Patent Grant
11937061
The present invention relates to electromechanical transducers and motor structures, and, more particularly, to loudspeaker driver motor structures and methods for cooling transducer voice coils in loudspeaker applications.
Moving-coil transducers (e.g., 100) generate considerable heat in their voicecoils due to inherent electrical resistance of the voicecoil and low efficiency of the transducer. This heat can cause a reduction in performance via “power compression” whereby the voicecoil's electrical resistance increases as the drive power increases, leading to a reduction in expected output, as illustrated in the “std. airflow” temperature and power plots of
High power signals driving a speaker's diaphragm or cone into extreme excursions can cause the (usually pistonic) motion of the diaphragm to become mis-aligned when driven by more challenging audio signals. Typical prior art woofers utilize circular baskets supporting frustoconical driver diaphragms having a circular peripheral edge carrying an annular surround or suspension, as shown in
The edge 108 and damper 109 support the voice coil 102 and voice coil bobbin 103 at respective predetermined positions in a magnetic gap of the magnetic circuit 107, which is constituted of a magnet 104, a plate or washer 105, a pole yoke 106 including a central, axially symmetrical pole piece 115. With this structure, the diaphragm 101 is elastically supported without contacting the magnetic circuit 107 and can vibrate like a piston in the axial direction within a predetermined amplitude range.
The first and second ends or leads of the voice coil 102 are connected to the respective ends of first and second conductive lead wires (not shown) which are also connected to first and second terminals (not shown) carried on frame 112. When an alternating electric current corresponding to a desired acoustic signal is supplied at the terminals to voice coil 102 through the lead wires, the voice coil 102 responds to a corresponding electro-motive force and so is driven axially in the magnetic gap of the magnetic circuit 107 along the piston vibration direction of the diaphragm 101. As a result, the diaphragm 101 vibrates together with the voice coil 102 and voice coil bobbin 103, and converts the electric signals to acoustic energy, thereby producing acoustic waves such as music or other sounds.
Returning to the specifics of the conventional speaker's voice coil gap, the magnetic field or “B” field acting on the voice coil 102 is generated in the annular magnet 104, and the lines of flux pass from magnet 104, through front plate or washer 105, across the annular magnetic gap to the peripheral upper edge of pole piece 115, down through pole piece 115, radially out through yoke 106 and then back into magnet 104, forming a closed loop of magnetic flux. The field strength in the magnetic gap is preferably very high, and so the radial distance across the magnetic gap is something most speaker designers seek to minimize. Narrow and efficient magnetic gaps create other problems, however, because the close mechanical tolerances of a tight magnetic gap require the outer winding surfaces of voice coil 102 to reciprocate in and out in very close proximity to the inner edge of top plate 105. If, during extreme excursions or when expanding due to resistance heating, coil 102 should rub or abrade against the inner edge of top plate 105, then voice coil 102 destroys itself and the loudspeaker fails catastrophically.
Loudspeaker or woofer failure can be often attributed to these types of thermal or mechanical overloading problems. Substantial amounts of power are required to provide very high sound pressure levels, and signals having such power require very large current flow through voice coil conductors, thus generating substantial amounts of heat and driving the woofer's diaphragm to extreme excursions. Those extreme excursions generate extreme mechanical loads on the diaphragm and its supportive suspension. In competitions, operators seek the loudest possible playback and often over-drive the loudspeaker drivers, causing voice coils to burn out or open circuit.
Returning to first principles, the function of a loudspeaker is to convert electrical energy to an analogous acoustical energy. This conversion process takes place in two steps. The first step is the conversion from electrical energy to mechanical energy. The second step is a conversion from mechanical energy to acoustical energy. The first step consists of generating a mechanical displacement proportional to the electrical input signal. The second step consists of coupling the mechanical displacement of the system to the surrounding air via some mechanism, such as forced movement of diaphragm 101. The class of loudspeakers known as electro-dynamic employs a combination of permanent magnet (e.g., 104) and electromagnet to produce the conversion of electrical to mechanical energy.
