EP1382221B1

EP1382221B1 - Inertial exciter for loudspeaker

Info

Publication number: EP1382221B1
Application number: EP01980673A
Authority: EP
Inventors: Andreas New Transducers Ltd. Cygnet House BUOS; Martin New Transducers Ltd. Cygnet Hous COLLOMS
Original assignee: New Transducers Ltd
Current assignee: NVF Tech Ltd
Priority date: 2000-11-08
Filing date: 2001-11-01
Publication date: 2012-01-04
Anticipated expiration: 2021-11-01
Also published as: HK1058454A1; CN1486580A; BR0115155A; MXPA03004022A; CN1243458C; WO2002039781A2; GB0027278D0; WO2002039781A3; EP1382221A2; JP4080870B2; JP2004515097A; ES2379763T3; AU2002212466A1

Abstract

According to a first aspect of the invention there is provided an inertial exciter (40) for an acoustic radiator (42), the exciter comprising a massive member (44); a coupling member (46, 56) adapted for attachement to the acoustic radiator (42) and adapted for relative movement to the massive member (44); a motor for moving the coupling member (46, 56) relative to the massive member; and a suspension (60) for supporting the massive member; and a suspension (60) for supporting the massive member relative to the coupling member. The suspension (60) acts in a plane generally passing through the centre of mass of the massive member, thereby reducing any moment acting on the suspension means. A second aspect of the present invention consists in a loudspeaker exciter assembly (70) comprising a base plate (86) for attachement to an acoustic radiator in a non-repeatedly engageable manner; and an exciter (40) attached to said base plate (86) in a repeatedly engageable manner.

Description

This invention relates to drivers or exciters for loudspeakers, in particular but not exclusively for the class of loudspeakers known as bending wave panel-form loudspeakers.
Such loudspeakers are known, for example from WO97/09842 to New Transducers Ltd. In general, such speakers include a resonant bending wave plate and a transducer mounted on the plate to convert electrical signals into mechanical vibrations. The transducer excites the resonant bending wave modes in the plate, which then emit sound to create an acoustic output.
The properties of the acoustic radiator may be chosen to distribute the resonant bending wave modes substantially evenly in frequency. In other words, the properties or parameters, e.g. size, thickness, shape, material etc., of the acoustic radiator may be chosen to smooth peaks in the frequency response caused by "bunching" or clustering of the modes. The resultant distribution of resonant' bending wave modes may thus be such that there are substantially minimal clusterings and disparities of spacing.
In particular, the properties of the acoustic radiator may be chosen to distribute the lower frequency resonant bending wave modes substantially evenly in frequency. The number of resonant bending wave modes is less at lower frequency than at higher frequency and thus the distribution of the lower frequency resonant bending wave modes is particularly important. The lower frequency resonant bending wave modes are preferably the ten to twenty lowest frequency resonant bending wave modes of the acoustic radiator. The resonant bending wave modes associated with each conceptual axis of the acoustic radiator may be arranged to be interleaved in frequency. Each conceptual axis has an associated lowest fundamental frequency (conceptual frequency) and higher modes at spaced frequencies. By interleaving the modes associated with each axis, the substantially even distribution may be achieved. There may be two conceptual axes and the axes may be symmetry axes. For example, for a rectangular acoustic radiator, the axes may be a short and a long axis parallel to a short and a long side of the acoustic radiator respectively. For an elliptical acoustic radiator, the axes may correspond to the major and minor axis of the ellipse. The axes may be orthogonal.
The transducer location may be chosen to couple substantially evenly to the resonant bending wave modes. In particular, the transducer location may be chosen to couple substantially evenly to lower frequency resonant bending wave modes. In other words, the transducer may be mounted at a location spaced away from nodes (or dead spots) of as many lower frequency resonant modes as possible. Thus the transducer may be at a location where the number of vibrationally active resonance anti-nodes is relatively high and conversely the number of resonance nodes is relatively low. Any such location may be used, but the most convenient locations are the near-central locations between 38% to 62% along each of the length and width axes of the panel, but off-central. Specific locations found suitable are at 3/7,4/9 or 5/13 of the distance along the axes; a different ratio for the length axis and the width axis is preferred.
A particularly preferred kind of exciter for use with bending wave loudspeakers is the inertial exciter, an example of which is shown attached to a panel form member 15 in Figure 1. The exciter 14 comprises an electromagnetic motor made up of a magnet assembly and a voice coil assembly. The magnet assembly comprises a magnet 20, a pole piece 22 and a magnet cup 24 such that the magnet 20 is sandwiched between and attached to both the pole piece 22 and the magnet cup.
The voice coil assembly comprises a voice coil wound on a former 27 which is attached to a coupler ring 28 which in turn is mounted on a mounting surface of the panel-form member 15. The magnet assembly is mounted on the voice coil assembly by means of a suspension 32 attached between the voice coil former 27 and the magnet cup.
Through audio connections 34, the exciter 14 receives electrical signals which are fed to voice coil. In accordance with well-known electromagnetic principles, these signals result in a force being exerted on the magnet assembly, with a reaction force being exerted on the voice coil, coupler ring and finally the panel 15. As a result of the higher mass (inertia) of the magnet assembly, it is the panel 15 that moves and, in combination with the preferential positioning mentioned above, generates sound.
The present inventors have identified two problems with known methods of mounting the magnet assembly.
Firstly, when installed on a non-horizontal panel as shown in Figure 1, the exciter tends to "creep", i. e. twist on its suspension under the effect of the weight, W, of the magnet assembly acting through its centre of mass, M.
Secondly, the exciter may exhibit rocking modes which degrade power handling, shorten life, and increase distortion. In particular, leakage of energy into rocking modes may impair the power delivery at the lowest frequencies.
Further issues surround the mounting of the exciter as a whole: as is known, it may be advantageous to attach an exciter to a bending wave, panel-form loudspeaker by means of adhesive. However, should an exciter attached in this manner develop a fault, it will be necessary to break the adhesive joint and remove adhesive residue from the surface of the loudspeaker panel before a replacement exciter can be attached by means of a new adhesive bond.
An electromagnetic inertial exciter is described in WO 98/34320 ; the exciter comprising a motor coil assembly, a magnet assembly disposed concentrically with respect to the motor coil assembly and means suspending the magnet assembly for axial movement relative to the motor coil assembly.
It is an object of the invention to ameliorate these problems and provide an improved exciter for use in such loudspeaker applications.
According to a first aspect of the invention there is provided an inertial exciter for an acoustic radiator as set out in claim 1.
As a result of an aspect of the invention as set out in the latter feature in claim 1, the exciter may have dynamic balance and suspension drift or creep under the force of gravity for a vertical placement may be alleviated.
It should be noted that in the context of the patent application, the term massive member generally means any member having a mass greater than the remaining components of the exciter combined.
The application also describes a loudspeaker exciter assembly comprising:

