Patent Application
20080084307
1. Field of the Invention
The present invention relates to an electronic article surveillance system and a marker for use therein; and more particularly, to a process for fabricating a magnetomechanically resonant marker with improved control of the resonant frequency of the marker that enhances the sensitivity and reliability of the article surveillance system.
2. Description of the Prior Art
Attempts to protect articles of merchandise and the like against theft from retail stores have resulted in numerous technical arrangements, often termed electronic article surveillance (EAS). Many of the forms of protection employ a tag or marker secured to articles for which protection is sought. The marker responds to an electromagnetic interrogation signal from transmitting apparatus situated proximate either an exit door of the premises to be protected, or an aisleway adjacent to the cashier or checkout station. A nearby receiving apparatus receives a signal produced by the marker in response to the interrogation signal. The presence of the response signal indicates that the marker has not been removed or deactivated by the cashier, and that the article bearing it may not have been paid for or properly checked out.
One common type of EAS system typically known as a harmonic (or electromagnetic) system relies on a marker comprising a first elongated element of high magnetic permeability ferromagnetic material, which is optionally disposed adjacent to at least a second element of ferromagnetic material having higher coercivity than the first element. When subjected to a low-amplitude electromagnetic field having an interrogation frequency, the marker causes harmonics of the interrogation frequency to be developed in a receiving coil. The detection of such harmonics indicates the presence of the marker. A marker having the second element may be deactivated by changing the state of magnetization of the second element, typically by exposing it to a dc magnetic field strong enough to appreciably saturate the second element. Depending upon the design of the marker and detection system, either the amplitude of the harmonics chosen for detection is significantly reduced, or the amplitude of the even numbered harmonics is significantly changed. Either of these changes can be readily detected in the receiving coil. In practice, harmonic EAS systems encounter a number of problems. A principal difficulty stems from the superposition of the harmonic signal and the far more intense signal at the fundamental interrogation frequency. The detection electronics must be responsive to the relatively weak harmonic signal and discriminate it from the carrier signal and other ambient electronic noise. Harmonic systems are also known to be vulnerable to false alarms arising from massive ferrous objects (such as shopping carts) also present in a typical retail environment.
Another type of EAS marker and system (known as magnetomechanical or magnetoacoustic) is disclosed by U.S. Pat. Nos. 4,510,489 and 4,510,490 (“the '489 and '490 patents”), both to Anderson et al., which are both incorporated herein in the entirety by reference thereto. The marker comprises an elongated, ductile strip of magnetostrictive ferromagnetic material adapted to be magnetically biased and thereby armed to resonate mechanically at a frequency within the frequency band of an incident magnetic field. A hard ferromagnetic element, disposed adjacent to the strip of magnetostrictive material, is adapted, upon being magnetized, to arm the strip to resonate at that frequency. The resonance condition is established by the equation:
fr=(½L)(E/δ)1/2 (1)
wherein fr is the resonant frequency for an elongated ribbon sample having length L, and E and δ are the Young's modulus and mass density of the ribbon, respectively.
The resonance causes the marker to respond to an ac electromagnetic field by changes in its mechanical and magnetic properties, notably including changes in its effective magnetic permeability. In the presence of a biasing dc magnetic field the effective magnetic permeability of the marker for excitation by an applied ac electromagnetic field is strongly dependent on frequency. That is to say, the effective permeability of the marker is substantially different for excitation by an ac field having a frequency approximately equal to either the resonant or anti-resonant frequency than for excitation at other frequencies. Exposing the resonant element to an external ac field urges it to vibration, with a coupling that may be characterized by the marker's magnetomechanical coupling factor, k, greater than 0, given by the formula:
k=[1−(fr/fa)2]1/2, (2)
wherein fr and fa are the resonant and anti-resonant frequencies of the magnetostrictive element, respectively. A detecting means detects the change in coupling between the interrogating and receiving coils at the resonant and/or anti-resonant frequency, and distinguishes it from changes in coupling at other than those frequencies. The coupling is especially strong for excitation at the natural resonant frequency. It is further known, e.g. from U.S. Pat. No. 5,495,230 to Lian, that the resonant frequency depends strongly on the magnitude of the biasing field imposed on the resonant element as a consequence of the bias-field dependence of Young's modulus E in the foregoing resonance equation.
A marker of the type disclosed by the '489 patent is depicted generally at 11 by
The '489 patent also discloses a pulsed EAS system in which a transmitter drives a transmitting antenna, such as a coil, that produces a pulsed electromagnetic field having an interrogation frequency. If present within the antenna field, an active marker having a resonance frequency equal to the interrogation frequency is driven into magnetomechanical resonance. During the interval between transmitted pulses, the excited marker continues to vibrate mechanically at its resonant frequency, thereby producing a magnetic field oscillating at the resonant frequency. The amplitude of the mechanical vibration and the resulting magnetic field decrease exponentially with time. This damped resonance thereby provides the marker with one form of characteristic signal identity.
A similar EAS marker disclosed by the '490 patent comprises multiple strips disposed in a side-by-side fashion. The strips have different resonant frequencies, permitting the marker to be coded by selecting particular frequencies. The coding is detected by ascertaining the multiple frequencies at which the '490 tag exhibits resonance.
However, known magnetomechanically resonant markers comprising magnetostrictive material and systems employing such markers, including those of the types disclosed by the '489 and '490 patents, have a number of characteristics that render them undesirable for certain applications. The markers are relatively large in size, in both their length and width directions. As a result, they are too large to be accommodated on some items of merchandise, including many for which protection is highly desirable because of their high value. A large marker is also relatively conspicuous when affixed externally to a merchandise item. Attempts to reduce the size of the marker encounter certain obstacles. In general, reducing the volume of the resonating magnetic element proportionally reduces the detectable signal from the marker and the size of the interrogation zone within which the marker is responsive, hindering reliable detection. For example, in a retail environment, it is a practical necessity that reliable detection be possible over the full aisle width at the store's exit.
