The present invention relates to pickups for sensing vibrations in a stringed musical instrument and, more specifically, to musical instrument pickups with ferromagnetic pole pieces.
String motion sensors, commonly known as pickups, are installed on guitars, bass guitars, mandolins and other stringed musical instruments to convert the sound produced by the vibrating instrument strings to an electronic signal. In various applications, the electronic signal generated by the pickup may be modified using analog and digital signal processing techniques, amplified, and recorded on a suitable sound recording medium before being converted back to a sound signal by a speaker or other output transducer. Conventional musical instrument pickups use different physical principles, including variations in magnetic reluctance, the Hall effect and the piezoelectric effect, to detect the motion of ferromagnetic strings.
Magnetic reluctance pickups typically comprise one or more ferromagnetic pole pieces, a magnetic source, and a coil with output terminals that surrounds the pole pieces. When the pickup is positioned near the ferromagnetic strings of a musical instrument the magnetic source, pole pieces and strings may be modeled as a magnetic circuit with a magnetic flux in each of the elements. The magnetic flux in a pole piece is partially dependent on the distance between the string-sensing surface of the pole piece and a string. String vibrations change the pole-to-string distance and the pole piece flux. The coil surrounding the pole pieces is said to link the flux in the pole pieces and an electromagnetic force is developed in the coil when the magnetic flux changes. An electronic signal is developed at the output terminals of the coil in response to the electromotive force.
The frequency-dependent response function of a magnetic musical pickup is nonlinear and the input string-motion signal is distorted by the pickup in the process of converting it to an electronic signal. This distortion imparts certain tonal attributes to the string-sensing process and, when properly controlled, adds desirable and highly musical qualities to the output signal.
Magnetic reluctance pickups came into common usage during the 1950's when hard ferromagnetic material and sensor technologies evolved to a point that the pickups could be economically mounted on a musical instrument. Magnetic pickups have been developed for many different instruments and a significant commercial market exists for magnetic guitar pickups. For purposes of clarity, the features of the present invention will be discussed with reference to a 6-string guitar with ferromagnetic strings. It will, however, be obvious to those skilled in the art that the scope of the invention is not limited to 6-string guitars and magnetic pickups that embody features of the invention may be mounted on many different instruments. Other instruments that are commonly equipped with magnetic pickups include, but are not limited to, 12-string guitars, bass guitars, mandolins, and steel guitars.
Magnetic musical instrument pickups may classified into broad categories that reflect differences in basic design and tonal quality. Pickups in the ‘single coil’ category have key design features that are shared by the pickups disclosed in U.S. Pat. No. 2,612,072 issued to H. de Armond on Sep. 30, 1952, U.S. Pat. No. 2,573,254, No. 2,817,261, No. 3,236,930, and No. 4,220,069 respectively issued to Leo Fender on Oct. 30, 1951, Dec. 24, 1957, Feb. 22, 1966, and Sep. 2, 1980 and U.S. Pat. No. 2,911,871 issued to C. F. Schultz on Nov. 10, 1959. The ‘single coil’ name derives from the fact that pickups in this category comprise a set of string-sensing ferromagnetic pole pieces with a magnetic flux that is linked by a single, string-sensing coil of wire. Some single coil pickups have pole pieces that are formed from magnetized hard ferromagnetic materials that generate the flux in the pickup. In other single coil designs a separate permanent magnet induces magnetic fields in the pole pieces. Single coil pickups have no means for external noise rejection and are sensitive to external electromagnetic noise sources.
The external noise sensitivity of a magnetic pickup may be significantly reduced by adding a second wire coil to the pickup. The second coil is designed to generate an electronic output signal at its terminals with a noise component that is similar to the noise output of a first coil. Noise reduction is accomplished by connecting the first and second coils so that the noise signals from the two coils have opposite phases.
