Receiver with coil wound on a stationary ferromagnetic core

Information

  • Patent Grant
  • 9888322
  • Patent Number
    9,888,322
  • Date Filed
    Monday, November 23, 2015
    9 years ago
  • Date Issued
    Tuesday, February 6, 2018
    6 years ago
Abstract
A receiver includes an acoustic module and a coil module. The acoustic module includes a first housing, a plurality of magnets, and an armature. The armature is disposed within the first housing and extends between the plurality of magnets. The coil module is coupled to the acoustic module, is physically separate from the acoustic module, and includes a second housing and a coil. The coil disposed within the second housing and does not surround the armature. The coil is excitable by an electrical current representative of acoustic energy and excitation of the coil produces a magnetic flux path which moves the armature.
Description
FIELD OF THE INVENTION

This application relates to acoustic devices and, more specifically, to hearing aid receivers and their design.


BACKGROUND OF THE INVENTION

Various types of microphones and receivers have been used through the years. In these devices, different electrical components are housed together within a housing or assembly. For example, a receiver typically includes a coil, magnets, a reed, among other components and these components are housed within the receiver housing. Other types of acoustic devices may include other types of components.


In receiver applications, a coil is used to induce magnetic flux or field as electrical current is run through the coil. The magnetic field is induced into a ferromagnetic core which comprises a portion of a magnetic circuit. As the magnetic flux or field is induced into the magnetic circuit a portion of the magnetic circuit called the reed (or armature) is moved relative to the coil, this in turn moves a paddle, and sound is thereby created as the paddle moves the air. In some applications, the armature is configured to move air itself without the need of an attached paddle. The sound can consequently be presented to and heard by a listener.


In previous systems, the movable reed comprised at least a portion of the electromagnetic core of the coil, thus the coil had to be configured to provide a tunnel of space around the reed within which the reed is able to move unimpeded during normal operation of the receiver. In some versions, structures within the coil would be provided to impede motion of the reed during abnormal events such as the receiver striking a surface after being dropped. The coil would have to be constructed and assembled into the receiver with very tight tolerances, and the coils became expensive to build and complicated and expensive to integrate with the rest of the components of the receiver.


Another problem with previous approaches was that the coil was typically fit around the moving portion of the reed. Unfortunately, by winding the coil around the moving portion of the reed, the overall shape and configuration receiver was limited.


Another problem was that coils were often configured to match the electrical requirements of the specific application. With previous approaches, coils were deeply integrated into the construction of the receiver, and not removable or configurable after the initial manufacturing steps. As a result, manufacturing efficiency was lower due to lack of commonality early in the manufacturing process.


As a result of the disadvantages mentioned above, user dissatisfaction with previous approaches has resulted.





BRIEF DESCRIPTION OF THE DRAWINGS

For a more complete understanding of the disclosure, reference should be made to the following detailed description and accompanying drawings wherein:



FIG. 1 comprises a top cut-away view of a receiver according to various embodiments of the present invention;



FIG. 2 comprises a top cut-away view of the yoke assembly of the receiver of FIG. 1 according to various embodiments of the present invention;



FIG. 3 comprises a top cut-away view of the coil module of the receiver of FIG. 1 according to various embodiments of the present invention;



FIG. 4 comprises an external perspective view of the receiver of FIG. 1 according to various embodiments of the present invention;



FIG. 5 comprises a magnetic circuit diagram of the receiver of FIG. 1 according to various embodiments of the present invention;



FIG. 6 comprises a top-cut-away view of a two-coil receiver according to various embodiments of the present invention;



FIG. 7 comprises a magnetic circuit diagram of the receiver of FIG. 6 according to various embodiments of the present invention;



FIG. 8 comprises a top cut-away view of another example of a two-coil receiver according to various embodiments of the present invention;



FIG. 9 comprises a side cut-away view of two-coil receiver of FIG. 8 according to various embodiments of the present invention.





Skilled artisans will appreciate that elements in the figures are illustrated for simplicity and clarity. It will further be appreciated that certain actions and/or steps may be described or depicted in a particular order of occurrence while those skilled in the art will understand that such specificity with respect to sequence is not necessarily required. It will also be understood that the terms and expressions used herein have the ordinary meaning as is accorded to such terms and expressions with respect to their corresponding respective areas of inquiry and study except where specific meanings have otherwise been set forth herein.