Another form of magnetoacoustic EAS marker is provided by U.S. Pat. No. 6,359,563 to Herzer. The '563 marker employs multiple strips of magnetostrictive amorphous ribbon that are cut to the same length and given the same annealing treatment. A marker having such strips disposed in registration is disclosed to produce a resonant signal amplitude that is comparable to that produced by a conventional magnetoelastic marker employing a single piece of material having about twice the width. On the other hand, a single strip of thicker ribbon, even after annealing, is disclosed not to provide a commensurate increase in resonant signal amplitude.
The '563 patent further discloses that prior art ribbon optimized for a multiple resonator tag is unsuitable for a single resonator marker and vice versa. Importantly, the multiple strip markers disclosed in the '563 reference all employ annealed ribbon, and not as-cast, unannealed material. A feedback controlled annealing system is said to provide extremely consistent and reproducible properties in treated ribbon, which otherwise is said to be subject to relatively strong fluctuations in the required magnetic properties.
While certain improvements have been achieved in the aforementioned EAS marker, none of the approaches to date has proven entirely satisfactory.
In one aspect, the present invention provides a magnetomechanical marker and an electronic article surveillance system using such a marker. The marker exhibits magnetomechanical resonance at a marker resonant frequency in response to the incidence thereon of an electromagnetic interrogating field. The marker comprises: (i) a magnetomechanical element comprising at least one, and preferably two or more, elongated resonator strips composed of unannealed magnetostrictive amorphous metal alloy; (ii) a housing having a cavity sized and shaped to accommodate the magnetomechanical element, the one or more resonator strips being disposed in the cavity and able to mechanically vibrate freely therewithin; and (iii) a bias element, such as a strip of semi-hard magnetic metal alloy, that is adapted to be magnetized to magnetically bias the magnetomechanical element, whereby the magnetomechanical element is armed to resonate at the marker resonant frequency in the presence of an electromagnetic interrogating field. If multiple resonator strips are present in the magnetomechanical element, the strips are disposed in the cavity in stacked registration. In some embodiments, they are of substantially the same length so that they resonate at substantially the same frequency. Other embodiments employ plural strips having a plurality of preselected resonant frequencies to provide a coded marker, such as a marker of the type disclosed by the '490 patent.
Further provided are a process and apparatus for continuously fabricating a sequence of such markers for a magnetomechanical electronic article surveillance system. The process preferably employs a measurement of marker resonant frequency of the markers during the fabrication and adaptive control of the cut length of resonator strips that are incorporated in markers subsequently produced in the sequence.
In one implementation of the process, each marker comprises: (i) a magnetomechanical element comprising at least one elongated resonator strip having a resonator strip cut length; (ii) a bias element adapted to magnetically bias the magnetomechanical element, whereby the magnetomechanical element is armed to resonate at a marker resonant frequency; and (iii) a housing having a cavity sized and shaped to accommodate the magnetomechanical element and permit it to mechanically vibrate freely therewithin. The process comprises: (a) forming a plurality of cavities along a web of cavity stock, each of the cavities having a substantially rectangular, prismatic shape open on a large side and a lip extending substantially around the periphery of the opening of the cavity; (b) cutting elongated resonator strips sequentially from a supply of magnetostrictive amorphous metal alloy using a resonator strip cutting system, the resonator strips having a resonator strip cut length; (c) extracting at least one of the resonator strips from the cutter system using an extractor; (d) disposing at least one of the resonator strips in each of the cavities to provide a magnetomechanical element of the marker; (e) affixing a lid to the lip to close the cavity and contain the magnetomechanical element therewithin; (f) supplying bias elements from a supply of semi-hard magnetic material, the bias strips having a bias shape and bias dimensions; (g) fixedly disposing a bias element on the lid in registration with the magnetomechanical element; (h) optionally activating at least a portion of the markers by magnetizing the bias elements, whereby the markers are armed to resonate at the marker resonant frequency; (i) measuring the resonant frequency of each of the markers in a preselected sample portion of the sequence; and (j) adaptively controlling the resonator strip cut length for resonator strips incorporated in subsequently produced markers of the sequence, the resonator strip cut length being adjusted to an updated resonator strip cut length determined from a difference between the measured marker resonant frequencies and a preselected target resonant frequency, whereby the difference for the subsequently produced markers is reduced. Steps (i) and (j) are repeated during the course of the fabrication. Optionally, the web is cut to separate the markers and the markers are adhered to a release liner.
As a result of the foregoing adaptive control, based on measurement of the resonant frequencies of finished markers during the production, the sequence exhibits a tight distribution of frequencies, improving the production yield of markers and the reliability of EAS system operation. Moreover, the control permits industrially viable construction of markers wherein the magnetostrictive element comprises plural strips of unannealed, magnetostrictive amorphous metal alloy. Such markers are smaller and are more easily and reliably produced than previous markers, which have required either a larger footprint or use of annealed magnetic materials.
There is further provided a press for fabricating a sequence of magnetomechanical EAS markers, such as markers of the foregoing construction. The press comprises: (a) a web infeed system for delivering a continuous web of cavity stock; (b) a cavity formation die set for forming a plurality of cavities along the web, each of the cavities having a substantially rectangular, prismatic shape open on a large side and side walls surrounding the cavity and defining a periphery; (c) a resonator strip cutter system comprising a first resonator strip cutter, and optionally, one or more additional resonator strip cutters, for cutting elongated resonator strips sequentially from a supply of magnetostrictive amorphous metal alloy to an adjustable, preselected resonator strip cut length; (d) an extractor for extracting at least one of the resonator strips from the resonator cutter system and disposing the at least one resonator strip, and preferably two or more resonator strips in stacked registration, in each of the cavities to provide a magnetomechanical element; (e) an affixing system for affixing a lid to the periphery to close the cavity and contain the magnetomechanical element therewithin; and (f) a bias strip cutter for cutting bias strips from a supply of semi-hard magnetic material, and fixedly disposing at least one of the bias strips on the lid in registration with the magnetomechanical element.