a base plate for attachment to an acoustic radiator in a non-repeatedly engageable manner; and
an exciter attached to said base plate in a repeatedly engageable manner.

Such an arrangement provides the vibration transfer benefits of a non-repeatedly engageable connection - such as adhesive - to the loudspeaker panel together with ease of replaceability of the exciter unit associated with a repeatedly-engageable, releasable connection such as a screw thread.
Also included in the invention are loudspeakers incorporating the aforementioned aspect.
Further advantageous embodiments of the invention are set out in the description and dependent claims.
The invention will now be described by way of example by reference to the following diagrams, of which:

Figure 1 is a cross-section of a known prior art exciter;
Figure 2 is a cross-section of an exciter according to a first embodiment of the invention;
Figure 3 is an exploded view of the exciter of Figure 2;
Figures 4A and 4B are perspective and cross-sectional views of an exciter according to a second embodiment of the invention; and
Figure 5 is a cross-section of an exciter according to a third embodiment of the invention.

Figure 1 shows a known prior art exciter 14 and is described in detail above. As is shown in Figure 1, the suspension 32 is spaced away from the plane of centre of mass 36 of the magnet assembly 16.
Figures 2 and 3 show an exciter 40 according to the present invention. In Figure 2, the exciter 40 is mounted on an acoustic radiator 42 and comprises an electromagnetic motor made up of a magnet assembly 44 and a voice coil assembly 46. The magnet assembly 44 comprises a magnet 48, a pole piece 50 and a magnet cup 52 such that the magnet 48 is sandwiched between and attached to both the pole piece 50 and the magnet cup 52. The voice coil assembly 46 comprises a voice coil 54 wound on a former 55 which is attached to a coupler 56.
The voice coil assembly 46 of the exciter 40 is attached to the acoustic radiator 42 via the coupler 56 mounted on a mounting surface 58 of the acoustic radiator 42. The magnet assembly 44 is mounted on the voice coil assembly 46 by means of a suspension spider 60 attached between the coupler 56 and the magnet cup 52.
As shown in Figure 3, the coupler 56 is in the form of a shallow cup and is made of plastics. The coupler 56 has a generally disc-like base 57 which provides a large bonding area for mounting on the acoustic radiator 40 and a side wall 63 running around the circumference of and at an angle of approximately 45 ° to the plane of the base. Three individual mounting provisions 64 project from the top of the side wall 63 and are equally spaced around the circumference of the base. The mounting provisions 64 are generally cylindrical. A fourth projection 65 which is generally flat with a larger surface area than that of the cylindrical mounting provisions 64 also projects from the side wall 63 and may be used to support the connections (not shown).
The suspension spider 60 is a planar, member in the form of a ring having three arms 67 and may be considered to be in the form of a metal cantilever suspension. The ring of the suspension spider 60 is fixed to the outside of the magnet cup 52 whilst one end of each arm 67 carries a suspension point 68, each of which coincide with one of the three individual mounting provisions 64 on the coupler 56. The coupler 56 may be fixed to the metal cantilever suspension by soldering tags.
As shown in Figure 2 and in contrast to the prior art exciter 14 of Figure 1, the suspension points 68 are in the plane of the centre of mass 66 of the massive member of the exciter, in this case the magnet assembly 48,50,52. Thus the exciter is balanced and the problems of "creep" of the suspension under the force of gravity when the exciter is mounted in non-horizontal orientation should be alleviated. It will also be appreciated that such balance will help reduce unwanted rocking modes of the massive magnet assembly relative to the voice coil.
Furthermore, such an arrangement provides much stiffer lateral support in both vertical mounting positions of the exciter (i.e. desk top multimedia, picture speaker application ect.) and in horizontal mounting positions (i.e. ceiling speakers etc.) may be provided. Thus, linear distortions caused by unstable support of the voice coil position in the air gap of the magnetic circuit may be prevented.
In addition, stable support of the magnet assembly relative to the voice coil allows gap tolerances to be tightened, thereby providing greater sensitivity and available force.
Advantageously, the suspension support point 60 is located towards a periphery of the exciter and at a greater radial diameter than for conventional constructions. The resulting additional support may provide improved restoring forces to control residual unwanted asymmetric movement. In particular, the stability of linear magnet movement is enhanced and a linear imparting of a mechanical force [N] at the drive point of a panel is provided.
In the particular embodiment shown, the exciter 40 is attractively light weight, slim and robust, having a 25 mm diameter, 4 ohm impedance and a short voice coil 54 which receives signals through audio connections 62 mounted on one of the mounting provisions 64.
