WO2006119763A1 - Methode, dispositif et systeme pour modifier le temps de reverberation d'une piece - Google Patents

Methode, dispositif et systeme pour modifier le temps de reverberation d'une piece Download PDF

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Publication number
WO2006119763A1
WO2006119763A1 PCT/DK2005/000322 DK2005000322W WO2006119763A1 WO 2006119763 A1 WO2006119763 A1 WO 2006119763A1 DK 2005000322 W DK2005000322 W DK 2005000322W WO 2006119763 A1 WO2006119763 A1 WO 2006119763A1
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WIPO (PCT)
Prior art keywords
sound
absorbing
frequency
devices
room
Prior art date
Application number
PCT/DK2005/000322
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English (en)
Inventor
Niels Werner Larsen
Original Assignee
Niels Werner Larsen
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 Niels Werner Larsen filed Critical Niels Werner Larsen
Priority to JP2008510408A priority Critical patent/JP4782193B2/ja
Priority to PCT/DK2005/000322 priority patent/WO2006119763A1/fr
Priority to PCT/IB2005/052580 priority patent/WO2006016321A2/fr
Priority to ES05773193T priority patent/ES2400912T3/es
Priority to PL05773193T priority patent/PL1779375T3/pl
Priority to PT57731937T priority patent/PT1779375E/pt
Priority to US10/587,898 priority patent/US7905323B2/en
Priority to SI200531676T priority patent/SI1779375T1/sl
Priority to EP05773193A priority patent/EP1779375B1/fr
Publication of WO2006119763A1 publication Critical patent/WO2006119763A1/fr

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    • G—PHYSICS
    • G10—MUSICAL INSTRUMENTS; ACOUSTICS
    • G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K11/00—Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/16—Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/172—Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using resonance effects

Definitions

  • the present invention relates to a method for altering the reverberation time of a room and particularly to a method for altering the reverberation time of a room in the low-frequency range.
  • the present invention furthermore relates to sound-absorbing devices and systems of such devices used for said altering of the reverberation time of a room.
  • the present invention furthermore relates to a room provided with such devices and/or systems, whereby the reverberation time of the room can be altered.
  • the reverberation time of the room differs for various kinds of music and for speech, recommended reverberation times for rooms in which classical music is to be performed thus being in the range of 1.5 seconds to 2.0 seconds, whereas rooms for performance of rhythmic music have recommended reverberation times in the range of 0.8 seconds to 1.0 seconds. Even shorter reverberation times may be beneficial for auditoriums in order to attain the best possible speech intelligibility. Furthermore, the reverberation time should ideally be almost the same throughout the relevant frequency range of the program material.
  • the reverberation time tends to decrease as a function of frequency, e.g. due to higher sound absorption in air at high frequencies, increased sound absorption at the boundaries of the room at higher frequencies as well as due to the presence of people in the room.
  • low-frequency reverberation often tends to be too high compared with high-frequency reverberation, which may lead to an unacceptably "boomy" reproduction of sounds in the room, a loss of perceived details of the music and even to a deterioration of speech intelligibility.
  • Figure 1 shows measured reverberation time as a function of frequency of seven different rooms that may be used for live performances or reproduction of music.
  • the figure shows an average reverberation time T30 above 500 Hz of approximately 1 second, whereas the average at low frequencies increases to approximately 1 ,5 seconds at 63 Hz. It also appears from figure 1 that large variations of reverberation time exist between the different rooms.
  • a sufficiently thick panel of an acoustic absorptive (porous) material will lead to sound absorption at low frequencies (as well as at higher frequencies) provided the thickness of the panel is sufficiently large compared with the wavelength of the sound at the lowest frequency at which an effective reduction of reverberation time is required.
  • Example of materials applicable for such panels are glass fibre, mineral wool and sintered metals.
  • Such panels may be mounted directly on a boundary or separated from the boundary by an air space, which will improve performance at low frequencies. The panels may also be hung from the ceiling thus giving access to the panel from both sides.
  • such panels will not selectively absorb sound at low frequencies but rather exhibit a sound absorption as a function of frequency which will be fairly constant above a given lower limiting frequency - determined among other things by the thickness of the panel and the acoustic properties of the particular material being used - and decrease below this lower limiting frequency, thus not being able to provide selective low- frequency reduction of reverberation time as often required.