Optionally, the press includes a heating means to preheat the cavity webstock prior to cavity formation.
The press may further comprise an activation magnet system comprising at least one activation magnet for activating at least some, and preferably all of the markers by magnetizing the bias strips, whereby the markers are armed to resonate at the marker resonant frequency.
In some implementations, the press also comprises an in-line frequency measurement and control system for adaptively adjusting the resonator strip cut length during fabrication of the sequence to match the marker resonant frequency to a preselected target resonant frequency. The system preferably comprises: (a) a measurement system comprising a transmitter for imposing a burst of electromagnetic field having substantially the target resonant frequency onto a preselected sample portion of markers of the sequence, the burst exciting the markers of the sample portion into magnetomechanical resonance, and a receiver for detecting the marker resonant frequency during a ringdown after the burst; and (b) a computing system connected to the receiver and the resonator cutter system, the computing system recording the marker resonant frequency for the markers of the sample portion, computing an updated resonator strip cut length based on a difference between the recorded marker resonant frequencies and the target resonant frequency, and causing adjustment of the resonator strip cut length to the updated resonator strip cut length for subsequently cut resonator strips to reduce the difference for subsequent markers of the sequence. Preferably, the activation system activates substantially all the markers produced by the press. Preferably, the sample portion comprises substantially all the markers within an interval of the sequence.
In still another aspect, there is provided an assemblage of a plurality of such magnetomechanical markers. The assemblage preferably is formed of markers produced in sequence using a supply of magnetostrictive amorphous metal alloy. In preferred embodiments the assemblage comprises a sequence of at least 2000 markers, which exhibit a narrow distribution of frequencies, preferably a distribution having a relative standard deviation of frequencies of markers no more than about 0.5% and, more preferably, no more than about 0.3%.
The invention will be more fully understood and further advantages will become apparent when reference is had to the following detailed description of the preferred embodiments of the invention and the accompanying drawing, wherein like reference numerals denote similar elements throughout the several views, and in which:
In an aspect, the present invention provides a marker comprising a resonator element, a biasing magnet element, and associated structure to contain these elements. Referring now to
The magnetomechanical element preferably consists essentially of two rectangular strips of an FeNiMoB-containing amorphous metal alloy. A suitable material is sold commercially as ribbon by Metglas, Inc., Conway, S.C., under the trade name METGLAS® 2826MB3 and understood to have a nominal composition (atom percent) Fe40Ni38Mo4B18. The 2826MB3 alloy is a magnetostrictive, soft ferromagnetic material, having a saturation magnetostriction constant (λs) of about 12×10−6, a saturation magnetization (Bs) of about 0.8 T, and a coercivity (Hc) of about 8 A/m (0.1 Oe). These resonator strips may used in the as-received condition from the manufacturer without being subjected to any heat-treatment. The resonating strips in a preferred implementation are about 6 mm wide and 38 mm long, resulting in acousto-magnetic resonance for an electromagnetic exciting frequency of about 56-60 kHz. Unannealed METGLAS® 2826MB alloy is another suitable resonator material. In other embodiments, other suitable magnetostrictive, soft ferromagnetic materials may also be used as resonator elements, in either the heat-treated or as-received condition.
As used herein, the term “ribbon” denotes a generally thin, substantially planar material extending to an indeterminate length along a length direction, and having a width direction perpendicular to the length. The length and width define two opposed ribbon surfaces. The thickness is substantially less than the width or length dimensions. Amorphous metal is generally supplied commercially in the form of such ribbon wound onto spools that may contain many kilograms of material having a length of thousands of feet or more. As used herein, an “elongated strip” refers to a finite geometric form having a length greater than either a thickness or a width. The elongated strip of resonator material used in the EAS marker of the invention may have the form of a wire having approximately equal width and thickness, but preferably is a finite, generally rectangular portion of a ribbon having length greater than thickness. Preferably, the length of a strip used in the magnetomechanical element of the present marker is at least 100 times its thickness and at least five times its width. By “registration” is meant a relative orientation and positioning of multiple elements in a predetermined arrangement. “Stacked registration” refers to a disposition of two or more strips having substantially similar dimensions, the strips being arranged one over the other in substantial overlap, if not exact congruency, and with their ribbon surfaces generally parallel. In any event, the term is intended to preclude a side-by-side or other non-collinear arrangement. Those skilled in the art will recognize that an elongated strip as defined herein possesses a low demagnetizing factor for magnetization along the elongated direction.
