and advantages of the present invention are provided by an apparatus and method of testing magnetic materials that is computer operated. 
     A particular embodiment of the method of the present invention consists of the steps of: providing a current pulse of a first polarity to a primary winding coupled to said magnetic material; changing the magnetization of said magnetic material and driving a flux density of said magnetic material to a saturation level of said first polarity and then down to a residual level of said first polarity; providing a controlled current pulse of a second polarity to said primary winding; changing the magnetization of said magnetic material and driving said flux density from said residual level of said first polarity to a saturation level of said second polarity and then to a residual level of said second polarity; measuring changes in a voltage across a secondary winding coupled to said magnetic material during said current pulse of said second polarity; converting said measured voltages to digital signals; storing said digital signals in a storage device; providing a second controlled current pulse of said second polarity to said primary winding; changing the magnetization of the magnetic material driving said flux density from said residual level of said second polarity to said saturation level of said second polarity and back to said residual level of said second polarity; measuring changes in the voltage across said secondary winding during said second current pulse of said second polarity; converting said measured voltages to digital signals; storing said digital signal in said storage device; and processing the data in said storage device. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a block diagram of a device embodying the present invention; 
     FIG. 2 is a graph of a current, I, being utilized by the device of FIG. 1; and 
     FIG. 3 is a graph of a hysteresis loop generated by the device of FIG. 1. 
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     Referring to the block diagram of FIG. 1 a device 10, embodying the present invention, for testing magnetic materials is illustrated. Device 10 consists of a computer 11, such as the 9616 produced by Creative Microsystems; positive, 12, and negative, 13, current sources; a high impedance amplifier 15, such as the HA2520 produced by Harris, Inc.; an analog-to-digital (A/D) converter 16, such as the TDC1007J produced by TRW, Inc.; and a memory 17, such as the MCM93425DC produced by Motorola, Inc. 
     A piece of magnetic material 14, here a toroid, is coupled to device 10 by a primary test winding 18 and secondary test winding 19. It should be noted here that, for other shapes of magnetic materials, other forms of connection can be devised. 
     In operation, computer 11 activates positive and negative current sources, 12 and 13, along lines 20 and 21, respectively, to provide a current to primary winding 18. The current provided by current sources 12 and 13 is of a controlled known rate of change. This causes changes in the magnetization of toroid 14 which induces a voltage in secondary winding 19. The analog signal from secondary winding 19 is converted to digital signals by A/D converter 16 which are then stored in memory 17 for later use by computer 11. 
     A more detailed description of the operation has computer 11 activate positive current source 12 to provide a positive current to primary winding 18. This is illustrated as pulse P 1 , FIG. 2. Pulse P 1  is provided to drive the magnetic field, H, and magnetic flux, B, of a hysteresis loop, FIG. 3 to a point B max . 
     The hysteresis loop of FIG. 3 is a curve showing two values of magnetic flux density, one when the magnetizing force is increasing and the other when it is decreasing. In this graph H represents the magnetic field measured in oersteds and B represents the magnetic flux measured in gauss. The points B max  and B min  represent the points of positive and negative saturation, respectfully, on the hysteresis loop. 
     Once pulse P 1  has driven the magnetic flux to B max , computer 11 reduces positive current source 12. This allows the magnetic flux of toroid 14 to fall back to point  +  B residual , FIG. 3. Since the natural state of the magnetic flux of torroid 14 can be either  +  B residual  or  -  B residual , pulse P 1  is used to insure that magnetic flux density will be at  +  B residual  thereby providing a known starting point for the measurements to be made. 
     Next, computer 11 causes negative current source 13 to provide a negative ramped increase in current to primary winding 18. This negative ramped current represents a strictly controlled and known change in current with respect to time. The change in current is represented in FIG. 2 by pulse P 2 . This ramped increase of current can be varied by computer 11 to provide differing sets of hysteresis loops. The negative current, FIG. 2, causes the magnetic field density to move from  +  B residual  to B min  providing data illustrative of the line between these two points, FIG. 3. 
     When computer 11 activates negative current source 13 along line 21 it also activates A/D converter 16. A/D converter 16 is not activated when the positive pulse, P 1 , is provided as this information is not required. Broken line 20, from computer 11 to A/D converter 16, is provided to illustrate that the functions of the negative and positive pulses may be interchanged and line 20 may be used in place of line 21. 
     The change in the magnetic flux density of toroid 14 causes a corresponding change in the voltage across secondary winding 19. One end of secondary winding 19 is coupled to ground and the other end is coupled to amplifier 15. Amplifier 15 is provided in the circuit to prevent the circuit from drawing current from secondary winding 19 and to condition the amplitude of the voltage to a level A/D converter 16 can utilize. 
     A/D converter 16, having been activated by computer 11 along line 21, converts the analog voltage signals received from amplifier 15 to digital signal. The digital signals are then stored in memory 17. 
     When the voltage across secondary winding 17 stabilizes it indicates that the point of negative saturation, B min , has been reached on the hysteresis loop, FIG. 3. Pulse P 2  is then reduced in a controlled ramped manner back to zero, FIG. 2. As the current proceeds to zero, the magnetic flux density proceeds from B min  to  -  B residual . The voltage readings along this path are also measured and stored in memory 17. 
     Once pulse P 2  has been completed a set of data can be provided that shows a portion of the hysteresis loop from  +  B residual  to B min  to  -  B residual . This data can be used to show the relative values of these points to each other, but not where these points reside on the H-B graph, FIG. 3. 
     Next, computer 11 causes a second controlled ramped negative pulse, P 3 , to be transmitted to primary winding 18. This drives the magnetic flux density from  -  B residual  to B min , FIG. 3. Once B min  has been reached a second time the current is again reduced to zero in a controlled ramped manner and the magnetic flux density returns to  -  B residual . 
     The controlled currents provided to the primary winding from the current sources are provided here at a controlled ramped rate. This provides the system with a known fixed rate of increase over time, which is required to determine the magnetizing properties accurately. While the current here is shown to be ramped other types of current wave forms may be used as long as they are of a known, controlled nature, such as an exponential wave form. 
     The data from pulses P 2  and P 3  is then transmitted to computer 11 to be analyzed. The data from pulse P 3  is utilized to assign H-B coordinate values to the data obtained from pulse P 2 . 
     The data, which computer 11 now contains, consists of the current, I, and voltage, V, that correspond to the magnetic flux densities of the hysteresis loop. Knowing V and I, the magnetic flux, B, values can be determined by the equation, 
     