DETAILED DESCRIPTION

Approaches are provided where one or more coils in receivers are configured to be fixedly attached to or directly wound upon a ferromagnetic core which comprises a portion of the magnetic circuit. So arranged, the coils do not require precision tolerances thereby making the coils significantly less expensive to manufacture as compared to previous coils. In addition, approaches are provided whereby one or more coils can be easily installed with other components to form a receiver module. In still another aspect, two (or potentially more) coils are provided and these coils are easily aligned with other magnetic components. The receivers provided herein have highly customizable designs, shapes, and dimensions, are easy to manufacture, and are significantly less expensive to produce as compared to previous devices.


Referring now to FIGS. 1-5, one example of a receiver 100 is described. The receiver 100 includes an acoustic module 102 and a coil module 150.


The acoustic module 102 includes a reed 104 and a yoke assembly 106. As used herein, the term “reed” is used interchangeably with “armature”. In any case, the term “reed” refers to a typically thin, flat and relatively long component that moves in the presence of a changing magnetic flux. The changing magnetic flux may be created by an electrical current that passes through a coil and interacts with magnetic fields produced by permanent magnets in a yoke assembly. In one example, the reed is constructed of soft magnetic steel, or “mu-metal”. Other examples of materials may be used to construct the reed. In another aspect, the reed 104 is constructed with thin and broad dimensions so as to act as a paddle. In one example, the reed 104 is 0.007 inch thin and 0.050 inch wide. One end of the reed 104 is attached (e.g., welded) to a soft magnetic steel bar 112 that protrudes from the receiver housing 142, 144, 146.


The yoke body 107 is constructed of soft magnetic steel and includes magnets 108 and 109 attached to yoke body 107. A hollow tunnel (or channel) 110 is formed and extends through the center of the yoke assembly 106. One end portion of the reed 104 extends into the tunnel 110. The other end portion of the reed 104 is attached to the bar 112. In one example, the bar is constructed of a metal.


The coil module 150 includes a coil 152. The coil 152 is wound around a soft magnetic steel core 154 that is attached to coil end portions 156 and 158. The coil module 150 couples to the acoustic magnetic module 102. It will be appreciated that since the coil module is secured to the acoustic magnetic module 102 and that the coil 152 is not wound around the moving portion of the reed 104, the coil 152 remains stationary (or substantially stationary) during operation of the receiver 100. It will be further appreciated that since the coil wire is tightly wound around the core, and that the wire is in contact with the core and does not form a tunnel within which the core could move with respect to the coil, as in previous receiver designs.


As can be seen in FIGS. 1-5, the moving portion of the reed 110 is not disposed down the axis of coil. Thus, the coil 152 does not need to be precisely placed or have a precise tolerance to avoid interference with the movement of the reed.


As mentioned and as shown, the coil 152 is not disposed on, around, or about the moving portion of the reed 104. The proximity of the coil module 150 next to the acoustic magnetic module 102 is used during operation of the receiver to create a magnetic flux path 140. As alternating current is applied to the coil 152, the flux path 140 is created by the interaction of the electrical current in the coil and magnetic fields created by the permanent magnets 108 and 109. The flux path 140 moves the reed 104. More specifically, as the reed 104 moves, the air about the reed 104 moves thereby creating sound. In other words, the reed 104 acts as a diaphragm and no separate diaphragm element is needed. The sound tube receives the produced sound for presentation to a user.


In one aspect, the magnetic flux path 140 is closed and carries all static flux plus the worst case dynamic flux. The dynamic flux produced by the coil 152 splits the gap/channel 110 in twain, and has closed paths without requiring shunts.


The coil module 150 is a self-contained unit. The coil 152 is wire that is wound on a micro-metal core, encapsulated except on one face where micro-metal is exposed. A terminal is attached to coil module 150 to provide an electrical interface to the coil wire.


It will be appreciated that the receiver 100 can be easily customized by replacing coil module 150. Thus, the size, shape, dimensions, performance characteristics, among other features of the coil module 150 can be customized to the particular needs and requirements of a particular acoustic module 102.