The present marker is further provided with a bias means that provides a magnetic field to bias the magnetomechanical element and thereby activate it by arming the element to resonate at a marker resonant frequency. The bias means may comprise a bias element, such as one or more magnetized elements composed of permanent (hard) magnetic material or semi-hard magnetic material. By a “hard magnetic material” is meant a material having a coercivity in excess of about 500 Oe. By a “semi-hard magnetic material” is meant a material having a coercivity sufficient to prevent inadvertent alteration of its magnetic state by exposure to fields ordinarily encountered during handling, transportation, and use of the present marker, but small enough to permit the material to be demagnetized by demagnetization apparatus conventionally used in connection with EAS markers, e.g. by exposure to an exponentially damped sinusoidal magnetic field that has initial strength at least sufficient to approximately saturate the biasing element. Typically, a semi-hard material has a coercivity in the range of about 10-500 Oe. A wide variety of magnetic materials are thus suitable. In some applications, the ordinary use of the marker does not entail any deactivation. In this situation, the bias element may employ a hard magnetic material, since there is no requirement that the bias element be demagnetizable in the field. High anisotropy, high coercivity materials, such as ferrites and rare-earth magnets, may be provided as magnets having a short aspect ratio, i.e., a low ratio of the dimensions along the magnetization direction and in a perpendicular direction. Semi-hard magnetic materials useful as demagnetizable bias elements, such as alloys sold under the tradenames Arnokrome, Vicalloy, MagneDur, and other semi-hard steels, are advantageously employed as thin strips. Preferably, one of these semi-hard bias materials is used in the form of a single strip aligned generally parallel to the elongated magnetomechanical element. The bias strip may have a generally rectangular shape or may have any other polygonal but elongated shape, such as the truncated parallelogram shape of element 4 shown in the embodiment of
A preferred semi-hard bias material is sold by Arnold Magnetics, Marengo, Ill. under the trade name ARNOKROME™ 4. Such magnet material is in thin strip form and has a nominal composition of 1-12% Cr and balance Fe. When measured in a hysteresis loop tracer with peak excitation field level of 250 Oe, and operating drive field frequency of 60 Hz, a sample 6.0 mm wide, 76.2 mm long, and 25.4 μm thick exhibits the following semi-hard magnetic properties: (i) a remanence Br: 1.4±0.1 tesla; (ii) a coercivity Hc23±3 oersteds; and (iii) a remanent flux Fr: 390±30 nano-webers, wherein Fr=Br*A and A is the cross sectional area of the ribbon sample.
The preferred bias magnet material additionally has the following properties when magnetized in a uniform solenoidal DC field of applied to a sample 6.0 mm wide×28.6 mm long: (i) the sample is magnetized to within 2% of its saturated remanent flux in a field of 100 Oe; (ii) the sample retains >12% of its saturated remanent flux after exposure to a demagnetizing DC field of strength 80e; (iii) after exposure to a 25 Oe demagnetizing AC field, the saturated sample retains no more than 30% of its saturated remanent flux, the demagnetizing field having an exponentially decreasing waveform; and (iv) a saturated sample, when bent around a radius of 13.5 mm does not exhibit a loss of magnetism of greater than 12% of the saturated remanent flux.
Another preferred bias material exhibiting similar physical and magnetic properties, including a coercivity of about 20 to 30 Oe and a flux of 400 to 500 nWb, is sold by Arnold Magnetics under the trade name ARNOKROME™ 5.
In a representative embodiment, the foregoing marker is used in conjunction with a pulsed, magnetomechanical EAS system that includes an apparatus that comprises a transmitter, a receiver, and one or more antennas in the form of loops of wire. Some or all of these system components are ordinarily disposed within one or more pedestals situated at a screening location, such as a retail store exit. The transmitter and receiver may share an antenna or use separate antennas. In operation, the transmitter generates a signal that is fed to a transmitting antenna to create an electromagnetic field having an interrogation frequency (often approximately 58 kHz) within an interrogation zone. During a transmit interval, the transmitter is gated on to produce an electromagnetic field that induces a magnetomechanical resonance at substantially the same frequency in the marker. The magnetomechanical element of the marker is urged to resonance during each pulse. After each pulse is completed, the energy stored in the magnetomechanically resonating element decays and as a result, the marker dipole field emanating from the marker decays or rings down correspondingly. The amplitude of the alternating field generally remains within an envelope that decays exponentially, affording the marker a signal-identifying characteristic that is detectable by the receiver. At a time subsequent to the transmit interval, the receiver is connected to a receiving antenna and gated on to receive a signal during a receive interval. The detection of this ring-down in synchrony with the activation of the marker by the interrogating field provides a preferred way of reliably discriminating the marker's response from other ambient electronic noise or the response of other nearby ferrous objects which are not resonantly excited. An indication means is operably associated with the receiver and is activated in response to the detection of the signal-identifying characteristic by the receiver. Articles to which the marker is attached thereby may be protected against shoplifting in a retail establishment. Typically, after the legitimate purchase of an item, the marker is either removed from it or deactivated by the aforementioned demagnetization process, permitting the bearer and the item to pass through an interrogation zone at the store's exit.
It will be readily appreciated that the electronic article surveillance system and marker of the invention can be employed for related, yet diversified uses that can be accomplished by reliable and unambiguous detection of a marker associated with a person or object. For example, the marker can function as: (i) an identification badge for a person, e.g. for regulating access to a controlled area; (ii) a vehicle toll or access plate for actuation of automatic sentries associated with bridge crossings, parking facilities, industrial sites or recreational sites; (iii) an identifier for checkpoint control of classified documents, warehouse packages, library books, domestic animals, or the like; or (iv) a identifier for authentication of a product. Accordingly, the invention is intended to encompass those modifications of the preferred embodiment that allow recognition of any person or object appointed, by attachment or other suitable association of the marker, for detection by an electronic article (EAS) system. It is further intended that invention encompass the identification by an electronic article surveillance system of a person or animal bearing a marker provided in accordance with the invention.
In typical commercial practice, it is preferred that the markers 10 of the type depicted by
A resonator strip cutter system is used to cut elongated resonator strips from a supply of magnetostrictive amorphous metal alloy. In the implementation shown in
Lidstock supply spool 140 provides lidstock material 142 which is sealed to lips around each cavity to contain the magnetomechanical element in the cavity. Preferably, the sealing is accomplished by passing the web and applied lidstock through heated rollers 144. Flowing air 148 is then delivered from second blower 146 to cool the web after the sealing. One suitable lidstock material is polyethylene-polyester laminate. The lid material is preferably planar, but may also include other non-planar features providing the markers with improved end-use capabilities.