         B=(1/N)∫Vdt                                           (1) 
    
     where: 
     N is the number of turns of the secondary winding; 
     V is the voltage measurement taken; and 
     t is the time. 
     The H, magnetic field, values of toroid 14 can be determined by the equation: 
     
         H=N(I/L)                                                   (2) 
    
     where: 
     I is the current; and 
     L is the mean path length of toroid 14. 
     From these values one-half of the hysteresis loop, FIG. 3, can be determined. Since a hysteresis loop is usually symetrical about its center point the positive half of the loop can also be generated. 
     In addition to the hysteresis loop a number of other magnetic properties of the material can be determined. A sample of these and their equations are listed below: 
     (A) incremental permeability, 
     
         μ.sub.in =(ΔB/ΔH)                           (3) 
    
     (B) permeability, 
     
         μ=(B/H)                                                 (4) 
    
     (C) reluctance, 
     
         R=∫(dL/μA)                                         (5) 
    
     where: 
     A is the cross sectional area of toroid 14. 
     (D) Energy, 
     
         w=AL∫HdB                                              (6) 
    
     (E) Hystersis Losses, 
     
         R.sub.h =HdB                                               (7) 
    
     (F) Coercive Forces  -  H c  and  +  H c , the value of H when B is zero; and 
     (G) The residual magnetic fluxes,  -  B residual  and  +  B residual , the value of B when H is zero. 
     It should be noted here that the above list is submitted as a sample of the information to be determined from the hysteresis loop and that other magnetic properties may be determined from this information. Computer 11 can be set to derive information and provide any or all of the information listed above. 
     Thus, it is apparent that there has been provided, in accordance with the invention, a device and method that satisfies the objects, aims and advantages set forth above. 
     It has been shown that the present invention provides an apparatus and method of testing magnetic materials that provides an increased frequency response; is more versatile in its ability to test a variety of magnetic properties; and has a higher dynamic range. 
     While the invention has been described in conjunction with specific embodiments thereof, it is evident that many alterations, 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 alterations, modifications, and variations in the appended claims.