The permanent magnetic structure in this type of loudspeaker (e.g., 104) utilizes a permanent magnetic material, such as neodymium iron boron, aluminum nickel cobalt, or other rare earth or ceramic materials, that is placed in a “magnetic circuit” consisting of a plate of low carbon steel (e.g., 105) on the north magnetic pole of the permanent magnet and another plate of low carbon steel (e.g., 106) on the south magnetic pole of the permanent magnet. Either the plate on the north magnetic pole or the plate on the south magnetic pole is shaped to provide a small magnetic gap. The magnetic gap is usually annular but need not necessarily be of an annular geometry to be functional. The “magnetic gap” then has a high magnetic field strength. The low carbon steel plates act to concentrate the magnetic field in that volume of space known as the magnetic gap.
The electromagnet portion of the transducer is provided by voice coil 102 which consists of a coiled length of electrical conductor suspended in that magnetic gap. When a time varying electrical current flows through the conductor a magnetic field is produced around the wire and that magnetic field is proportional to the magnitude of the electrical current flowing through the wire in the voice coil. If the permanent magnetic gap has an annular geometry then the electromagnet coil may be immersed into the permanent magnetic gap. This gives rise to a force of interaction between the permanent magnetic field and the electro-magnetic field. This force is known as the Lorentz force and is shown in algebraic form as:
F=BLi (1)
where F is the force of interaction between the two magnetic fields. B is the magnitude of the permanent magnetic field and L is the length of wire immersed in the permanent magnetic field and associated with the coil. In this equation, “i” is the magnitude of the electrical current flowing thru the voice coil's wire.
The force of interaction between the permanent magnetic field and the electro-magnetic, or coil, will produce an acceleration in accordance with Newton's laws of motion.
The motor structure 107 shown in
The ability of the loudspeaker to convert electrical signals to proportional mechanical displacements and subsequently to acoustical energy is often referred to as the conversion efficiency of the transducer, or loudspeaker (e.g., 100). The conversion efficiency is proportional to Lorentz force as well as the total moving mass of the loudspeaker, including voice coil, cone, dust cap, and all parts of the transducer that move relative to the permanent magnet structure and frame. The efficiency of loudspeakers, like all transducers, can be rated as a percentage of the input power to the output power. Typical loudspeakers can range from less than 1% efficient to over 30%. The conversion efficiencies approaching 30% are for a specific type of loudspeaker referred to as compression driver. Typical (non compression driver) loudspeakers range from 1% to 5% efficiency but can be lower or higher as well. These efficiency levels relate the ratio of the electrical input to the acoustic output. As an example, 100 electrical watts of power are typically converted to 3 to 4 watts of acoustic power for a 3% to 4% efficient loudspeaker. The remaining electrical power is converted to heat.
Loudspeaker voice coils can be heated to temperatures of over 450° F. degrees (232° C.). These heat levels are extreme and can produce device failure due to degradation of the adhesive systems used to bond the voice coil to its carrier as well as the adhesives used to bond each turn to the next on the voice coil itself. In addition to device failure, the voice coil's direct current (“DC”) resistance is also affected by heat. Every alloy of conductor has a Temperature Coefficient of Resistance. This coefficient relates the temperature of the conductor to the DC resistance of the conductor. As the temperature increases, the DC resistance of the conductor also increases. As the DC resistance increases, the current flow thru the conductor decreases and is described by Ohms law,
V=I/R (2)
where V is the applied voltage across the voice coil, I is the current flow thru the voice coil and R is the voice coil's DC resistance. As mentioned earlier, the force of interaction between the permanent magnet 104 and the electro-magnet (the voice coil 102) is proportional to the current flow thru the coil 102. If the DC resistance of the voice coil is raised due to heating, then the current draw reduces and, as a consequence, the Lorentz force is reduced.