The receiver 100 includes a top half cup housing portion 142, a bottom half-cup housing portion 144, and an end cap housing portion 146. The housing portions 142, 144, and 146 cannot be constructed of ferromagnetic materials but are instead constructed of some non-ferromagnetic material (such as plastic or hard stainless steel) that will not short the magnetic circuit. A terminal board 148 couples to the coil module 150 and provides a connection with external components. A reed magnetic terminal 149 extends from the bottom cup housing portion 144. Yoke magnetic terminals 143 are exposed. The coil module has terminals 137 and 139 which couple respectively to terminals 149 and 143. In so doing, the magnetic flux path 140 can be created.


In one example, a manufacturing process for creating the receiver 100 includes welding the thin, wide reed 104 to the bar 112. In one aspect, the reed 104 may have a pie-pan shape to prevent flexing. Other examples of shapes may also be used. Then, a ring 113 welded to bar 112. A thin film 114 is attached to ring 113 and reed 104.


The yoke assembly 106 (including the yoke body 107, and magnets 108 and 109) is placed over the reed 104. In this respect, the position of the yoke assembly 106 is adjusted to center the reed 104 in the channel 110. The yoke assembly 106 is affixed to the bottom half cup housing portion 144, for example, using welding or glue. The top half-cup housing portion 142 and the end cap housing portion 106 are added (attached). The magnetic terminals (i.e., the exposed side of bar and yoke) are polished so as to provide an adequate magnetic connection.


The use of the detachable coil module 150 makes the present approaches highly customizable. In this respect, an appropriate coil module can then be attached to the module 102. In addition, the cup housing portions mentioned above can also be exchanged out, for instance, to create more back volume in the receiver 100 as needed. For instance, housing portions having different dimensions, shapes, and configurations can be fitted to the particular needs of a particular receiver. In one example, a housing portion providing an increased back volume may be used to improve the performance characteristics of the receiver 100. It will be appreciated that the cup housing portions 142, 144, and 146 are the primary structured members of the receiver 100.


Referring now to FIG. 6 and FIG. 7, a receiver motor 600 with two coils is described. As shown, the receiver has a first coil 602 and a second coil 603. The coils 602 and 603 include coil cores 610 and 612 and the coil cores 610 and 612 carry the static flux as well as the dynamic flux that is created during operation of the receiver 600. The receiver 600 includes a reed 604, a yoke assembly 606 (that includes a yoke body 607, a first magnet 608, and a second magnet 609). It can be appreciated that all the sources of magnetic radiation in the receiver 600 (i.e., the coil and magnets) are aligned. A tunnel 620 is disposed through the yoke assembly 606 and extends between the magnets 608 and 609. In one aspect, the reed 604 is secured between the coils 602 and 603 and extends between the gap created by the tunnel 620 between the magnets 606 and 608.


As can be seen in the receiver of FIGS. 6 and 7, the coils 602 and 603 are not disposed around the moving part of the reed 620. Thus, the coils 602 and 603 do not need to be precisely placed or be constructed with precise tolerances. It will also be understood that although two coils are shown in this example (as well as the example of FIGS. 8 and 9), any number of coils may be used.


In one example of the operation of the system of FIG. 6 and FIG. 7, an alternating electrical current is generated and flow through the coils 602 and 603. The flow of the alternating electrical current through the coils 602 and 603 interacts with the magnetic field produced by the magnets 608 and 609 to generate a magnetic flux. The magnetic flux flows in a direction indicated by the arrow labeled 622 down the reed 604 and moves the reed 604. Reed 604 may then be attached to a paddle of a receiver, not show in FIG. 6.


Referring now to FIGS. 8 and 9, another example of a receiver 800 with two coils is described. As shown, the receiver 800 includes a first coil 802 and a second coil 803. The coils 802 and 803 are wound about coil cores 810 and 812 and the coil cores 810 and 812 carry the static flux as well as the dynamic flux during operation of the receiver 800. The receiver 800 includes a reed 804, a yoke assembly 805 (that includes a yoke body 807, a first magnet 808, and a second magnet 809). It can be appreciated that all the sources of magnetic radiation in the receiver 800 (i.e., the coils and the magnets) are aligned. A tunnel 820 is formed in the yoke assembly 805 between the magnets 806 and 808. The reed 804 is secured between coils and has a tongue 823 that extends in the tunnel 820. An opening 821 extends through the reed 804.