Noise-reducing humbucking pickups or ‘humbuckers’ share key design features with the devices that are disclosed in U.S. Pat. No. 2,896,491 ('491) issued to Seth Lover in Jul. 28, 1959 and U.S. Pat. No. 2,892,371 issued to J. R. Butts on Jun. 30, 1959. Pickups in this class have at least two-string sensing coils, each linked to a separate set of string-sensing pole pieces. The magnetic field direction in the poles and the direction of signal propagation within the coils are selected so that a large portion of the string-generated signals from the two are coils have an in-phase, additive relationship and a large percentage of the common-mode noise signals from the two coils have an out-of-phase, subtractive relationship. Split-blade designs such as the Lindy Fralin Split-blade pickups manufactured by Lindy Fralin of Richmond, Va. also fall into the ‘humbucking’ category. In most cases, the amplitude of the output signal of a humbucking pickup is greater than that obtained from a single coil pickup and the output noise signal is significantly reduced.
Noise-cancelling single coil pickups have tonal characteristics similar to those of single coil pickups and comprise a single set of string-sensing pole pieces, a string sensing coil and a noise cancelling coil that is connected to the string-sensing coil. Illustrative noise-cancelling single coil pickups are disclosed in U.S. Pat. No. 7,166,793 issued to Kevin Beller on Jan. 23, 2007, U.S. Pat. No. 7,189,916 issued to Christopher I. Kinman on Mar. 13, 2007, and U.S. Pat. No. 7,227,076 issued to Willi L. Stich on Jun. 5, 2007.
The design and manufacture of magnetic musical instrument pickups are described from an historical and lay engineering perspective in The Guitar Pickup Handbook, the Start of Your Sound by Duncan Hunter (Backbeat/Hal Leonard, New York, 2008) and Pickups, Windings and Magnets and the Guitar Became Electric, by Mario Milan (Centerstream, Anaheim Hills, 2007). On a more technical level, Engineering the Guitar, Theory and Practice by Richard Mark French (Springer, New York, 2009) contains a chapter on Guitar Electronics and a thorough treatment of musical sound quality and tone as viewed from an engineering and physics perspective.
In some embodiments, magnetic musical instrument pickups according to the invention have one or more string-sensing composite pole pieces. Each composite pole piece has two or more ferromagnetic components with different material properties and is assembled so that one surface of each ferromagnetic component is fixed in a contiguous position with respect to a surface of a different ferromagnetic component. In contrast to conventional pole pieces that are formed from one or more pieces of a single material, the integrated ferromagnetic properties of a composite pole piece may be engineered over a wide parameter space to obtain desirable tonal characteristics from a pickup in which they are mounted.
The ferromagnetic components of a composite pole piece may be formed from hard or soft ferromagnetic materials. The magnetization states of hard ferromagnetic components may vary over a wide range and, in some cases, a hard ferromagnetic component may be unmagnetized.
Depending on the component shapes and pole piece design, the contiguous surfaces of component pieces may be approximately parallel or perpendicular to a plane that is tangent to a string-sensing surface of the composite pole piece at its center. Composite pole piece components may be held in fixed relative positions by joining the pieces together or pole piece components may be held together by mechanical pressure. Soldering, bonding with an adhesive, and other known techniques may be used to join the components. In some cases, the bonding materials may be electrically conductive and/or magnetically permeable.
In further embodiments, the invention is a magnetic pickup that comprises a first set of pole pieces, each having a string-sensing surface, a magnetic device that generates a magnetic field in the set of pole pieces, and at least one string-sensing wire coil with output terminals that links a magnetic flux in the first set of pole pieces. The set of pole pieces may be magnetized and, in such cases, they are at least a component of the magnetic device.
The first set of pole pieces may comprise two or more composite pole pieces. Multiple composite pole pieces may have similar components or they may have components that differ in material properties or volume ratio. In certain embodiments, all of the pole pieces are magnetic composite pole pieces and each composite pole piece has a string-sensing surface that is the surface of a permanent magnet component.
Noise cancelling pickups according to the invention comprise a first set of string-sensing pole pieces, a string-sensing wire coil, a second wire coil that is connected to the string-sensing coil in a noise-cancelling configuration and a magnetic flux source. In humbucking embodiments, the second wire coil surrounds a second set of string-sensing pole pieces and, in noise-cancelling single coil embodiments, the second coil is in electromagnetic communication with a set of passive pole pieces that do not sense string motion.
