EP1201102B1 - Loudspeaker - Google Patents

Loudspeaker Download PDF

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Publication number
EP1201102B1
EP1201102B1 EP00946162A EP00946162A EP1201102B1 EP 1201102 B1 EP1201102 B1 EP 1201102B1 EP 00946162 A EP00946162 A EP 00946162A EP 00946162 A EP00946162 A EP 00946162A EP 1201102 B1 EP1201102 B1 EP 1201102B1
Authority
EP
European Patent Office
Prior art keywords
duct
panel
cavity
loudspeaker according
frequency
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
EP00946162A
Other languages
German (de)
English (en)
French (fr)
Other versions
EP1201102A2 (en
Inventor
Neil Harris
Graham Bank
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NVF Tech Ltd
Original Assignee
New Transducers Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by New Transducers Ltd filed Critical New Transducers Ltd
Publication of EP1201102A2 publication Critical patent/EP1201102A2/en
Application granted granted Critical
Publication of EP1201102B1 publication Critical patent/EP1201102B1/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Classifications

    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R1/00—Details of transducers, loudspeakers or microphones
    • H04R1/20—Arrangements for obtaining desired frequency or directional characteristics
    • H04R1/22—Arrangements for obtaining desired frequency or directional characteristics for obtaining desired frequency characteristic only 
    • H04R1/28—Transducer mountings or enclosures modified by provision of mechanical or acoustic impedances, e.g. resonator, damping means
    • H04R1/2807—Enclosures comprising vibrating or resonating arrangements
    • H04R1/2853—Enclosures comprising vibrating or resonating arrangements using an acoustic labyrinth or a transmission line
    • H04R1/2857—Enclosures comprising vibrating or resonating arrangements using an acoustic labyrinth or a transmission line for loudspeaker transducers
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R1/00—Details of transducers, loudspeakers or microphones
    • H04R1/20—Arrangements for obtaining desired frequency or directional characteristics
    • H04R1/22—Arrangements for obtaining desired frequency or directional characteristics for obtaining desired frequency characteristic only 
    • H04R1/28—Transducer mountings or enclosures modified by provision of mechanical or acoustic impedances, e.g. resonator, damping means
    • H04R1/2807—Enclosures comprising vibrating or resonating arrangements
    • H04R1/283—Enclosures comprising vibrating or resonating arrangements using a passive diaphragm
    • H04R1/2834—Enclosures comprising vibrating or resonating arrangements using a passive diaphragm for loudspeaker transducers
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R7/00—Diaphragms for electromechanical transducers; Cones
    • H04R7/02—Diaphragms for electromechanical transducers; Cones characterised by the construction
    • H04R7/04—Plane diaphragms
    • H04R7/045—Plane diaphragms using the distributed mode principle, i.e. whereby the acoustic radiation is emanated from uniformly distributed free bending wave vibration induced in a stiff panel and not from pistonic motion
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R7/00—Diaphragms for electromechanical transducers; Cones
    • H04R7/02—Diaphragms for electromechanical transducers; Cones characterised by the construction
    • H04R7/04—Plane diaphragms
    • H04R7/06—Plane diaphragms comprising a plurality of sections or layers