The change in Lorentz force as a function of DC resistance change from heating is referred to as Power Compression (e.g., as seen in
It is desirable to minimize the heat rise associated with current flowing through the voice coil. Technical reviews of the heat produced by voice coils and subsequent performance alterations can be found in various professional journals. “Heat Dissipation and Power Compression in Loudspeaker”, Douglas Button, J. Audio Eng. Soc., Vol. 40, No. 1/2 1992, and “heat Transfer Mechanisms in Loudspeakers: Analysis, Measurement, and Design”, Clifford a. Henricksen, J.Audio Eng. Soc., Vol. 35, No. 10, 1987 are typical examples of theoretical analysis and measurement of the thermal effects of loudspeaker voice coils.
More elaborate motor structures have been developed in the search for more linear performance over greater excursions such as E.M. Stiles U.S. Pat. No. 6,917,690, which describes a dual-gap geometry including a second 2nd magnet spaced between first and second annular plates (not shown) and this geometry creates an even greater obstruction for convective cooling air flow.
There is a need, therefore, for a loudspeaker motor structure adapted to withstand the thermal extremes encountered in modern high-power long-excursion loudspeaker systems.
There has been summarized above, rather broadly, the prior art that is related to the present invention in order that the context of the present invention may be better understood and appreciated. In this regard, it is instructive to also consider the objects and advantages of the present invention.
It is a primary object of the present invention to overcome the above mentioned difficulties by providing a transducer motor structure adapted to withstand high-excursion, high power loudspeaker applications.
Another object of the present invention is to provide a loudspeaker motor structure economically configured to conduct, convect and radiate heat energy away from the critical voice coil and magnetic gap areas.
Another object of the present invention is to provide a loudspeaker motor structure configured to withstand high thermal loads and overcome the prior art's voice-coil temperature induced dynamic distortion and compression mechanisms.
The aforesaid objects are achieved individually and in combination, and it is not intended that the present invention be construed as requiring two or more of the objects to be combined.
In accordance with the method and structure of the present invention, a new loudspeaker motor configuration includes a transducer motor structure with substantially radial air channels which define inner and outer airflow lumens or vent passages that allow greatly increased airflow which is aimed to impinge directly on the voice coil for maximum cooling effect. The natural pumping action of the transducer is used to drive this airflow. This increased airflow reduces the operating temperature of the voice coil, enhancing the transducer's acoustic output and its durability.
Applicant's work has shown that improving airflow allows more power to be applied to the loudspeaker. The improved transducer of the present invention with increased airflow allows for more power to be applied for the same voice coil temperature, increasing the acoustic output the transducer can generate. In accordance with the present invention, an improved Audio Transducer with Forced Ventilation includes a spacer member defining radial forced ventilation cooling channels or lumens in the ferrous or possibly non-ferrous annular member which is aligned and assembled between the front plate or washer and the basket on the outside.
As will be illustrated and described in greater detail below, the transducer motor structure for generating acoustic vibrations in response to an electrical audio signal, comprises a voice coil former having an open interior lumen with a surface adapted to carry a conductive voice coil and the voice coil former's interior lumen defines an interior pumping volume with a selected axial length. A magnetic circuit comprises at least a first magnet configured to generate a permanent magnetic field, a pole piece having a central axis, a magnetic field return path, and a first magnetic gap defining plate or washer, where the pole piece, return path and first magnetic gap defining plate are all configured to constrain lines of magnetic flux from the permanent magnetic field across a first magnetic gap and where the pole piece projects into the voice coil former's open interior lumen. The magnetic circuit preferably includes a ferrous or magnetically conductive vented annular spacer defining a plurality of (e.g., ten) radially aligned channels or lumens giving fluid communication between the voice coil and the former's interior lumen and the ambient environment surrounding the transducer motor. The magnetic gap defining plate or washer abuts the ferrous or magnetically conductive vented annular spacer and is configured to provide a first magnetic gap selected thickness that is less than the voice coil's selected length.