Other pickups embodying the invention comprise a first set of string-sensing pole pieces, a string-sensing wire coil, a magnetic device that generates a magnetic field in the pole pieces, and a mechanical assembly that holds the pole pieces, coil and magnetic device in a stable configuration. In some cases, the assembly comprises a body for holding at least one composite pole piece component and a removable component holder that applies mechanical pressure in a direction that is normal to the contiguous component surfaces when the component holder is fastened to the body.
In further embodiments the invention provides methods for changing the tone of an existing pickup by reconfiguring at least one monolithic pole piece as a composite pole piece. In certain embodiments, one or more monolithic pole pieces are reconfigured by replacing them with composite pole pieces and, in alternative embodiments, they are reconfigured by adding pole caps.
Magnetic musical instrument pickups are commonly used to sense the motion of strings on a guitar, bass guitar, pedal steel guitar or other stringed musical instrument. When mounted near a ferromagnetic string, a magnetic pickup generates an electronic signal that varies with the string motion. The amplitude of the signal and the fidelity with which it represents the spectrum of the string vibrations are dependent on the detailed design features of the pickup. Typically, the fidelity is not high and it is common practice to describe the distortions introduced by a pickup by attributing a ‘musical tone’ or a ‘tonal quality’ to the device.
The terms ‘musical tone,’ and ‘tonal quality’ are commonly used by those skilled in the art of musical instrument and pickup design to refer to a set of physical parameters that determine the musical qualities of the sound emanating from an instrument or component as perceived by a human observer. In this provisional application, the terms ‘pickup tone,’ ‘tonal quality,’ and ‘sound quality’ will be used interchangeably to describe the contributions of the pickup to the perceptual features of a sound generation process. This process typically includes the conversion of the sound produced by the vibrating strings of the instrument to an electronic signal that passes through one or more signal processing and amplification stages before being converted to sound by a speaker. Because it senses string motion and generates the electronic signal that is amplified and modified by downstream components, the sound quality of a pickup plays a significant role in determining the overall tone of an amplified instrument. Sound qualities that are lost in the conversion of string motion to an electronic signal cannot be regenerated in subsequent signal processing and amplification stages.
According to R. M French in the chapter of Engineering the Guitar, Theory and Practice entitled “Sound Quality” (pp 180-207, Springer, New York, 2009), “few topics are more controversial than sound quality. Skilled players and experienced listeners generally agree on subjective rankings of instruments, but the differences are notoriously difficult to measure and to describe using objective metrics.” Like flavor, artistic quality, and other variables that describe the properties of an item in terms of its effect on human perception, good sound quality and tone are readily recognized by a knowledgeable individual but impossible to completely quantify using physical measurement parameters.
Magnetic instrument pickups generate an output signal when the magnetic flux in one or more string-sensing ferromagnetic pole pieces changes in response to the motion of an instrument string. The pole pieces have magnetic fields that may be self-generated or induced by an external permanent magnet. In a typical magnetic pickup, the flux in the pole pieces is linked by a wire coil and an output signal is generated by the coil in response to string-induced flux variations.
It is well-known within the prior art that pickup tone is affected by the basic pickup design, by the number of turns, wire tensions and winding patterns of the constituent wire coils and by the shape, material and magnetization state of pole pieces and permanent magnets. There is a general understanding of the tonal attributes of monolithic pole pieces that are fabricated from commonly-used permanent magnet materials and steels but a detailed theory relating the tone of a pickup to the ferromagnetic properties of the pole piece materials has yet to be developed. While the qualitative tonal differences between a Stratocaster-style single coil pickup with fully magnetized Alnico 5 pieces and an identical pickup with fully magnetized Alnico 3 pole pieces are well-known, an understanding of these differences in terms of the fundamental electromagnetic material properties of the pole piece materials, including eddy current and hysteresis losses, recoil permeability, coercivity, and residual induction is lacking.
In embodiments of the invention, the tonal properties of a pickup are shaped, at least in part, through the use of one or more composite pole pieces. The composite pole pieces comprise two or more ferromagnetic components and have integrated ferromagnetic properties that may be engineered over a wide parameter space. Pickups that include one or more composite pole pieces typically have tonal attributes that are difficult or impossible to obtain using monolithic pole pieces that are fabricated from a single material.