  • panel absorbers or membrane absorbers basically consisting of a rigid frame adapted for mounting on a wall or other boundary of a room. Over the frame and at a given distance from said wall or boundary there is provided a thin, flexible panel for instance of plywood, which is brought to vibrate driven by the sound field in the room.
  • the mass and stiffness of the panel together with the compliance of the air volume defined by the frame, the panel and the boundary behind the panel will determine the resonance frequency of the absorber and the internal losses will determine the Q value of the resonator and hence its bandwidth.
  • acoustic damping material such as mineral wool may be introduced into the cavity within the frame.
  • the resonance frequency may be changed by changing the depth of the resonator and maintaining the circumferential dimensions of the frame. A deeper absorber thus provides a lower resonance frequency.
  • Low-frequency sound absorption can furthermore be attained using a so-called Helmholz resonator basically consisting of one or more passages or tubes of a given length and cross sectional area, these one or more passages representing an acoustic mass, where one longitudinal end of one or more passages is/are coupled to the sound field in the room and the other end is coupled to a cavity of a given volume representing an acoustic compliance essentially proportional with the volume of the cavity.
  • the particular combination of mass and compliance determines the resonance frequency of the Helmholz resonator and the internal losses determine the Q value or effective bandwidth of the Helmholz resonator.
  • the input impedance of the resonator will be very low and the resonator will hence absorb sound energy from the surrounding sound field selectively in a frequency region around the resonance frequency.
  • damping material such as mineral wool may be introduced in the Helmholz resonator to alter the Q value hereof.
  • Helmholz resonators are often of a form somewhat resembling the above mentioned panel resonators, where the thin, flexible panel have been replaced by a thicker, rigid panel provided with a pattern of passages through the panel.
  • Helmholz resonators comprising a single passage or tube and a cavity have also been used for changing the reverberation time and/or suppression of undesired low-frequency room modes.
  • a membrane absorber typically consists of a light plate in front of a closed cavity. Often the cavity is filled with a porous material, which provides damping for the system.
  • the walls and back of the cavity are assumed to be rigid and the bending stiffness in the plate is assumed to be negligible compared to the stiffness of the air column in the cavity.
  • the system is characterized by the mass per unit area of the plate, m, the depth of the cavity, d, and the internal losses of the system, ⁇ , consisting of the losses due to the flow resistance of the porous material, internal losses in the plate and losses in the joints along the edges of the plate, p is the density of air or other gas in the cavity and c is the speed of sound.
  • the acoustic impedance of the system can be shown to be:
  • the resonance frequency is inversely proportional to the square root of both the mass of the membrane and the depth of the cavity.
  • the membrane in order to obtain a maximum absorption at around 63 Hz, with a cavity depth of 0.2 m, the membrane must have a mass of about 5 kg/m 2 . But by pressurizing the cavity, the stiffness of the system grows and it may be possible to apply a less heavy material.
  • the impedance of the absorber can be tuned in order to maximize the absorption at the resonance frequency and the usable bandwidth of the absorber (half-power bandwidth, B). If the impedance is too high, relative to the radiation resistance of the membrane, r s , the incident sound field will reflect off of the membrane and not be absorbed. If the impedance is too low, then the internal losses will be too small and not enough sound energy will be absorbed.
  • the impedance ratio of the internal losses and the external radiation resistance can be expressed as:
  • the absorbing device be of substantially the same depth d throughout the device.
  • the depth d changing in a characteristic and predetermined manner over the surface of the absorbing device.
  • the above expressions may be reformulated in terms of the actual air or gas volumes and the corresponding compliances as is known within the field of acoustics.
  • the absorption coefficients of the test specimen can be calculated from the measured reverberation time of the empty reverberation chamber and the reverberation chamber with test specimen present as follows:
  • V is the volume of the reverberation chamber
  • S 5 is the area of the test specimen
  • T ⁇ 0 is the reverberation time in the chamber with the specimen present
  • T 60 is the reverberation time of the empty chamber.
  • the sound absorption characteristics of the above prior art absorbers can not readily be altered once the absorber has been constructed. Specifically major changes of the absorption coefficient ⁇ and/or the resonance frequency can not be accomplished by minor modifications of a given absorber. Also the absorption coefficient can not be changed systematically in a simple manner, such changes comprising for instance a shift between a very high absorption coefficient and a very low absorption coefficient, i.e. essentially an on/off function of the absorber.