Bias cutter head 150 provides bias elements, such as magnet strips 158 which are cut by bias shears 156 from bias alloy ribbon 154 supplied from bias supply spool 152. Elements 158, which have a preselected bias element shape, are adhered onto one side of double sided tape 162 supplied from spool 160 and fed across idler roll 163. The side of tape 162 bearing elements 158 is then impressed onto the outside face of lidstock 142, e.g. by tape rollers 164, thereby securing element 158 in registration with the magnetomechanical element. The opposite side of tape 162 is preferably covered with a release liner, such as a liner composed of paper, a thin polyester, or other known release liner material. It is preferred that bias cutter head 150 include provision for adjusting bias shears 156 during machine setup or maintenance, or during production, to cut bias strips that have a preselected length and shape. Optionally, the adjustment of shears 156 is made adaptively under computer control to permit compensation for variation in the mechanical or magnetic properties of the bias material.
In the
In still other implementations, the markers are not cut during initial production. For example, the continuous web might be cut only at the point of being associated with merchandise by a supplier as part of a source tagging method. Such applications also may not require the marker to include an adhesive backing and release liner, if the marker is merely intended to be incorporated within merchandise packaging.
It will be understood that the various rollers, spools, and shears in apparatus 100 may be driven by any suitable prime movers, including electric motors of any suitable type, electromechanical actuators, hydraulic or pneumatic drives, or other like means. The relative speeds of the various drives may be established and regulated by electronic control, gearing, clutches, or the like. A suitably programmed PLC or general purpose computer is preferably used to control the entire press system. The inline measurement and control system may employ this computing means or a separate system. Tension control and suitably provided idler loops in the web feed path preferably are employed in a manner known to a person skilled in the art. The rollers may be smooth cylinders, but preferably are provided with suitable patterning or grooves such that pressure is applied principally to portions of the web outside the formed cavities, so that the internal shape of the cavity is not compromised or deformed in a manner that would impair free vibration of the magnetomechanical element during marker interrogation. It will also be understood that apparatus 100 may be appointed to simultaneously produce multiple columns of markers from the same feedstocks and attach them to a common release liner. For example,
It will also be understood that the present invention may be practiced using different materials and production methods. For example, different materials may be used in a production process of the foregoing type and the various mechanical steps may be carried out in a difference sequence and with other suitable mechanical techniques. For example, vacuum formation might be effected in the cavity formation die system.
If it is desired to produce markers in other convenient forms of supply, the production method depicted by
The components of the housing of the present marker are constructed of one or more suitable materials, such as rigid or semi-rigid plastic materials. The magnetomechanical element cavity may be formed by any suitable casting, molding, or machining technique that yields a chamber within which the magnetomechanical element is permitted to vibrate freely. Preferably, the forming method is suited to high-speed, continuous production in an in-line press. Embossing, vacuum and injection forming, molding and cylinder compression are especially suited. In other implementations, suitably shaped cavities to house the magnetomechanical element my be formed by folding a flat material. While the bias element in the embodiment of
The present techniques are beneficially used in conjunction with source tagging, by which is meant a business practice in which a manufacturer of goods associates a marker with the goods, e.g. by placing the marker within or on the packaging during original manufacture or at least prior to shipment of the articles to the final retail vendor. In certain aspects of the invention parts or all of the housing may be integrally formed in packaging, e.g. that used for an article of commerce. In some embodiments, the packaging of the merchandise is provided with internal or eternal structures to accommodate the marker. The location of such structures may intentionally be made inconspicuous or not. Alternatively, the marker may be disposed within a carton or other container for an item of merchandise or similar article of commerce. Some such implementations do not require external adhesive.
The continuous marker process of
In particular, the inventors have found, surprisingly and unexpectedly, that markers employing plural, unannealed amorphous metal resonator strips can be fabricated while maintaining the resonant frequency within tight limits and providing high characteristic signal output. By way of contrast, it previously was believed that unannealed ribbon could not be used in this manner to obtain a high production yield. Of course, the present adaptive feedback control is also beneficially employed in manufacturing markers employing a single unannealed resonator strip or single or multiple annealed resonator strips.
In order to limit false alarms triggered by extraneous ambient electronic noise, magnetomechanical EAS receivers typically use a narrow bandpass delimited by suitable digital or analog input filtering. Accordingly, these receivers are responsive only to markers having a resonance within a relatively narrow range of frequencies. For example, known magnetomechanical EAS systems may operate at a target frequency of about 58 kHz with a bandwidth of ±300 Hz. Ideal methods of producing markers must therefore be highly robust, maintaining a high yield of markers providing, in combination, a resonance falling within a narrow bandwidth and a high output amplitude. These characteristic improve the selectivity of the EAS detection process and the pick rate, i.e. the probability that an activated marker present in the interrogation zone is successfully detected. Ideally, even tighter control would be desired and would to permit the input bandwidth to be further restricted.
A tighter resonant frequency distribution provides a further benefit in operating an EAS system, because it facilitates reliable deactivation. Ideally, the deactivation process completely demagnetizes the semi-hard biasing element, resulting in a maximized shift of marker resonant frequency. Such a resonant frequency shift is known, for example, from FIG. 2 of the '230 patent. But in practice, the semi-hard element often is incompletely demagnetized, leaving it with some residual magnetization. Thus, the resonant frequency is shifted by a reduced amount.
Implementations of the present production technique providing markers with a tighter distribution of resonant frequencies about a target frequency permit an EAS detection system to recognize a smaller frequency shift as indicative of deactivation. More specifically, prior art production may be capable of ensuring that all markers have a resonant frequency between Fr−ΔFr and Fr+ΔFr. Any marker having a frequency outside this interval may be regarded as deactivated. On the other hand, an improved process will ensure that all active markers have resonant frequency between Fr−Δfr and Fr+Δfr, wherein Δfr<ΔFr.