In pickups embodying the invention, the ferromagnetic properties of composite pole piece components may differ with respect to one or more parameters. One such parameter is the ability of a component to be magnetized as a permanent magnet. Hard ferromagnetic materials differ from soft ferromagnetic materials in at least this respect. Ferromagnetic material properties are described in numerous texts including Ferromagnetism by Richard M. Bozorth (IEEE Press/Wiley, Hoboken, 2003), Permanent Magnetic Materials and their Application by Peter Campbell (Cambridge University Press, Cambridge, 1994) and Modern Ferrite Technology, 2nd Edition by Alex Goldman (Springer, New York, 2006).
As described in these books and elsewhere, pole piece components formed from hard or soft ferromagnetic materials may differ in their ferromagnetic loss coefficients. Ferromagnetic losses are frequency dependent and are commonly described by three material-dependent coefficients: a hysteresis coefficient, an eddy current coefficient and an anomalous loss coefficient.
Hard ferromagnetic component materials may also differ in the shape of their demagnetization curves, the shape of minor hysteresis loops along the demagnetization curve, and in the values of parameters that describe these shapes. Such parameters include, but are not limited to, maximum energy product, recoil permeability, coercive force or coercivity, residual induction and required magnetizing field. Soft ferromagnetic materials may differ in the shape of their magnetization curves, hysteresis loops, and permeability curves and in values of parameters that are derived from them. Such parameters include but are not limited to permeability, incremental permeability, saturation induction, coercive force, residual induction, coercivity and retentivity.
In this application, the string-sensing surface of a pole piece is defined as the surface that is closest to a string when the pickup is mounted in an instrument. In pole pieces with a planar string sensing surface, the string-sensing surface tangent plane is defined by and includes the string-sensing surface. In pole pieces with curved or beveled string-sensing surfaces, the string-sensing surface tangent plane is tangent to the surface at a center point.
In an experimental prototype of the pickup 100, the pole pieces had the same components and the design of the representative pole piece 103 illustrated in
The magnetic field at the string-sensing surface 132 of each of the pole pieces 101-106 was partly self-generated by the magnetized Alnico 5 component 130 and a partly induced by the permanent magnet 109. The permanent magnet 109 was fabricated from ceramic 7 material and had a thickness of approximately 0.25 inches in the magnetization direction. The cross section was approximately rectangular with a width dimension of approximately 0.5 inches and a length dimension of approximately 2.5 inches. In alternative embodiments, the permanent magnet 109 may be formed from any magnetized hard ferromagnetic material including bonded and flexible hard magnetic materials.
The design of the representative Alnico 5/ferrite composite pole piece 103 illustrated in
In alternative embodiments, the pole pieces 101-106 of the pickup 100 may have different designs as illustrated in
In one realization of the design that is illustrated in
The composite pole piece design 160 of
Composite pole pieces may also comprise two or more concentric cylindrical components. The concentric composite pole piece design 170 that is illustrated in
In some embodiments of the invention, the component pieces of the composite pole pieces may have different designs or shapes. For example, a composite pole pickup may have one or more pole pieces with the design of
In alternative embodiments, a single pole cap may be attached to more than one pole piece.
Pole caps 230-235 are mounted in a pole piece holder 228 using a conventional adhesive that may be, for example, cyanoacrylate cement, an epoxy, or a flexible adhesive such as RTV. The holder 228 is attached to the upper end piece 218 with conventional fasteners 238 that allow the holder 228 and pole caps 230-235 to be easily replaced. In a typical application, a musician may have one or two pickups and several different pole cap sets, each optimized for a different style of music.
In an exemplary realization of the
In some magnetic pickups with magnetized pole pieces, keeper bars are used to shape the magnetic field distribution above the pickup. Composite magnetic pole pieces in which the magnetic field is generated by magnetized pole caps offer unique advantages in these designs.