  • absorbers are rather bulky structures that will be difficult - or occasionally even impossible - to remove from a given room once installed. They are to be regarded as fixed installations in the particular room and not installations that can readily be dismantled from a given room, transported to another room and used here. Even though dismantling and transport to another room may be possible, great costs would be incurred by the transport due to the bulky nature of such absorbers.
  • an essentially on/off function of the absorbing device i.e. a change between a very high absorption coefficient and a very low absorption coefficient within a certain specified frequency region would be desirable.
  • a sound-absorbing device for placement in a sound field in air, and absorbing acoustic energy from said sound field in a predetermined frequency region, specifically, although not exclusively, a low-frequency region
  • the device comprising an at least partly flexible body containing one or more cavities, where at least a portion of the outer surface of the body is in contact with said sound field and where said body is inflatable and collapsible by supplying a gas to or removing the gas from said at least one cavity, respectively, whereby the absorption coefficient a and the resonance frequency of said body can be varied, thus determining the frequency region in which maximum absorption will take place.
  • the desired altering of the reverberation time of a given room may be accomplished by using a single device as described above - depending for instance on the dimensions of the room, the dimensions of the absorbing device and the various acoustical properties of the device, but in many instances a plurality of such devices will advantageously be used to form a system covering sufficiently large and predetermined areas of the room. Many configurations of such systems are conceivable, and some embodiments hereof will be described in the detailed description of the invention.
  • a system for reducing the reverberation time of a room comprises according to the present invention a plurality of sound-absorbing devices of the basic configuration described above, where the system furthermore comprises conduits through which gas can be supplied from a source to each of said bodies and removed from these.
  • the said bodies could either each be provided with valve means for controlling the supply of gas to/removal of gas from each of said bodies separately, or all the bodies of the system - or groups of bodies in the system - could also alternatively be provided with common valve means.
  • valve means could be remote controllable and the system could be provided with a central control device for controlling the static pressure in each of the bodies and hence the compliance or dimensions of each of the bodies separately.
  • the tension of the material of the bodies could be monitored by for instance piezo-electric devices or the dimensions and shape of the bodies could also be supervised by other means.
  • the system could furthermore be provided with means for measuring the reverberation time of a room in which the system is installed, thereby facilitating the appropriate set-up of the system.
  • Such means could of course also be provided in connection with only a single device according to the invention.
  • the system could comprise data storage means for storing measured reverberation times and corresponding parameter settings of the device or system for later analysis and retrieval, thereby facilitating empirical improvements of the parameter choices (overall absorption area of the devices, required inflation, optimal material characteristics, etc.) of the device or system.
  • the bodies of the device according to the invention can according to the invention be provided with self-inflatable means in the manner of self-inflatable air mattresses, an alternative which will be briefly described in the detailed description of the invention.
  • the present invention furthermore relates to a method for reducing the reverberation time of a room at least in a low-frequency region from a given reverberation time (T 6 o) to a desired reverberation time (T 60 ,s) comprising the introduction of one or more bodies according to any of the preceding claims 1 to 7 into the room, where the required total surface area S s of said one or more bodies is determined by the equation
  • ⁇ is the absorption coefficient
  • V is the volume of the room
  • c is the speed of sound.
  • the device, system and method is designed specifically for altering the reverberation time in the frequency region of approximately 63 - 125 Hz with a maximum absorption coefficient of at least 0.7 and a usable bandwidth of at least one octave, i.e. in the frequency region where many rooms exhibit an unacceptable high reverberation time as described initially in connection with figure 1.
  • the device according to the invention could furthermore be provided with absorbing devices effective at higher frequencies.
  • the high-frequency absorbers could for instance be provided as a thin sheet of a suitable fabric of a sufficiently high flow resistance to yield it effective as an acoustic absorber at higher frequencies.
  • figure 1 shows actual measurements of the reverberation time T30 in seven different rooms which can be used for live performances of music as well as reproduction of sound:
  • figure 2 shows a schematic representation of a first embodiment of a device according to the invention comprising a substantially rigid frame structure covered by a thin, flexible membrane;
  • figure 3 shows the absorption coefficient ( ⁇ ) as a function of frequency of a device according to the invention of the kind shown in figure 2.