The transducer motor structure of the present invention is optionally configured with first and second “XBL style” voice coil gaps and the ferrous or magnetically conductive vented annular spacer is then defined as a two-piece assembly comprising an inside annular spacer member (e.g., 355A) and a co-planar outside annular spacer member (e.g., 350-O), each preferably having an equal number of (e.g., ten) axially aligned channels configured to aim cooling airflow at and around the voice coil.
The above and further objects features and advantages of the present invention will become apparent with consideration of the detailed description of specific embodiments thereof, particularly when taken in conjunction with the accompanying drawings, wherein like reference numbers in the various illustrative figures are used to designate like components.
Turning now to
In accordance with the method and structure of the present invention, a new loudspeaker motor structure includes a transducer motor with substantially radial air channels which define inner and outer airflow lumens or vent passages that allow greatly increased airflow which is aimed to impinge directly on the voicecoil for maximum cooling effect. The natural pumping action of the transducer is used to drive this airflow. This increased airflow reduces the operating temperature of the voicecoil, enhancing the transducer's acoustic output and its durability.
As can be seen in the “Increased Airflow” plots of
In accordance with the present invention (e.g., as illustrated in the embodiment of
As noted above, high power signals driving a speaker's diaphragm or cone (e.g., 201) into extreme excursions can cause the (usually pistonic) motion of the diaphragm to become mis-aligned when driven by more challenging audio signals, but the motor structure of the present invention helps maintain voice coil alignment. Woofer 200 utilizes a circular basket supporting frustoconical driver diaphragm 201 having a circular peripheral edge carrying an annular surround or suspension 208. The cylindrical voice coil bobbin 203 carries conductive voice coil 202 wound around its outer circumferential wall and is affixed to the center of a frusto-conical diaphragm 201 or cone, and both are fixed to the inner peripheral edge of annular or ring-shaped surround or edge 208 and to an annular damper or “spider” 209 having a selected compliance and stiffness. The outer peripheral ends of the surround 208 and the spider 209 are fixed to a rigid supportive frame or basket 212 that also carries magnetic circuit 207, so that the frame 212 supports diaphragm 201 and voice coil bobbin 203, which are pistonically movable within the frame along the central axis of bobbin 203. Centered “dust” cap 213 is fixed on the diaphragm 201 to cover the hole at the center of the diaphragm and moves integrally with the diaphragm.
The edge 208 and damper 209 support the voice coil 202 and voice coil bobbin 203 at respective predetermined positions in magnetic gap 208 of the magnetic circuit 207, which (in the embodiment of
The spacer's air flow channels are aligned axially with an equal number of aligned air flow channels defined in vented distal pole tip member 255. With this structure, diaphragm 201 is elastically supported without contacting the magnetic circuit 207 and can vibrate like a piston in the axial direction within a predetermined amplitude range for which cooling air is focused on or around voice coil 202 during excursions.
First and second ends or leads of the voice coil 202 are connected to the respective ends of first and second conductive lead wires (not shown) which are also connected to first and second terminals (not shown) carried on frame 212. When an alternating electric current corresponding to a desired acoustic signal is supplied at the terminals to voice coil 202 through the lead wires, the voice coil 202 responds to a corresponding electro-motive force and so is driven axially in the magnetic gap of the magnetic circuit 207 along the piston vibration direction of the diaphragm 201. As a result, the diaphragm 201 vibrates together with the voice coil 202 and voice coil bobbin 203, and converts the electric signals to acoustic energy, thereby producing acoustic waves such as music or other sounds.
As noted above, the magnetic field or “B” field acting on the voice coil 202 is generated in the annular magnet 204, and the lines of flux pass from magnet 204, through the vented spacer 250 and then through front plate or washer 205, across the annular magnetic gap to the vented distal pole tip member 255 and the peripheral upper edge of pole piece 215, down through pole piece 215, radially out through yoke 206 and then back into magnet 204, forming a closed loop of magnetic flux. The field strength in the magnetic gap is very high, and so the radial distance across the magnetic gap is selected to minimize loss of field strength while enhancing operation and reliability.