In a novel embodiment of the invention, the pole pieces 255-260 are composite pole pieces with permanent magnet pole caps. The permanent magnet pole caps may advantageously be thin discs of a flexible or bonded permanent magnetic material. The bodies may be monolithic structures that are formed from a single material or they may be composite structures with one or more cylindrical components. In an exemplary realization, the pole caps are 0.060″ thick discs of standard Ultramag flexible magnetic material manufactured by the Flexmag Division of Arnold Magnetics in Marietta, Ohio and the bodies are two-component structures as illustrated in
Magnetic fields of opposite direction are induced in the pole piece sets 305-310 and 315-320 by the permanent magnet 335. The magnetic field in the bar magnet 335 is parallel to the large face of the magnet 335 in the shorter (width) direction. A keeper bar 338 is in contact with the south pole of the magnet 335 and has clearance holes for the screw poles that are positionally matched to the threaded holes in bobbin 330. The keeper bar increases the magnetic coupling between the screw pole pieces 305-310 and the magnet 335. The composite slug pole pieces 315-320 typically contact the north pole of the permanent magnet along their diameters. The bobbin 332 is supported by a spacer 340 and secured to a baseplate 343 by screws 345.
In one example, the pole caps on the composite slug pole pieces 315-320 are 0.187″ dia.×0.020″ thick discs of CMI-B ultralow carbon magnetic iron manufactured by CMI Specialty of Bristol, Conn. The body of each slug has a length of approximately 0.470″ and a diameter of 0.187″ and consists of an upper component that is fabricated from a high carbon music wire and a lower component that is fabricated from low carbon steel alloy such as 1018 alloy. The body components have approximately equal length. The body components and pole caps of each of the composite slug pole pieces are joined together with cyanoacrylate cement or an alternative conventional adhesive.
In alternative embodiments the slug pole pieces 315-320 may comprise at least one conventional monolithic, single material pole piece and one or more composite pole pieces. In embodiments with a multiplicity of composite pole pieces, two or more of the composite pole pieces may have the same designs and materials combined in the same volume ratios. Alternatively, two or more composite pole pieces may differ with respect to design, component materials and/or volume ratios.
In the illustrated humbucking pickup 300 the screw pole pieces are formed from a single material. In other embodiments, however, one or more of the screw pole pieces may be a composite pole piece.
In the design 420, the composite screw pole piece is formed from two machinable ferromagnetic material pieces 426, 423 that are bonded together. Suitable machinable ferromagnetic materials include but are not limited to low and ultralow carbon steels, machinable ferromagnetic stainless steel alloys, alloys of FeCoCr, CuNiFe, and a wide range of bonded hard and soft magnetic materials. Bonded materials are particularly useful in this design due to their wide range of material properties and the ease with which they can be threaded and bonded.
In the design 440, a ferromagnetic Allen screw 443 is threaded into a composite body with components 446,449 that are formed from ferromagnetic materials with different ferromagnetic properties. The screw may be a conventional hardened steel fastener or it may be formed from a different machinable ferromagnetic material. The upper body component 446 may be formed from a machinable carbon steel or an alternative machinable ferromagnetic material. The lower body component 449 is not threaded and may be formed from a wide range of soft and hard ferromagnetic materials, that include soft and hard ferrites and the alnico alloys. Threaded components may be easily cast or machined from bonded soft and hard ferromagnetic materials and any of the pole piece components 443, 446 and 449 may be fabricated from these materials.
Noise cancellation is achieved by connecting the coils 525 and 530 so that the noise signal from the noise cancelling coil 530 is opposite in phase to the noise signal generated by the string sensing coil 525.