  • FIGS. 4a, 4b and 4c show a schematic representation of two versions of a second embodiment of a device according to the invention of a "mattress" configuration
  • figure 5 shows a schematic representation of a third embodiment of a device according to the invention comprising an inflatable frame structure for suspension of at least one flexible membrane
  • figure 6 shows a schematic representation of a fourth embodiment of a device according to the invention, which is an alternative to the one shown in figure 5;
  • figure 7 shows a schematic representation of a fifth embodiment of a device according to the invention of an "ice bag” structure
  • figure 8a shows a schematic perspective exploded view of a sixth embodiment of a device according to the invention.
  • figure 8b shows a plane view and a cross-sectional view of the embodiment shown in figure 8a;
  • figure 8c shows a schematic perspective view of a system of devices according to the invention assembled to form a system for altering the reverberation time of a room;
  • figure 9a shows a schematic perspective view of a seventh embodiment of a device according to the invention mounted on a boundary of a room and provided with both low-frequency and high-frequency absorbing members;
  • FIGS 9b, 9c and 9d show schematic perspective views of the embodiment of the invention shown in figure 9a in three different conditions
  • FIGS 10a, 10b and 10c show schematic perspective views of an actual implementation of the seventh embodiment of the invention.
  • figure 11 shows a computer simulation of an installation of a system according to the present invention in a concert hall.
  • FIG 2 there is now shown a schematic representation of a first embodiment of a device according to the invention comprising a substantially rigid frame structure 1 comprising edge portions 1" surrounding a central portion 1', thus forming an open box- or tray-like support structure. Opposite the central portion 1' and supported by the edge portions 1" is suspended a thin, flexible membrane 2.
  • the frame structure and the membrane define an internal cavity 4 which can be inflated/deflated with air or another suitable gas via a conduit and valve arrangement indicated by reference numeral 10.
  • the cavity 4 may optionally be provided with a certain amount of acoustic damping material, for instance in the form of a panel 3 of porous material provided at the central portion 1 1 or in the form of a suspended sheet of fabric with suitable flow resistance, suspended between the edge portions 1" at a suitable distance from the central portion 1'.
  • acoustic energy of an incident sound field as schematically indicated by S in figure 2 will be absorbed by the device, partly due to internal friction in the flexible membrane 2 and provided an acoustic absorbent material is introduced into the cavity 4, partly by friction and thus generation of heat in this material.
  • Figure 3 shows actual measurements of the absorption coefficient ( ⁇ ) as a function of frequency of a device according to the invention of the kind shown in figure 2 and provided with an absorbing panel 3 as described above.
  • an absorption coefficient of close to 0.8 i.e. approximately 80% of the sound energy incident on the membrane is absorbed by the device, is reached at a frequency of 63 Hz and fairly high absorption coefficients are attained in a frequency range of approximately 1 octave around this frequency.
  • Due to the presence of the absorbing material 3 in the cavity 4 of the device a relatively high absorption coefficient of approximately 0.6 is still attained in the deflated ("vacuum") state although at a higher frequency due to the reduced compliance (i.e.
  • the membrane which is not resting on the surface of the absorption material 3.
  • absorption of acoustic energy can thus be attained at and around two different frequencies, i.e. the reverberation time of the room in which the device is installed can be altered at two different frequencies according to the state of the device. If the absorbing panel 3 had not been provided in the cavity 4, significant absorption would still have been attained at and around the frequency 63 Hz, but essentially no absorption would have been attained in the deflated state, thus yielding an on/off device for altering reverberation time.
  • the device shown in figure 3 comprises the above-mentioned substantially rigid frame structure, which could for instance be made of plywood or a moulded plastic material, but for many applications it will be beneficial at least to a large extent to avoid rigid structures in the devices according to the invention, thereby facilitating transport and storage of these devices. This becomes particularly important for mobile applications where a plurality of such devices are to be moved from one location to another and temporarily set up to form a system covering larger areas of a room. For such applications it is desirable if the device according to the invention can be practically completely collapsed and if relatively heavy support structures can furthermore be avoided.
  • the embodiments of the device according to the invention shown in figures 4, 5, 6 and 7 are all of this collapsible type.
  • figures 4a, 4b and 4c show a schematic representation of different versions of a second embodiment of a device according to the invention of a "mattress" configuration.
  • the device may have the rectangular shape of a traditional mattress comprising upper and lower (not visible) substantially planar surfaces 5 bounded by edge portions T 1 7", thus forming an internal cavity in the mattress.
  • Both the planar portions 5 and the edge portions 7', 7" are made of a suitable flexible material whereby the mattress can be brought into an inflated state as shown in figure 4a by the provision of air or other gas under pressure via an inlet 10 with suitable valve means.