Definitions

  • This invention relates to loudspeakers and more particularly to loudspeakers incorporating resonant panel acoustic radiators.
  • electrical circuits can adequately equalise the peak.
  • equalisation may not be desirable in high quality products - for example ambient temperature may affect the electrical circuits differently from the acoustical properties.
  • Damping is another way to reduce such coupled mode peaks. This is again more suited to low quality applications. Moreover, damping increases the width of the peaks and so a system can sound worse with damping than without.
  • shallow cavity is meant a cavity which has ceased to function as a volume behind the panel but in which the finite thickness gives rise to effects such as the coupled whole body mode within the acoustic range.
  • the cavity will need to be less than half the smaller dimension of the panel in its plane before such effects become significant, preferably less than a quarter or further preferably less than 10% of the smaller dimension. The shallower the cavity, the thinner the loudspeaker can be and this is generally desirable.
  • the sound is selectively absorbed at the coupled mode frequency it is not required that the absorption is exactly tuned to a specific frequency.
  • the whole body mode resonance can be quite broad and the absorption can advantageously be suitably broad as well.
  • the solution proposed may allow several advantages over the alternative approaches. Firstly, the cost of providing the duct can be absorbed in the cost of providing the initial tooling to form the cavity. The approach may also be tolerant of temperature changes, since these are likely to affect the air in the duct and the cavity in parallel. The approach is also permanent.
  • the coupled mode can be the whole body mode, since this is in general the dominant mode in a shallow cavity and hence the mode that requires reduction.
  • One end of the duct may be open to the cavity.
  • the other end is closed. Slots may be provided in the duct to adjust the properties of the cavity.
  • the duct can be tuned as a quarter wavelength duct to a frequency within 10% of the coupled mode frequency.
  • a starting point for the length of the duct is a quarter wavelength of the sound wave at the required frequency, the exact length depends on end corrections, and whether the duct is bent. Such corrections are well known in the art. Accordingly, by "quarter wavelength duct” is meant an appropriately tuned duct, not a duct of exactly that wavelength.
  • the coupled mode absorption may be quite broad over the frequency range so it is not necessary for the length to be precisely a quarter of the wavelength of the frequency of the coupled mode.
  • the duct is tuned to a frequency within 5% of the coupled mode frequency.
  • a quarter wavelength converts a real impedance to an imaginary, and vice versa. Accordingly, a quarter wavelength duct can act as an effective acoustic absorber for sound at the frequency for which its length is a quarter wavelength.
  • the ducts need not be straight. Slight curvatures barely affect them, and sharp bends add acoustic mass, causing them to tune low. This effect can be countered by altering the length of the duct appropriately, as is known.
  • the ducts can be located either inside or outside the main cavity, as required.
  • the sound absorbing material may be acoustic fibre and/or foam plastic.
  • the duct may be both coupled to the cavity and separated from the cavity by a membrane, so that the duct in effect forms an auxiliary cavity.
  • the coupled system of the duct and membrane may be arranged to resonate at approximately the coupled mode/whole body mode frequency in the cavity.
  • the cavity can be in a different plane to the main cavity.
  • absorbing material in the duct may be useful.
  • the membrane itself may be absorbing, by providing damping in the membrane, and/or by providing a damped suspension of the membrane.
  • the duct is an aperture connecting the cavity with the ambient.
  • the length determines the tuning of the duct
  • the width and area of the duct provide some tuning. That is because the area can be too small for lower frequencies to readily pass through, whereas at higher frequencies the area has a low sound radiation efficiency.
  • a strip may be provided around the edge of the panel to support the panel on the box, wherein the strip is omitted over part of the edge to so that the panel, box and strip define the duct; in this case the duct may be open to the air away from the cavity.
  • the strip may be a resilient strip to resiliently support the panel. In this way, the panel can be freely mounted, i.e. not clamped at the edges.
  • the duct is a hole provided in the front of the panel, or alternatively in the box. Such holes are in the central area of panel or of the rear of the box. Such ducts are less frequency selective than a quarter wave plate, but this can be sufficient for some applications.