In further embodiments, the invention provides methods for changing the tone of an existing pickup by converting one or more monolithic pole pieces to composite pole pieces. Depending on the design of the pickup and monolithic pole pieces, the conversion may be accomplished by replacing a monolithic pole piece with a composite pole piece of approximately the same outside dimensions or by simply mounting a pole cap on the string-sensing surface of a monolithic pole piece. In a conventional humbucking pickup the slug pole pieces are press fit into one bobbin and the screw pole pieces are typically threaded into the other bobbin. According to the invention, one or more of the slug pole pieces may be replaced by composite pole pieces and/or one or more of the screw pole pieces may be replaced by composite screw pole pieces. Possible designs for the slug pole pieces are illustrated in
In one example of the pole piece replacement method, the low carbon steel slugs of a 9000 Ohm, PAF-style humbucking bridge pickup manufactured by Lindy Fralin Pickups of Richmond, Va. were replaced by composite pole pieces that each comprised a 0.5″ long cylinder of low loss, medium permeability ferrite material (Magnetic Arts of Escondido, CA part number FRD18750x6) and a 0.060″ thick cylinder of low carbon steel. The components of each pole piece were joined with cyanoacrylate cement. The original pole pieces were pushed out of the bobbins and the replacements inserted so the string-sensing surfaces of each replacement pole piece was a surface of the low carbon steel component.
If the pole pieces of a pickup are the primary supporting structures for a coil, removing one or more of them can destroy the pickup. Pickups with coil-supporting pole pieces include, but are not limited to, the pickups in the Custom Shop Texas Special, 57/62 and '69 Stratocaster pickup sets manufactured by Fender Musical Instrument Company of Scottsdale, Ariz. In an alternative embodiment, the invention provides a method that may be used to alter the tone of any pickup with ferromagnetic pole pieces, including those with coil supporting pole pieces. This method comprises the step of attaching a pole cap to the string-sensing surface of the original pole piece. In an exemplary realization of this method, the harmonic content and the low-frequency response of the neck pickup in a set of Custom Shop Texas Special pickups was modified by attaching pole caps to the low E, A and high E pole pieces. The low E and A pole caps were 0.187″ diameter by 0.030″ discs of a low loss, medium permeability ferrite material with ferromagnetic material properties similar to those of Fair-Rite Material 77 and the high E pole piece was a 0.017″×0.040″ thick disc of partially magnetized Alnico 2.
It will be obvious to those skilled in the art that the representative embodiments described in this application are but a small fraction of the large number of different embodiments that can be obtained by incorporating composite pole pieces in conventional magnetic pickup designs. For example, composite pole pieces may be advantageously incorporated in P-90 pickups, mini-humbucking pickups including NY, Johnny Smith, and Firebird style mini-humbuckers, split rail single coil pickups, narrow-field humbucker pickups, lipstick tube pickups, active pickups, and pickups with one or more blade-type pole pieces. It will additionally be obvious that composite pole pieces may be the basis for new and novel pickup designs with tonal characteristics that cannot be obtained using conventional single-material pole pieces.
This application claims priority to U.S. Provisional Patent Applications 61/258,454, “Method for Modifying the Tone of a Musical Instrument Pickup” which was filed on Nov. 5, 2009 and 61/258,912, “Single Coil Pickup with Increased Tonal Range,” which was filed on Nov. 6, 2009. Both applications are incorporated herein by reference in their entirety.
Number | Name | Date | Kind |
---|---|---|---|