  • cross connections 6 are provided internally between the two opposing planar surfaces 5, as is well known in itself.
  • Figures 4b and 4c show two cross sectional views of two different versions of the mattress embodiment of the invention.
  • the version shown in figure 4b comprises flexible surfaces 5 on either opposing side of the mattress and is provided with the cross connections 6 and the flexible edge portions 7".
  • Devices of this type could for instance be hung from the ceiling or from other support structures, thus providing access for the incident sound field on either of the opposing substantially planar surfaces of the device.
  • the device shown in figure 4c comprises only one flexible surface 5, whereas the opposing planar side of the "mattress" structure consists of a substantially rigid panel 44. This panel may extend beyond the edge portions 7" as indicated by reference numeral 45, thus providing flange-like edge portions facilitating attachment of the device to for instance a ceiling or a wall.
  • Figure 5 shows a schematic representation of a third embodiment of a device according to the invention of the collapsible type comprising an inflatable frame structure 8', 8" for suspension of at least one flexible membrane 9, although one of these may also be a substantially rigid panel as in the previous embodiment.
  • the frame structure may be provided by the hollow toroidal structure 8' and 8" shown in figure 5 and inflated with air at a pressure P 1 above atmospheric pressure via the inlet and valve member 11 in order to attain a relatively rigid frame structure. Suspended over this frame structure is either one or two flexible membranes 9, whereby a cavity 12 is formed between the membranes.
  • the cavity 12 can be varied (inflated/deflated) by controlling the pressure p 2 of air or other gas within the cavity, the cavity being also provided with inlet and valve means 10.
  • other shapes than the cylindrical shape shown may of course be envisaged without departing from the invention, as exemplified by the embodiment shown in figure 6 comprising inflatable edge portions 15', 15" forming an inflatable rectangular frame structure over which flexible membranes (or one membrane and a substantially rigid panel) 13, 14 can be suspended.
  • Separate inlet and valve members 16, 17 are also present in this embodiment for controlling the pressure in the respective cavities.
  • FIG. 7 shows a schematic representation of an embodiment of a device according to the invention of an "ice bag” structure somewhat resembling the mattress structure shown in figures 4a, 4b and 4c.
  • the device is generally indicated by reference numeral 18 and comprises a body of a mattress-like structure subdivided into a plurality of portions 20, 20', which portions may be of identical shape and dimensions, although this is not a requirement, the individual portions being bounded by a bracing structure 19.
  • the individual portions, each defining an internal cavity 21 may be in fluid connection with each other or a given portion may be in fluid connection with certain other adjacent portions, whereby air or other gas used for inflating the device can be provided at a given inlet and valve member and flow to the other of the said portions.
  • partitions 22 between adjacent portions and thereby subdividing the device into a number of sections, for instance the rows or columns of the matrix-like structure shown in figure 7.
  • Each of these sections is then provided with separate inlet and valve members 10 for inflating/deflating the portions of the particular section.
  • figure 8 there is shown a sixth embodiment of a device according to the invention.
  • figure 8a shows a schematic perspective exploded view of this embodiment comprising opposing membranes 25 and 26 suspended between opposing substantially linear longitudinal edge portions 29 of a spilt-up cylindrical configuration provided with a slit 35 through which the membranes 25, 26 can be introduced into the edge portions and afterwards attached to the edge portions (and to each other) in an airtight manner, thus defining an internal cavity between the membranes and opposing end portions 27, the end portions being also secured to the membranes and the edge portions in an airtight manner.
  • the end portions 27 could be made of a single sheet of a suitable flexible material but it would also be possible to form the end portions 27 as inflatable bodies in order to increase the rigidity (moment of inertia) about the relevant plane and thereby also prevent a cylindrical configuration in the inflated state of the device.
  • One or more intermediate shape retainment members 28 may be provided at appropriate locations within the internal cavity in order to attain the desired shape of the device in its inflated and deflated states.
  • the shape retainment members 28 are provided with suitable passages 36 to allow passage of air or other gas between the various compartments formed within the device by the introduction of the members 28.
  • the longitudinal edge portions 29 can accommodate correspondingly shaped (i.e.
  • figure 8c shows a part of a system of devices according to this embodiment of the invention, where individual vertical columns of devices are hung for instance from a ceiling or other support structure, each of the devices being connected to the adjacent devices by connecting members 37 formed for releasable engagement with the rods 32 through the recesses 31 in the edge portions described above.