An EAS system designed for the new markers could then operate with a tighter input filtering and discrimination. A prior art system had to regard any marker with a resonant frequency between Fr−ΔFr and Fr+ΔFr as being a valid, active marker. Moreover, prior art systems required that deactivation shift the resonant frequency to a value outside this range. The new system could have a narrower bandwidth and accept a smaller frequency shift (possibly resulting from incomplete demagnetization of the bias element) as still being indicative of deactivation.
Both these effects improve the present EAS system. The reduction of bandwidth decreases the sensitivity of the receiver to ambient electronic noise, improving the system's discrimination between noise and actual active marker signals. The relaxed tolerance for deactivation reduces the probability that false alarms will be triggered, for example by an incomplete deactivation. Both improvements are strongly sought in the marketplace.
However, known production processes typically are not capable of continuously producing markers with resonant frequencies as closely controlled as would be desirable. Production lots are found to include markers characterized by a wide statistical distribution of natural resonant frequencies, resulting in the need for extensive quality control testing to weed out markers not having a resonant frequency within requisite limits. Such inspection itself is fraught with problems and results in reduced production efficiency and the need to discard large numbers of unusable markers. Recycling these defective markers in an environmentally acceptable way is quite difficult. Of necessity, the marker packaging must generally be strong to resist tampering by would-be thieves in a store. The markers contain several incompatible materials, commingling both two different metallic materials and disparate plastics and other organics. Although it would be particularly desirable to recycle the relatively expensive magnetic metal materials, removal of the adjacent plastic and organic materials is needed to minimize unacceptable contamination. Manufacturing processes that minimize the need to discard off-frequency markers are thus strongly sought.
Previous attempts to tighten the resonant frequency distribution during marker production have taken various approaches, including: (i) annealing the magnetomechanical element material to regularize its critical properties and reduce the inherent variation thereof (see, e.g., the '563 patent); (ii) using feedback control of the annealing process, based solely on measurements of the properties of the magnetostrictive strip (see, e.g., the '563 patent); and (iii) adjusting the magnetization state of the bias magnet of each marker after it is produced to shift the resonance to within tolerable limits (see, e.g., the '230 patent). In addition, attempts have been made to adjust the length of cut resonator strips based on measurement of the resonance under bias provided by an externally imposed magnetic field, e.g. a field provided by electromagnets. None of these approaches has proven fully satisfactory for high-volume production.
Without being bound by any particular theory, it is believed that several sources contribute to the ultimate variability of the marker resonant frequency, including the properties of both magnetic materials (the resonant strip and the bias magnet) and details of marker construction, such as the precise relative placement of the magnetomechanical element and the bias magnet. Equation (1) above indicates that the resonant frequency fr is affected by both the sample length L and the effective Young's modulus E. It has been found that the physical variation in length L of the resonant strip attainable in known cutting processes is too small to account for the observed variation in frequency fr, so that other effects, including material variability and field-dependent changes that are manifest in variations in the effective value of E are apparently operative. These frequency variation problems are found to be exacerbated in markers wherein the magnetomechanical element comprises plural strips of amorphous magnetic material. Both the magnetostrictive and bias magnetic materials used in magnetomechanical EAS markers are typically supplied as spools or reels containing indefinite amounts of material in ribbon form and having the requisite width. Each spool may contain sufficient material to produce hundreds or thousands of actual markers. Variations in the magnetic materials are believed to exist both between spools of the same nominal material and within a given spool. The operative magnetic properties of a given section of material depend on plural factors, including inter alia ribbon thickness, composition, physical and surface condition, and heat treatment details. Variations within a given reel may represent changes that occur either gradually through a reel or on a length scale more commensurate with the length of each individual piece that is cut from a longer reel. All of these variations alter the effective value of E and thus change the marker resonant frequency, even though the lengths of marker elements are cut to tight tolerances. Off-line adjustment before a full production run can somewhat compensate for inter-reel variations, but result in significant waste of material and inefficient production. Correcting for either slow or rapid intra-reel variations presents a far greater challenge.
On the other hand, the present inventors have discovered an adaptive, feedback-driven process that can reduce the variability of markers produced in a production sequence to a level that renders the process economically and industrially viable. Moreover, such a process is sufficiently robust to permit unannealed resonator element material to be used in multi-element markers, for which previous processes have not been capable.
More specifically, a feedback technique based on in-line measurement and control of the resonant frequency of actual markers provides a process that is far more robust than any process which relies solely on off-line measurement of the resonant frequency of strips exposed to a well-defined, externally imposed biasing magnetic field, e.g. a field produced by solenoidal electromagnets. Such an off-line process at best can partially compensate for variations, but only in the properties of the resonant material itself. By way of contrast, the present in-line, adaptive process can compensate for changes in both the resonator material, the bias material, and the finished marker configuration. Specifically, the in-line process can address subtle variations in the bias field that arise either from changes in inherent physical properties, geometric changes in the markers, or differences in the magnetization achieved during activation of the markers. Measurement and control using the actual marker resonance instead of simply the resonance of isolated amorphous metal resonator strips permits compensation for all these effects. The result is a more robust process that is more efficient and cost-effective, both in material usage and production yield.
In preferred implementations, the present press and production method permit fabrication of markers in which the relative standard deviation of resonant frequency is no more than about 0.5%, and more preferably, no more than about 0.3%.
A further benefit of some implementations of the present adaptive control system is the ability to rapidly adjust the system after supply reels of the magnetostrictive and bias materials are changed during extended production. It is found that each new reel of material requires slight adjustment of resonator strip cut length to attain the desired resonant frequency. The present system allows these accommodations to be made quickly and with minimal loss of yield at startup.