2573254 | Fender | Oct 1951 | A |
2612072 | De Armond | Sep 1952 | A |
2612541 | De Armond | Sep 1952 | A |
2817261 | Fender | Dec 1957 | A |
2892371 | Butts | Jun 1959 | A |
2896491 | Lover | Jul 1959 | A |
2909092 | De. Amond | Oct 1959 | A |
2911871 | Schultz | Nov 1959 | A |
2933967 | Riscol | Apr 1960 | A |
3236930 | Fender | Feb 1966 | A |
3249677 | Burns et al. | May 1966 | A |
3541219 | Abair | Nov 1970 | A |
3983777 | Bartolini | Oct 1976 | A |
3983778 | Bartolini | Oct 1976 | A |
4184398 | Siegelman | Jan 1980 | A |
4220069 | Fender | Sep 1980 | A |
4320681 | Altilio | Mar 1982 | A |
4524667 | Duncan | Jun 1985 | A |
4624172 | McDougall | Nov 1986 | A |
5168117 | Anderson | Dec 1992 | A |
5221805 | Lace | Jun 1993 | A |
5378850 | Tumura | Jan 1995 | A |
5389731 | Lace | Feb 1995 | A |
5391831 | Lace | Feb 1995 | A |
5408043 | Lace | Apr 1995 | A |
5530199 | Blucher | Jun 1996 | A |
5668520 | Kinman | Sep 1997 | A |
5792973 | Riboloff | Aug 1998 | A |
5811710 | Blucher et al. | Sep 1998 | A |
5834999 | Kinman | Nov 1998 | A |
5949014 | Rashak et al. | Sep 1999 | A |
6103966 | Kinman | Aug 2000 | A |
6111185 | Lace | Aug 2000 | A |
6392137 | Isvan | May 2002 | B1 |
6846981 | Devers | Jan 2005 | B2 |
6998529 | Wnorowski | Feb 2006 | B2 |
7022909 | Kinman | Apr 2006 | B2 |
7166793 | Beller | Jan 2007 | B2 |
7189916 | Kinman | Mar 2007 | B2 |
7227076 | Stich | Jun 2007 | B2 |
8178774 | Salehi | May 2012 | B2 |
20020020281 | Devers | Feb 2002 | A1 |
20020083819 | Kinman | Jul 2002 | A1 |
20040003709 | Kinman | Jan 2004 | A1 |
20060112816 | Kinman | Jun 2006 | A1 |
20060156911 | Stich | Jul 2006 | A1 |
20070017355 | Lace | Jan 2007 | A1 |
20080245218 | Stewart | Oct 2008 | A1 |
20100005954 | Higashidate et al. | Jan 2010 | A1 |
20100101399 | Calvet | Apr 2010 | A1 |
20100122623 | Salo | May 2010 | A1 |
Entry |
---|
Hunter, Duncan et al., “The Guitar Pickup Handbook, The Start of Your Sound”(Backbeat/Hal Leonard, New York, 2008) (total of 260 pages). |
Milan, Mario, “Pickups, Windings and Magnets and the Guitar Became Electric”, (Centerstream, ANaheim Hills, 2007) (total of 216 pages). |
French, Richard M., “Engineering the Guitar, Theory and Practice”, (Springer, New York, 2009) (total of 274 pages). |
Bozworth, Richard M., “Ferromagnetism”, (IEEE Press/Wiley, Hoboken, 2003) (total of 492 pages). |
Bozworth, Richard M., “Ferromagnetism”, (IEEE Press/Wiley, Hoboken, 2003) Second Part of AP (total of 493 pages). |
Campbell, Peter, “Permanent Magnetic Materials and their Application” (Cambridge University Press, Cambridge, 1994) (total 218 pages). |
Goldman, Alex. Modern Ferrite Technology, 2nd Edition, (Springer, New York, 2006), Part 1 (total pp. 218). |
Goldman, Alex. Modern Ferrite Technology, 2nd Edition, (Springer, New York, 2006), Second Part of AS (total pp. 218). |
Errede, Professor Steven, Presentation entitled “Electronic Transducers for Musical Instruments”, Department of Physics, The University of Illinois at Urban-Campaign, AES Talk, UIUC, Nov. 29, 2005 (43 pages). |
Lemme, Helmuth E.W., “The Secrets of Electric Guitar Pickups”, updated Feb. 25, 2009, retrieved from http://buildyourguitar.com/resources/leme/ on May 10, 2009 (9 pages). |
Sulzer, Mike, “Music Electronics Forum”, retrieved from http://music-electronic-forum.com/t13930/ on Sep. 23, 2009 (9 pages total). |
Article entitled Common Magnetic Terminology as Used in Specification and Claims of U.S. Appl. No. 12/940,478 retrieved from Wikipedia at http://en.wikipedia.org/wiki/Magnet. |
Article entitled “Seymour Duncan Zephyr TM, The Next Great Sound of Guitar” retrieved from http://www.seymourduncan.com/newproducts/zephyr-silver-pickups.php on Oct. 29, 2011 (2 pages). |
Ressler, Phil, “Zephyr Silver Background”, retrieved from http://www.seymourduncan.com/forum/showthread.php?t=207793 on May 16, 2012 (15 pages). |
Number | Date | Country | |
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61258454 | Nov 2009 | US | |
61258912 | Nov 2009 | US |