The motor in woofer 200 preferably utilizes a permanent magnetic material, such as neodymium iron boron, aluminum nickel cobalt, or other rare earth or ceramic materials, that is placed in magnetic circuit 207 with front plate or washer 205 consisting of a plate of low carbon steel on the north magnetic pole of the permanent magnet 204 and another plate-like surface of low carbon steel (e.g., incorporated in yoke 206) on the south magnetic pole of the permanent magnet. Either the plate on the north magnetic pole or the plate on the south magnetic pole is shaped to provide a small magnetic gap. The magnetic gap is usually annular but need not necessarily be of an annular geometry to be functional. In addition to the annular space defining the magnetic gap 208, the spaces between the annular inner surfaces of magnet 204 and within yoke 206 define a partially enclosed annular volume into which the voice coil former or bobbin can move during an inward excursion. The low carbon steel plates act to concentrate the magnetic field in that volume of space known as the magnetic gap and provide a path for conductive cooling of the voice coil region 208.
The electromagnet portion of the transducer is provided by voice coil 202 which consists of a coiled length of electrical conductor (e.g., copper, aluminum or silver wire of a selected gauge) suspended in magnetic gap 208.
The force of interaction between the permanent magnetic field and the electro-magnetic, or coil, will produce an axial acceleration and direction of the voice coil displacement will be pistonic (either up or down) along the central axis 240. The ability of loudspeaker 200 to convert electrical signals to proportional mechanical displacements and subsequently to acoustical energy or the conversion efficiency is proportional to Lorentz force as well as the total moving mass of the loudspeaker 200, including voice coil 202, cone 201, dust cap 213, and all parts of the transducer that move relative to the permanent magnet structure and frame 212. The efficiency transducer 200 (i.e., the ratio of the electrical input to the acoustic output) is typically greater than for a prior art transducer, since less of the input power is lost to heat, and, as illustrated in the plots labelled “increased airflow”) temperatures are usually lower and power converted to acoustical energy is higher, and less compressed at the highest drive levels.
Typical loudspeaker voice coils can be heated to extreme temperatures of over 450° F. degrees (232° C.). In woofer 200, during operation, the cooling air has been observed to keep voice coil temperatures in an acceptable operating range for very large drive signals over extended test intervals, demonstrably reducing the instances of failure due to degradation of the adhesive systems used to bond the voice coil to its carrier as well as the adhesives used to bond each turn to the next on the voice coil itself. In addition the voice coil's direct current (“DC”) resistance is also less affected by heat. As mentioned earlier, the force of interaction between the permanent magnet 204 and the electro-magnet (the voice coil 202) is proportional to the current flow thru the coil 202, and when the DC resistance of the voice coil is raised due to heating, the current draw reduces and, as a consequence, the Lorentz force is reduced.
The change in Lorentz force as a function of DC resistance change from heating (or Power Compression, e.g., as seen in
In operation, the reciprocating excursions of woofer cone 201 create forced air flow which is aimed by the radial forced ventilation channels defined or incorporated into vented distal pole tip member 255, or into a secondary part or parts that sits on top of the pole 215 and aligned with the radial forced ventilation channels in the annular spacer member 250. These channels redirect airflow from a generally downward path (as seen in
In another embodiment 200A illustrated in
In yet another embodiment 300, the key characteristics of an XBL-type motor are used (See
Returning to the woofer 300 illustrated in
The spacer(s), either the outside, inside or both (e.g., 350-O and 355A), and preferably have aligned radial airflow paths, lumens or channels cut into them (See, e.g.