It will be appreciated that the first aspect of the invention is not restricted to the embodiment detailed above. For example, the suspension means may be a spider formed from a corrugated foil of metal or polymer or a strengthened cloth. Alternatively, the suspension means may be in the form of an arm type cantilever which may be made from polymer or thin metal e.g. stainless steel or beryllium copper. The suspension means may be made from low corrosion metal alloys for high stress environments. Such metal alloys are generally resistant to adverse effects of humidity and temperature, are low fatigue and have good long-term stability. The cantilever suspension means may also be formed by thermoforming pressing or moulding, for example, for foil or thin plate suspension means. The suspension means may be attached to the coupler, for example by a screw and stud construction or alternatively by use of adhesive to reduce mass. Alternatively, the suspension means may be co-moulded or moulded integrally with the coupler.
It will also be appreciated that by attaching the exciter to suspension means in the plane of the centre of mass of the magnet assembly, a portion of the mass of the suspension means may add to the mass of the exciter at a driving point on the acoustic radiator. Accordingly, the design of the exciter should take into account the additional mass.
As regards the magnet assembly comprising a magnet sandwiched between a magnet cup and a pole piece, the cup defining a magnet gap around the magnet, the magnet gap may be filled with retentive fluid of suitable viscosity to damp motion of the voice coil. Such fluid may also provide thermal dissipation.
Finally, it should be understood that whilst the massive member of the first aspect is most likely to be the magnet assembly of an electromagnetic motor system, the invention does include non-electromagnetic arrangements and electromagnetic arrangements in which a voice coil or its equivalent fulfil the role of the massive member.
Figures 4A and 4B are perspective and sectional views of a loudspeaker exciter assembly 70 incorporating an exciter 40 similar to that of figure 2 but having reduced thickness. The same reference figures have been used for those features common to the two exciters. However, the orientation of the illustration has been reversed so as to better show the second aspect of the invention, namely a base plate 86 for attachment in a non-repeatable manner to the surface of a loudspeaker panel (not shown). To this end, the surface 87 of the plate is formed with annular grooves 88 to accommodate adhesive.
Base plate 86 is in turn provided with a screw connection 90 which allows releasable - and thus repeatable - engagement of an exciter 40. As in the previous embodiment, this comprises a magnet assembly made up of magnet 48, pole piece 50 and magnet cup 52. This assembly is suspended for movement (denoted by arrow 92) relative to coupling member 56 by a suspension spider 60. In the example shown, the inner periphery of spider 60 is mounted on magnet cup 52 such that it acts in a plane 66 generally passing through the centre of mass of' the magnet assembly, in accordance with the first aspect of the invention.
The outer periphery of spider 60 is attached, e.g. by means of screws 93, to mounting provisions 64 of the coupling member 56. As in the earlier embodiment, coupling member 56 also carries a former 55 on which is wound a voice coil 54. This sits in an annular gap 94 formed by the extremities of the pole piece 50 and cup 52 and, as is well known, excites the magnet assembly to movement when supplied with an electrical drive signal via connections 62. A bellows seal 94 protects coil and gap from dirt, moisture and the like without inhibiting this movement.
The security of the releasable screw thread connection between coupling member 56 and base plate 86 is ensured in the embodiment shown by pawls 95 formed on base plate 86 and which engage with corresponding racks 96 formed on the coupling member 56. In a manner generally known per se, the teeth of the pawls and racks are so angled as to allow the screw connection to be tightened but to prevent it from being released without intervention to disengage the pawl and rack. Such intervention, e.g. by means of a screwdriver, allows the exciter 40 to be detached and a replacement unit to be installed quickly, easily and independently of the adhesive bond between the panel and base plate 86.
It will also be understood that alternative designs, e.g. of the screw connection and pawl locking arrangements, can be used. Similarly, alternatives to adhesive for non-repeatably attaching the base plate to the acoustically-radiating loudspeaker panel can be used or indeed the base plate can be formed integrally with the panel.
Figure 5 shows an exciter 98 similar to the exciter 40 of Figure 2 but having an annular compliant member 97 incorporated into the side wall 63 of the coupler 56. The compliant member 97 has a lower compliance than the compliance of the suspension spider 60 and is connected in mechanical series between a region of the coupler local to the voice coil and regions of the coupler to which the suspension means is attached or electrical lead out connections are located. By adding the compliant member, a lower effective mass at the driving point may be achieved with respect to the electrical lead out connections and the suspension means.
The compliant member may have a lower compliance than the compliance of the suspension means in order not to effect the suspension means. Nevertheless the compliant member may act to decouple a proportion of the mass of the suspension means at higher frequencies from the voice coil assembly. Thus, the compliant section should improve the high frequency bandwidth without affecting a main resonance of the exciter system. The compliant section may also introduce a second resonance to the exciter which may adjust the overall frequency response of the exciter. The exciter system may further comprise damping to control spurious resonances. The damping may be in the form of a resilient layer and/or a visco-elastic layer in contact with any one of the compliant section or the suspension means which may introduce resistive damping.