  • a plurality of ducts as described above may be provided for reducing sound pressure at the coupled mode frequency.
  • a plurality of quarter-wave ducts tuned to different frequencies are provided acoustically connected to the cavity. This changes the resonant modes in the cavity, and in particular the ducts may be selected to reduce the fundamental frequency of the cavity and also increase the density of coupled resonant modes in frequency.
  • the panel may be a distributed mode panel which operates by having a variety of resonant modes distributed in frequency.
  • the increase in the number of modes for the coupled enclosure system can significantly improve the properties of a distributed mode loudspeaker having such multiple selective frequency control.
  • the quarter-wave ducts may be provided along one side of the cavity, in which case that side of the cavity may be considered to act as a sound absorber.
  • the technique in all its forms, is thought for resonant bending wave loudspeakers the technique can also be used for removing unwanted resonance or resonances in any panel coupled to a shallow cavity. This may allow a shallow box pistonic loudspeaker to be manufactured.
  • a distributed mode panel 11 is produced using the teaching of WO97/09842.
  • the panel is of a preferred distributed mode aspect ratio, i.e. 1:882 or 1:0.707.
  • a transducer 13 is mounted on the rear of the panel at a preferred transducer location.
  • a shallow box 15 defines a shallow cavity 17 in co-operation with the panel 11.
  • a duct 19 is provided at one end of the cavity.
  • the duct is one quarter of the wavelength of the coupled whole body mode of the panel 11 on the spring constituted by the air in the cavity 17 and any resilience in the panel 11 supports. Sound absorbing material 21 is provided in the duct 19.
  • the second embodiment is shown viewed from behind through the rear of the cavity 17 that is 260mm by 210mm.
  • the panel 11 forms the upper surface of the cavity and the transducer is shown at 13.
  • Four ducts 19 are provided, one on each side wall of the cavity.
  • the ducts are each 120mm long; accordingly, they are all intended to tune the same resonance, here the whole body mode resonance.
  • Figure 3 shows the results achieved.
  • the original frequency response is shown with a dashed and dotted line and the response with the ducts with a dashed line.
  • Figure 4 shows similar arrangement to the embodiment of Figure 1 except that a membrane 23 is provided to divide the duct 19 from the cavity 17.
  • the duct 19 is tuned to resonate at the whole body mode frequency.
  • the duct 19 may be in a different plane to the main cavity.
  • Damping 21 is provided in the duct: the damping may be acoustic fibre or foam as conventionally used for acoustic damping.
  • the membrane may have a density chosen to act in co-operation with a resilient support of the membrane to vibrate at a resonant frequency to determine the selected resonant frequency of the duct.
  • the resilient support may be provided in the duct, and may comprise foam, the air in the cavity or a combination of the two.
  • Figures 5 and 6 show a fourth embodiment of the invention.
  • the panel 11 is supported on the box 15 by a resilient strip 29 around the panel edge.
  • the panel is supported 5mm from a rim 31 on the box.
  • the box 15 and panel 11 are separated around the circumference of the panel by a 2mm gap therebetween.
  • the strip has gaps in its length defining slots 33 along one side of the panel.
  • the slots function as ducts but act in a different way to a quarter wavelength duct - they act as vents releasing sound pressure particularly at the whole body mode frequency.
  • Damping 21 is provided in the cavity, fixed to the panel 11.
  • Figure 10 shows a schematic diagram of a cavity with six quarter wavelength ducts 19 of different lengths, from 80 to 180mm in 20mm steps. These provide multiple frequency selective acoustic termination.
  • the ducts 19 function to make the boundary acoustically effectively invisible over a range of frequencies. Calculations have shown that the number of useful resonant modes of the coupled system can significantly increase; the modes qualitatively differ from the modes without the ducts. Table 1 lists the resonant modes with the quarter wave ducts in the first three columns and without in the final three. It can clearly be seen that the number of modes is much higher with the ducts than without.
  • the cavity appears less stiff by controlling sound pressure at the whole body mode frequency so that the lowest coupled mode is now at a beneficially lower frequency.
  • the lowest mode is at 388Hz rather than 660Hz without changing the volume of air or the external dimensions of the box.
  • the modal density of the system is also increased by about 50% in the range up to 3KHz range shown in the table.