For Dual Gap woofer 300 (as illustrated in
As noted above, high power signals driving a speaker's diaphragm or cone (e.g., 301) into extreme excursions can cause the (usually pistonic) motion of the diaphragm to become mis-aligned when driven by more challenging audio signals, but the motor structure of the present invention helps maintain voice coil alignment. Woofer 300 utilizes a circular basket supporting frustoconical driver diaphragm 301 having a circular peripheral edge carrying an annular surround or suspension 308. The cylindrical voice coil former or bobbin 303 carries conductive voice coil 302 wound around its outer circumferential wall and is affixed to the center of a frusto-conical diaphragm 301 or cone, and both are fixed to the inner peripheral edge of annular or ring-shaped surround or edge and to an annular damper or “spider” 309 having a selected compliance and stiffness. The outer peripheral ends of the surround and the spider 309 are fixed to a rigid supportive frame or basket 312 that also carries magnetic circuit 307, so that the frame 312 supports diaphragm 301 and voice coil bobbin 303, which are pistonically movable within the frame along the central axis 340. Centered “dust” cap 313 is fixed on the diaphragm 301 to cover the hole at the center of the diaphragm and moves integrally with the diaphragm.
The edge and damper 309 support the voice coil 302 and voice coil bobbin 303 at respective predetermined positions in the magnetic gaps 308A, 308B of the magnetic circuit, which (in the embodiment of
Voice coil former or bobbin 303 optionally includes a sealing voice coil plug 303P which provides a substantially airtight seal at the distal or dustcap end, thus trapping air in the proximal volume enclosed within the interior of the bobbin. The Inside and Outside spacers' air flow channels are aligned axially with an equal number of aligned air flow channels as shown in
In all embodiments, the airflow is driven by the natural pumping action of the key moving parts: cone 301, voicecoil 302, and dustcap 313 or voicecoil plug 303P. During woofer operation, the reciprocating motion provides a pumping action is a normal consequence of the production of sound, as illustrated in
The channels can be shaped in such a way as to smooth the airflow and minimize turbulence. Similar shaping can be applied to the upper inside disk or top of pole to smooth the airflow on the inside of the voicecoil. For example, an optional distally projecting tapered plug (e.g., 355B, as shown in
The air volume contained inside the voicecoil bobbin is preferably sealed near the distal or top end so that the air contained therein is forced through the channels. If the typical dustcap is not of an airtight nature, possibly due to other performance concerns, or the total enclosed air volume is too great, the optional voicecoil plug (e.g., 203P or 303P) can be used inside the voicecoil bobbin or former.
If airflow velocity is too high through the channels and turbulence is created as a result, flow resistance and/or flow straightening may be incorporated placed in the channels to slow and smooth the airflow and reduce turbulence.
If a vented pole (one with a hole through the center) is used, say to save weight or material, then an air flow restrictor may be inserted to block air flowing through the center of the pole, which will would provide an alternate path for air to flow that is not against the voicecoil. If noise generated by airflow turbulence proves to be a problem, this block could be replaced with an attenuating plug that restricts but does not eliminate air flow to reduce the velocity of flow through the spacer channels. A similar feature may be used on the vents in the basket under the spider.