In addition, the present process obviates the need for functional testing of markers subsequent to production, since such testing is inherently accomplished during production, eliminating the need for the multiple testing steps previously employed. The present process is even seen to be capable of controlling production of markers employing a magnetomechanical element with multiple, unannealed strips to produce acceptably low variation. On the other hand, the prior art, such as the '563 patent, has taught markers with multiple stacked resonating strips that are producible only with annealed material. Beneficially, unannealed amorphous magnetic material is easier to handle and cut than annealed material, which is often found to be brittle and difficult to cut reliably and cleanly. Cracks and other similar microstructural defects often result from cutting and/or slitting annealed ribbon. Such defects can alter the effective length of the ribbon, drastically shifting its resonant frequency, and can also reduce the mechanical Q of the resonance, thereby degrading the output amplitude, often to the point of rendering a particular marker undetectable. Elimination of the annealing step, previously regarded as needed to reduce the inherent variability of as-cast amorphous magnetic material to acceptable levels, thus simplifies production, increases reliability, and reduces cost. Still further, dual-strip EAS marker embodiments provided by the '563 patent disclose only cobalt-containing amorphous metals, which have higher raw materials cost than the Co-free alloys that are employed in preferred implementations of the present process.
The present feedback-driven length adjustment provides for adjustment of the resonator strip cut length based on measurement of the resonant frequency of a sample portion of one or more markers previously made and activated in a production sequence. That is to say, the length Li of the one or more resonant strips in the i-th marker produced in a sequence is based on the measurement of the natural marker resonant frequencies of a preselected sample portion of a preselected sample of previous markers of the sequence, such as the frequencies frj to frk of the j-th through k-th markers, respectively, wherein j≦k≦i. For example, the preselected markers may comprise an uninterrupted sequence of every marker within a production interval, or a subset thereof. Preferably, j≠k, that is to say, the measurement of more than one previous marker is used in the corrective adjustment. The adjustment may be made based on an average of the marker resonant frequencies of any suitable number of previous markers, such as 10 to 1000 previous markers. Preferably, the adjustment is based on an average of the frequencies of about 50 to 500 previous markers. More preferably, the measurement is based on a weighted or moving average. Most preferably, the measurement is based on an exponentially declining moving average, which puts greater statistical weight on results from more recently produced markers. However, any other appropriate statistical averaging and correction may also be applied. It is preferred that measurement of marker resonant frequency be carried out on at least a sizeable fraction of the markers being produced, if not substantially all the markers. It is further preferred that any lag between measurement and correction be minimized. That is to say, it is preferable that the correction of resonant element cut length be based on the most recently produced markers, which corresponds to having the value of k be as close as possible to the value of i. Of course, markers of the sample portion must be activated prior to measurement of their natural resonant frequencies.
The correction of resonant element cut length is based on the difference between the actually observed resonant frequencies of the markers of the sample portion and a preselected target marker resonant frequency. Typically the fractional adjustment of length for future markers in a sequence is inversely proportional to the fractional deviation in actual frequency from the aim of the immediately preceding markers, the deviation being calculated using the selected form of averaging. The use of averaging techniques improves the closed-loop stability of the present feedback process. It will be understood that after initial start-up and stabilization, the needed adjustments are ordinarily quite small, so that even with the foregoing adjustment, the resonant element cut lengths of all the elements fabricated in a production sequence are substantially the same, by which is meant the lengths are sufficiently close to permit all the markers of a production sequence to resonate at a frequency of about the target, deviating by no more than about the desired input bandwidth of the EAS receiver with which the markers are to be used.
One implementation of the feedback system employs the detection system shown generally at 180 by
Some implementations of the feedback measurement system employ a single coil that is switched between connection to the transmitter and receiver. That is to say, the coil is first connected to the transmitter during the duration of the transmitted electromagnetic field burst and thereafter connected to the receiver to receive the field emitted by the resonant element during the ringdown of its mechanical vibration. A single-coil system optionally includes magnetic shielding elements to reduce interference. Both single and multiple coil systems might include an idler loop for the marker web so that the forward motion of the portion of the web bearing the marker being tested can be arrested in the vicinity of the coil system for the brief interval required for excitation and ringdown of that marker. Alternatively, the testing is carried out rapidly enough that a given marker under test remains within the range of the coil system for long enough to be excited and the ringdown sensed, despite its progress through the press.
In a preferred implementation depicted by
The efficacy of the present control system may be measured using any appropriate statistical metric characterizing the width of a distribution. Most commonly, a conventionally calculated standard deviation of the measured marker resonant frequencies is used, and may be specified as a relative standard deviation, i.e., a ratio of the standard deviation of the measured frequencies to the mean marker resonant frequency of the sample population.
It will be understood that in some implementations, parallel columns of targets are produced on a single advancing web, with each column being supplied with its magnetic elements from different feed spools that are cut by different cutter heads. In such implementations, it is preferred that a suitable detection system 180 be provided for each column, so that the resonant strip cut lengths can be independently selected and adjusted for each column.
The principles of the present adaptive technique can also be employed to produce coded markers, in which each marker comprises a plurality of strips resonant at different preselected frequencies. Such a system might be implemented either with multiple transmit and receive coils, in which each set is devoted to measurements for a particular one of the different resonant frequencies. Alternatively, a single set might be used for a sequence of multiple excitations. In either case, the one or more cutter heads used can be controlled to produce strips having different resonant frequencies, the various lengths being adaptively controlled such that each of the multiple frequencies is within tight limits.
The following examples are provided to more completely describe the properties of the component described herein. The specific techniques, conditions, materials, proportions and reported data set forth to illustrate the principles and practice of the invention are exemplary only and should not be construed as limiting the scope of the invention.