Landscapes

  • Otolaryngology (AREA)
  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
  • Signal Processing (AREA)
  • Health & Medical Sciences (AREA)
  • Obtaining Desirable Characteristics In Audible-Bandwidth Transducers (AREA)
  • Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
  • Details Of Audible-Bandwidth Transducers (AREA)
  • Liquid Crystal (AREA)
  • Surgical Instruments (AREA)
  • Media Introduction/Drainage Providing Device (AREA)
  • Chair Legs, Seat Parts, And Backrests (AREA)
  • Soundproofing, Sound Blocking, And Sound Damping (AREA)
EP00946162A 1999-07-30 2000-07-24 Loudspeaker Expired - Lifetime EP1201102B1 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
GB9917908 1999-07-30
GBGB9917908.7A GB9917908D0 (en) 1999-07-30 1999-07-30 Loudspeakers
PCT/GB2000/002784 WO2001010168A2 (en) 1999-07-30 2000-07-24 Loudspeaker

Publications (2)

Publication Number Publication Date
EP1201102A2 EP1201102A2 (en) 2002-05-02
EP1201102B1 true EP1201102B1 (en) 2003-07-02

Family

ID=10858223

Family Applications (1)

Application Number Title Priority Date Filing Date
EP00946162A Expired - Lifetime EP1201102B1 (en) 1999-07-30 2000-07-24 Loudspeaker

Country Status (11)

Country Link
EP (1) EP1201102B1 (zh)
JP (1) JP2003526968A (zh)
CN (1) CN1250042C (zh)
AT (1) ATE244494T1 (zh)
AU (1) AU6003700A (zh)
DE (1) DE60003692D1 (zh)
GB (1) GB9917908D0 (zh)
HK (1) HK1042012B (zh)
NZ (1) NZ516351A (zh)
TW (1) TW490988B (zh)
WO (1) WO2001010168A2 (zh)

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7426804B2 (en) 2002-02-06 2008-09-23 Andersen Corporation Specialty display window
US6988339B2 (en) 2002-02-06 2006-01-24 Andersen Corporation Specialty media window
US7207413B2 (en) * 2003-06-02 2007-04-24 Tbi Audio Systems Llc Closed loop embedded audio transmission line technology for loudspeaker enclosures and systems
GB0400323D0 (en) * 2004-01-08 2004-02-11 New Transducers Ltd Loudspeakers
GB0410962D0 (en) 2004-05-17 2004-06-16 Mordaunt Short Ltd Loudspeaker
US20060061504A1 (en) * 2004-09-23 2006-03-23 The Regents Of The University Of California Through wall detection and tracking system
WO2007109828A1 (en) * 2006-03-28 2007-10-04 Immersion Technology Property Limited Loudspeaker system with acoustic equalisation
CN104038855A (zh) * 2014-06-04 2014-09-10 瑞声光电科技(常州)有限公司 电声器件及所述电声器件的组装方法
WO2018070399A1 (ja) 2016-10-13 2018-04-19 パナソニックＩｐマネジメント株式会社 平板スピーカおよび表示装置
CN107205194B (zh) * 2017-06-07 2020-03-06 鞠波 一种音箱以及音箱系统

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3848090A (en) * 1971-11-18 1974-11-12 J Walker Wall hanging speaker system
US3938617A (en) * 1974-01-17 1976-02-17 Fort Enterprises, Limited Speaker enclosure
US4899390A (en) * 1986-09-19 1990-02-06 Matsushita Electric Industrial Co., Ltd. Thin speaker having an enclosure within an open portion and a closed portion
DE69110530T2 (de) * 1990-04-20 1996-02-29 Matsushita Electric Ind Co Ltd Lautsprechersystem.
UA51671C2 (uk) * 1995-09-02 2002-12-16 Нью Транзд'Юсез Лімітед Акустичний пристрій

Also Published As

Publication number Publication date
AU6003700A (en) 2001-02-19
ATE244494T1 (de) 2003-07-15
HK1042012B (zh) 2003-10-03
WO2001010168A3 (en) 2001-08-16
GB9917908D0 (en) 1999-09-29
NZ516351A (en) 2002-09-27
HK1042012A1 (en) 2002-07-26
WO2001010168A2 (en) 2001-02-08
TW490988B (en) 2002-06-11
CN1250042C (zh) 2006-04-05
DE60003692D1 (de) 2003-08-07
JP2003526968A (ja) 2003-09-09
CN1360809A (zh) 2002-07-24
EP1201102A2 (en) 2002-05-02

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