As can be seen in FIGS. 8 and 9, the coils 802 and 803 are disposed out of the tunnel 820. Thus, the coils 802 and 803 do not need to be precisely placed or be constructed with precise tolerances.


In one example of the operation of the system of FIG. 8 and FIG. 9, an alternating electrical current is generated and flow through the coils 802 and 803. The flow of the alternating electrical current through the coils 802 and 803 interacts with the magnetic field produced by the magnets 808 and 809 to generate a magnetic flux. The magnets and coils are contained within a yoke assembly 805. The magnetic flux flows in a direction indicated by the arrow labeled 622 (in FIG. 6 which is also the equivalent magnetic circuit for the devices shown in FIG. 8 and FIG. 9) down the reed 804 and acts to move the tongue 823 of the reed 804. Consequently, the reed 804 (and its tongue 823) acts as a diaphragm. As the reed 804 moves, the air around the reed 804 is moved thereby creating sound. The sound moves through the sound tube of the receiver 800 and after it exits the sound tube can be presented to a user.


It will be appreciated that in the approaches described herein, the sources of magnetic radiation are aligned. Because of the alignment, there is a much greater control of this magnetic radiation as compared to previous approaches. For instance, the amount and direction of created magnetic flux is better controlled.


Preferred embodiments of this invention are described herein, including the best mode known to the inventors for carrying out the invention. It should be understood that the illustrated embodiments are exemplary only, and should not be taken as limiting the scope of the invention.

Claims
  • 1. A receiver comprising: an acoustic module, wherein the acoustic module includes a first housing, a plurality of magnets, and an armature, the armature disposed within the first housing and extending between the plurality of magnets; anda coil module coupled to the acoustic module through terminals that provide a magnetic flux path from the coil module to the acoustic module, wherein the coil module is physically separate from the acoustic module and includes a second housing and a coil, the coil disposed within the second housing and not surrounding the armature;wherein the coil is excitable by an electrical current representative of acoustic energy and excitation of the coil produces a magnetic flux path which moves the armature.
  • 2. The receiver of claim 1, wherein the acoustic module is detachable from the coil module.
  • 3. The receiver of claim 1, wherein the armature is 0.007 inches in thickness and 0.050 inches wide.
  • 4. The receiver of claim 1, wherein the coil comprises a wire that is wound around a micro-metal core.
  • 5. The receiver of claim 1, wherein the first housing and the second housing are constructed of a non-ferromagnetic material.
  • 6. The receiver of claim 1, wherein one or more of the acoustic module and the coil module are interchangeable with other acoustic modules and coil modules.
  • 7. A dual coil receiver comprising: a first coil disposed on a first supporting structure;a second coil disposed on a second supporting structure;a yoke coupled to one or more magnets; andan armature, wherein a first end of the armature is mounted between the first supporting structure and the second supporting structure such that the first coil and the second coil do not surround the armature;wherein excitation of one or more of the first coil and the second coil produces a magnetic flux path which moves the armature.
  • 8. The dual coil receiver of claim 7, wherein the one or more magnets include two magnets, the two magnets form a gap there between, and a second end of the armature extends through the gap.
  • 9. The dual coil receiver of claim 7, wherein the first coil comprises wire wound about the first supporting structure and the second coil comprises wire wound about the second supporting structure.
CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of U.S. Provisional Patent Application Ser. No. 62/088,197, filed Dec. 5, 2014, entitled RECEIVER WITH COIL FREE REED which is incorporated by reference in its entirety herein.