A series of magnetomechanical EAS labels having a natural resonant frequency for magnetomechanical oscillation are produced using a continuous-feed, web-based press. Each label comprises a housing having a cavity, two resonator strips disposed in the cavity to form a magnetomechanical element, and a bias magnet adjacent the resonator strips. The production is accomplished using a press adapted to carry out, in sequence, the following steps: (i) embossing cavities in a high-impact polystyrene-polyethylene laminate webstock material; (ii) cutting magnetostrictive amorphous metal ribbon stock using a resonator strip cutter system to form resonator strips having a preselected resonator strip length; (iii) extracting two of the resonator strips from the cutter system; (iv) disposing the extracted strips in each cavity in stacked registration; (v) covering and sealing each cavity with a lidstock material that confines the resonator strips in the cavity without constraining their ability to vibrate mechanically; (vi) cutting semi-hard magnetic material to form bias magnet strips having a preselected bias strip length; (vii) placing and securing a bias magnet strip on the lidstock proximate the resonator strips; and (viii) activating the EAS label by magnetizing the bias magnet strip substantially to saturation. The press is capable of operating in two different modes: (i) a fixed-length mode, in which the preselected resonator strip length is set to a fixed value; or (ii) an adaptive, feedback driven mode in which the resonator strip cut length is adaptively adjusted to maintain a preselected target resonant frequency, which is chosen to be about 58 kHz.
The feedback system employs an in-line measurement and control system that includes a transmitter coil that provides a gated burst of electromagnetic field applied to the labels in the production stream. After each burst, the natural magneto-mechanical resonance of a particular marker is detected generally as a sinusoidal voltage induced in a receiving coil, the voltage having an exponentially decaying amplitude. The free oscillation frequency corresponds to the natural magneto-mechanical resonance frequency of that label. The system employs an electronic measurement system, preferably one based on a general-purpose computer programmed to continuously accumulate, in a first-in, first out buffer, the resonant frequencies of the labels in the production. A buffer size of 300 measurements (about 1 minute's worth of production) is chosen as a sample portion, and the average resonant frequency and standard deviation are calculated using the computer. In feedback mode, if the average frequency deviates by more than a preselected amount from the target frequency, the computer directs the cutting head to cut subsequent resonator strips to an updated cut length to compensate for the deviation and bring the frequency back into range. In particular, the system is programmed to increase/decrease the nominal cut length by 0.002 inches if the frequency is more than 50 Hz higher/lower than a nominal target, e.g. 58,050 Hz.
A production run is carried out to yield the results set forth in Table I hereinbelow, in which is set forth the nominal resonator cut length, the average and standard deviation of the resonant frequency of a 300-label buffer at the indicated time during the run. These data are collected on labels made using resonator strips cut from a single supply lot of METGLAS® 2826MB magnetostrictive amorphous metal and bias strips cut from a single supply lot of ARNOKROME™ 4 semi-hard magnet material.
It is seen that after the adaptive feedback system is activated at about 12 minutes into the production run, the system senses the deviation from the target 58,050 Hz resonant frequency and begins making adjustments to the cut length that rapidly brings the observed average resonance into a close match to the desired target frequency, with a relatively small standard deviation within each buffer size.
The efficacy of the adaptive feedback label production system used for the experiments of Example 1 is tested during extended duration production. The system is operated in a normal factory production schedule to produce labels using the same nominal resonator and bias materials employed in Example 1. However, multiple supply lots are used over several days' worth of production. The press is operated for several days each without and with use of the adaptive resonator strip length control. Results are set forth in Table II below.
Although Runs A1 and B1 both achieve an average resonant frequency close to the desired 58050 Hz value, the standard deviation over the production run of over 1,000,000 markers is substantially larger than the standard deviations attained in runs A2 and B2 made with the adaptive feedback system engaged.
An implementation of the present marker fabrication press and process employing an extractor using a permanent magnet disposed below the traversing webstock is used for high-rate production of markers. The markers are formed using METGLAS® 2826MB3 resonator strips and ARNOKROME™ 5 semi-hard magnet alloy strips as bias elements. An in-line frequency measurement and control system is used to adaptively adjust the resonator strip cut length during fabrication of a sequence of markers. The measurement system includes a single coil used for both transmit and receive functions, the coil being electrically switched under computer control between transmitter circuitry during pulse excitation of the marker under test and receiver circuitry to sense the subsequent resonant ringdown of the marker. Alternate markers in the production sequence are thus tested.
The efficacy of the adaptive feedback label production system in maintaining a tight distribution of resonant frequencies in the production sequence is indicated by the data of Table III set forth below. From each lot a group of ten markers is randomly selected as being representative. The resonant frequency and ringdown behavior of each marker are tested using an off-line tester. The average values of frequency, amplitude immediately after the cessation of the exciting pulse (V0) and after a 1 ms ringdown interval (V1) are tested. A standard deviation of the frequency values is calculated. All of the markers exhibit satisfactory behavior, permitting them to be used in a magnetomechanical EAS system operating at a nominal 58 kHz exciting frequency. The markers exhibit a relative standard deviation of resonant frequency well below 0.3%.
Having thus described the invention in rather full detail, it will be understood that such detail need not be strictly adhered to, but that additional changes and modifications may suggest themselves to one skilled in the art, all falling within the scope of the invention as defined by the subjoined claims.
This application is a continuation-in-part of U.S. patent application Ser. No. 11/705,946, filed Feb. 14, 2007, and entitled “Electronic Article Surveillance Marker,” and further claims the benefit of U.S. Provisional Application Ser. No. 60/773,763, filed Feb. 15, 2006, and entitled “Electronic Article Surveillance Marker,” which applications are both incorporated herein in their entirety by reference thereto.
| Number | Date | Country | |
|---|---|---|---|
| 60773763 | Feb 2006 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 11705946 | Feb 2007 | US |
| Child | 11981999 | Oct 2007 | US |