Claims

Inertial exciter for an acoustic radiator, the exciter comprising:
a massive member comprising a magnet assembly (44);

a coupling member (56) adapted for attachment to the acoustic radiator and adapted for relative movement to the massive member, the coupling member (56) comprising a voice coil assembly (46); and

a suspension means for supporting the massive member relative to the coupling member (56);

wherein the magnet assembly (44) and the voice coil assembly (46) form an electromagnetic motor for moving the coupling member (56) relative to the massive member

characterised in that the suspension means acts in a plane generally passing through the centre of mass of the massive member, thereby reducing any moment acting on the suspension means.
Inertial exciter according to claim 1, wherein the suspension means is generally planar.
Inertial exciter according to claim 1 or claim 2, wherein the suspension means is a spider formed from a corrugated foil of metal or of polymer or a strengthened cloth.
Inertial exciter according to claim 1, wherein the suspension means is in the form of an arm type cantilever.
Inertial exciter according to claim 4, wherein the suspension means is made from polymer or thin metal.
Inertial exciter according to any one of the preceding claims, wherein the suspension means is co-moulded or moulded integrally with the coupler.
Inertial exciter according to any one of the preceding claims, further comprising a compliant member connected in mechanical series connection between a region of the coupler local to the voice coil and regions of the coupler to which the suspension means is attached or electrical lead out connections are located.
Inertial exciter according to claim 7, wherein the compliant member has a lower compliance than the compliance of the suspension means.
Inertial exciter according to any of the preceding claims, further comprising damping to control spurious resonances.
Inertial exciter according to any one of the preceding claims, wherein the magnet assembly comprises a magnet sandwiched between a magnet cup and a pole piece, the cup defining a magnet gap which is filled with retentive fluid of suitable viscosity to damp motion of the voice coil.
Inertial exciter according to any one of the preceding claims, further comprising a support to provide restoring forces to control residual unwanted asymmetric movement the support being located towards a periphery of the exciter.
Bending wave loudspeaker comprising an acoustic radiator and mounted thereon an inertial exciter according to any of claims 1 to 11.