US Referenced Citations (122)
Number Name Date Kind
1799510 Goldberg et al. Apr 1931 A
3002058 Knowles Sep 1961 A
3515818 Tibbetts Jun 1970 A
3588383 Carlson et al. Jun 1971 A
3617653 Tibbetts et al. Nov 1971 A
3935398 Carlson et al. Jan 1976 A
4002863 Broersma Jan 1977 A
4015227 Riko et al. Mar 1977 A
4109116 Victoreen Aug 1978 A
4272654 Carlson Jun 1981 A
4410769 Tibbetts Oct 1983 A
4450930 Killion May 1984 A
4473722 Wilton Sep 1984 A
4518831 Stanley et al. May 1985 A
4628907 Epley Dec 1986 A
4956868 Carlson Sep 1990 A
5068901 Carlson Nov 1991 A
5101435 Carlson Mar 1992 A
5139717 Peuckert et al. Aug 1992 A
5193116 Mostardo Mar 1993 A
D360691 Mostardo Jul 1995 S
D360948 Mostardo Aug 1995 S
D360949 Mostardo Aug 1995 S
5610989 Salvage Mar 1997 A
5647013 Salvage Jul 1997 A
5708721 Salvage Jan 1998 A
5757947 Van Halteren et al. May 1998 A
5809158 Van Halteren et al. Sep 1998 A
5960093 Miller Sep 1999 A
6041131 Kirchhoefer Mar 2000 A
6075870 Geschiere et al. Jun 2000 A
6078677 Dolleman et al. Jun 2000 A
6654477 Miller Nov 2003 B1
6658134 Van Hal et al. Dec 2003 B1
6751326 Nepomuceno Jun 2004 B2
6757403 Urushibata et al. Jun 2004 B2
6801632 Olson Oct 2004 B2
6931140 Van Halteren et al. Aug 2005 B2
7050602 Miller May 2006 B2
7103196 Warren Sep 2006 B2
7136500 Collins Nov 2006 B2
7164776 Miller Jan 2007 B2
7203334 Schafer Apr 2007 B2
7236609 Tsangaris Jun 2007 B1
7305098 Vonlanthen et al. Dec 2007 B2
7336797 Thompson Feb 2008 B2
7362878 Miller Apr 2008 B2
7366317 Miller Apr 2008 B2
D573588 Warren Jul 2008 S
7415125 Warren Aug 2008 B2
7443997 Miller Oct 2008 B2
7477756 Wickstrom Jan 2009 B2
7680292 Warren Mar 2010 B2
7747032 Zei Jun 2010 B2
7817815 Miller Oct 2010 B2
7860264 Jiles Dec 2010 B2
7869610 Jayanth Jan 2011 B2
7921540 Jiles Apr 2011 B2
7925041 Jiles Apr 2011 B2
7995789 Tsangaris Aug 2011 B2
8027492 Miller Sep 2011 B2
8135163 Blanchard et al. Mar 2012 B2
8233646 Lutz Jul 2012 B2
8284964 Windischberger et al. Oct 2012 B2
8385583 Thompson Feb 2013 B2
8401215 Warren Mar 2013 B2
8494209 Miller Jul 2013 B2
8594351 Harlow et al. Nov 2013 B2
8634587 Nagumo et al. Jan 2014 B2
8824726 Miller Sep 2014 B2
8837755 Jiles Sep 2014 B2
8995705 van Reeuwijk Mar 2015 B2
9137605 Manley Sep 2015 B2
9137610 Jiles Sep 2015 B2
9326074 Jiles Apr 2016 B2
9401768 Inha Jul 2016 B2
20010022844 Urushibata et al. Sep 2001 A1
20020003890 Warren Jan 2002 A1
20020061113 van Halteren et al. May 2002 A1
20020074995 Spellman Jun 2002 A1
20020142795 Imahori Oct 2002 A1
20030021454 Weyl Jan 2003 A1
20030021458 Hamada et al. Jan 2003 A1
20030190053 van Halteren Oct 2003 A1
20040258260 Thompson et al. Dec 2004 A1
20050152574 Van Banning Jul 2005 A1
20060083400 Miller Apr 2006 A1
20060133636 Harvey et al. Jun 2006 A1
20060159298 Von Dombrowski et al. Jul 2006 A1
20060227990 Kirchhoefer Oct 2006 A1
20070036378 Saltykov Feb 2007 A1
20070104340 Miller May 2007 A1
20070133834 vanHalteren Jun 2007 A1
20070223735 Lopresti Sep 2007 A1
20070230734 Beard Oct 2007 A1
20070258616 Tsangaris Nov 2007 A1
20080063223 Van Halteren et al. Mar 2008 A1
20080101640 Ballad May 2008 A1
20080205691 Beekman et al. Aug 2008 A1
20080226115 Beekman et al. Sep 2008 A1