Persons of skill in the art will appreciate that the present invention makes available a transducer motor structure for generating acoustic vibrations in response to an electrical audio signal, and includes: a voice coil former (e.g., 203) having an open interior lumen with a surface adapted to carry a conductive voice coil (e.g., 202) having first and second electrical connections; said voice coil former being configured to drive a diaphragm (e.g., 201); wherein said single voice coil former's interior lumen defines an interior pumping volume with a selected axial length; a magnetic circuit (e.g., 207) comprising at least a first magnet (e.g., 204) configured to generate a permanent magnetic field, a pole piece (e.g., 215) having a central axis (e.g., 240), a magnetic field return path, and a first magnetic gap defining plate or washer (e.g., 205), wherein said pole piece, said return path and said first magnetic gap defining plate are all configured to constrain lines of magnetic flux from said permanent magnetic field across a first magnetic gap (e.g., 208 or 308A); wherein said first magnetic gap is annular and dimensioned to receive said voice coil former in coaxial alignment, such that said voice coil is immersed in the magnetic field in said first magnetic gap; wherein said pole piece (e.g., 215) projects into said voice coil former's open interior lumen and is coaxially aligned with said voice coil former, such that said voice coil is constrained to move axially over said pole piece in response to an audio signal; wherein said magnetic circuit (e.g., 207) includes a ferrous or magnetically conductive vented annular spacer (e.g., 250) defining a plurality of (e.g., ten) radially aligned channels or lumens which provide fluid communication between said voice coil and said former's interior lumen and the ambient environment surrounding the transducer motor; wherein said pole piece has an axial length projecting into said former's lumen that corresponds to voice coil's selected length; and wherein said first magnetic gap defining plate or washer (e.g., 205) abuts said ferrous or magnetically conductive vented annular spacer (e.g., 250) and is configured to provide a first magnetic gap selected thickness, said first magnetic gap selected thickness being less than said voice coil's selected length.
The transducer motor structure of the present invention optionally (e.g., as illustrated in
The transducer motor structure's ferrous or magnetically conductive vented annular spacer co-planar outside annular spacer member (e.g., 350-O) is also preferably cast, machined or forged as a contiguous one-piece member having a substantially planar bottom surface opposite a crenelated upper surface defining a plurality of radially aligned equally spaced channels or lumens, and that crenelated upper surface preferably defines an equal plurality of (e.g., ten) radially aligned equally spaced channels or lumens as the inside annular member, where, preferably each radially aligned channel or lumen is defined along one of inside annular spacer member's radial flow cooling axes 360 and aimed at the voice coil when said transducer motor structure is assembled. Preferably, the ferrous or magnetically conductive vented annular spacer inside annular spacer member (e.g., 355A) and co-planar outside annular spacer member (e.g., 350-O), are each made of a thermally conductive steel alloy.
In the embodiment of
The present invention also makes available an audio speaker (e.g., 300, as seen in
The audio speaker transducer motor structure's ferrous or magnetically conductive vented annular spacer inside annular spacer member (e.g., 355A) is again preferably a contiguous one-piece member having a substantially planar bottom surface opposite a crenelated upper surface defining said plurality of (e.g., ten) radially aligned equally spaced channels or lumens, wherein each radially aligned channel or lumen is defined along a radial flow cooling axis and aimed at said voice coil when said transducer motor structure is assembled.
In accordance with the method of the present invention, the operating temperature of a voice coil (e.g., 202, 302) in a loudspeaker (e.g., 200 or 300) is maintained by:
Having described preferred embodiments of a new and improved transducer motor structure and method, it is believed that other modifications, variations and changes will be suggested to those skilled in the art in view of the teachings set forth herein. It is therefore to be understood that all such modifications, variations and changes are believed to fall within the scope of the present invention as set forth in the following claims.
This application is a continuation of and claims priority to related, commonly owned U.S. utility patent application Ser. No. 17/278,215 filed Sep. 19, 2021 entitled Audio Transducer with Forced Ventilation of Motor and Method, which is a national phase application of and claims priority to U.S. PCT application No. PCT/US19/51923 filed Sep. 19, 2019 also entitled Audio Transducer with Forced Ventilation of Motor and Method, which claims the benefit of priority to U.S. provisional patent application No. 62/733,332 filed Sep. 19, 2018, the entire disclosures of which are incorporated herein by reference and priorities of which are claimed. This application is also broadly related to commonly owned U.S. Pat. Nos. 5,517,573 and 8,638,968, the entire disclosures of which are also incorporated herein by reference.
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| Number | Date | Country | |
|---|---|---|---|
| 20230199394 A1 | Jun 2023 | US |
| Number | Date | Country | |
|---|---|---|---|
| 62733332 | Sep 2018 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 17278215 | US | |
| Child | 18109645 | US |