20090060245 Blanchard et al. Mar 2009 A1
20090147983 Jiles Jun 2009 A1
20090214068 Wickstrom Aug 2009 A1
20090296971 Saltykov et al. Dec 2009 A1
20100034418 Bonin Feb 2010 A1
20100054509 Thompson Mar 2010 A1
20100067730 van Halteren et al. Mar 2010 A1
20100128905 Warren et al. May 2010 A1
20100284561 Miller Nov 2010 A1
20100310106 Blanchard Dec 2010 A1
20120008804 Bedwell et al. Jan 2012 A1
20120155694 Reeuwijk Jun 2012 A1
20130051580 Miller Feb 2013 A1
20130190552 Leblans Jul 2013 A1
20130272564 Miller Oct 2013 A1
20140355787 Jiles Dec 2014 A1
20150086049 Jiles Mar 2015 A1
20150110338 McCratic Apr 2015 A1
20150373456 Dayton Dec 2015 A1
20160044420 Albahri Feb 2016 A1
20160183004 Jiles Jun 2016 A1
20160198267 Jiles Jul 2016 A1
Foreign Referenced Citations (53)
Number Date Country
1314771 Sep 2001 CN
1910956 Feb 2007 CN
2899360 May 2007 CN
201234336 May 2009 CN
102428715 Apr 2012 CN
203840067 Sep 2014 CN
203840177 Sep 2014 CN
203840179 Sep 2014 CN
203872027 Oct 2014 CN
203933199 Nov 2014 CN
203951282 Nov 2014 CN
203951286 Nov 2014 CN
203951601 Nov 2014 CN
204046390 Dec 2014 CN
204046391 Dec 2014 CN
204118999 Jan 2015 CN
204119001 Jan 2015 CN
204119490 Jan 2015 CN
204145685 Feb 2015 CN
204168459 Feb 2015 CN
2014168483 Feb 2015 CN
204291354 Apr 2015 CN
204350281 May 2015 CN
204350282 May 2015 CN
204350283 May 2015 CN
204350284 May 2015 CN
204350285 May 2015 CN
204350286 May 2015 CN
105050010 Nov 2015 CN
105340296 Feb 2016 CN
105453588 Mar 2016 CN
105684463 Jun 2016 CN
112014002634 Mar 2016 DE
112014002865 Mar 2016 DE
112014004371 Jun 2016 DE
178195 Aug 2015 DK
1247427 Nov 2003 EP
1281293 Jul 2010 EP
2229339 Sep 1990 GB
03-073099 Jul 1991 JP
2001268692 Sep 2001 JP
2006041768 Feb 2006 JP
2006186615 Jul 2006 JP
2007074499 Mar 2007 JP
2008141694 Jun 2008 JP
4876293 Feb 2012 JP
2013138292 Jul 2013 JP
0074435 Dec 2000 WO
01087008 Nov 2001 WO
2005072009 Aug 2005 WO
2006043964 Apr 2006 WO
2006114767 Nov 2006 WO
2013010384 Jan 2013 WO
Non-Patent Literature Citations (9)
Entry
International Search Report and Written Opinion for PCT/US2015/062418 dated Mar. 28, 2016 (9 pages).
International Search Report and Written Opinion; International Application No. PCT/US2014/039724; dated Sep. 24, 2014.
International Search Report and Written Opinion; International Application No. PCT/US2014/042243; dated Oct. 8, 2014.
International Search Report; International Application No. PCT/US05/000875; dated May 20, 2005.
International Search Report and Written Opinion; International Application No. PCT/US2010/034355; dated Nov. 30, 2010.
International Search Report and Written Opinion; International Application No. PCT/US2015/063713; dated Mar. 28, 2016.
Chinese Search Report with Translation for Chinese Application No. 201080020681.8; 4 pages; dated Sep. 23, 2013.
Danish Patent and Trademark Office, Search Report, Examination Report, Application No. PA 2011 70690, 6 pages.
International Search Report and Written Opinion; International Application No. PCT/US2014/056725; dated Dec. 23, 2014.
Related Publications (1)
Number Date Country
20160165354 A1 Jun 2016 US
Provisional Applications (1)
Number Date Country
62088197 Dec 2014 US