  • Air or other suitable gas is provided to the devices from an external source via a hose or pipeline 34 at the outermost column of devices as shown in figure 8c and between devices of adjacent columns via short hoses or pipelines 38. It is understood that other patterns of fluid interconnections between the various devices can be envisaged without deviating from the system of devices according to the invention.
  • valve means to control the flow of air or other gas into and out of the devices.
  • each individual device with its separate valve means and thereby be able to control the inflation of each individual device separately.
  • the valves may be manually operated but remote controllable valves, controlled for instance by a central control system as mentioned in the following, could also be envisaged.
  • FIG 9 a schematic perspective view of a seventh embodiment of a device according to the invention mounted on a boundary 40 of a room and provided with both low-frequency and high-frequency absorbing members 42 and 46, respectively, whereby the reverberation time of the room may not only be altered at low frequencies but also at higher frequencies.
  • the device according to this embodiment is shown and described mounted on a boundary, it may alternatively be designed for free suspension for instance from a ceiling, in which case a high-frequency absorbing device (fabric etc.) 46 may be provided on either side of a central low-frequency absorbing device 42.
  • a device according to the invention comprising a low-frequency absorbing device 42 according to the invention, for instance a device of the "mattress" design or “ice-bag” design described previously in connection with figures 4a, 4b and 7, respectively, and a high-frequency absorbing device 46, for instance a suitable fabric.
  • the low-frequency absorbing device 42 is wound around a drum 43, the drum being mounted for rotation around its longitudinal axis in a supporting/suspension structure or bracket 41 and driven by a motor 45 through a belt 44 or other equivalent means.
  • the motor may be remote-controlled for instance from a central control system, which may also control and supervise other functions of the device or system of devices.
  • the high-frequency absorbing device 46 is in this embodiment wound around a drum 47 and guided over a suitable roller 48 to a drawn out position substantially in parallel with the low-frequency absorbing device.
  • the motor drives both absorbing devices 42 and 46, but it would also be possible to provide separate drives for each of these devices, whereby one of these could be brought into its active, drawn out position with the other remaining inactive.
  • the absorbing devices may also be operated manually if desired.
  • the absorbing devices 42 and 46 are provided with bottom rails 49 and 50, respectively, where the bottom rail 50 of the high-frequency absorbing device mainly serves to provide the necessary weight to the lower end of this device to make it extend downward in a substantively planar fashion, parallel with the low-frequency absorbing device.
  • the low-frequency absorbing device 42 will generally be much heavier than the high-frequency absorbing device 46, and the bottom rail 49 of the low-frequency absorbing device 42 can be used primarily for providing a fixed attachment to a bottom support 51 mounted on the wall 46 and for the provision of the inlet and valve member 52 through which air or other gas is supplied to/withdrawn from the device 42.
  • the bottom support 51 may be provided with means for establishing fluid connection between the inlet and valve member 52 and a source, although the device 42 may also be supplied with air or gas by other means.
  • the valve may also be provided in the bottom support 51 in stead of in the inlet 52 to the device 42.
  • Figures 9b, 9c and 9d show three different states of this embodiment of the invention, i.e. (b) essentially inactive, (c) high-frequency absorbing device active but low-frequency absorbing device inactive, as it has not yet been inflated and (d) both devices active.
  • FIGS 9a through 9d show a device comprising both a low-frequency absorbing part 42 and a high-frequency absorbing part 46, it is emphasised that supporting/suspension structure 41 could also be formed for only comprising the low-frequency absorbing device 42 in cases where no modifications of high- frequency reverberation time are needed. Also the structure 41 may be formed for comprising a high-frequency absorbing device 46 on either side (front and rear) of the low-frequency device 42.
  • the inflatable low-frequency absorbing devices may comprise one or more internal cavities without acoustic damping material provided in the cavities. In these cases the absorbing effect is due primarily to internal friction in the membranes themselves. It is, however, also possible to provide acoustic damping material within the cavities, which material could for instance be a panel of porous material such as mineral wool, etc. or a thin sheet of fabric, etc., with a sufficiently high acoustic flow resistance.
  • Such systems could for instance comprise a matrix structure of absorbing devices with a given number of rows and columns, the individual devices being connected in a chosen manner by pipelines providing the air/gas for inflating the absorbing devices to the degree necessary to attain the required resonance frequency and absorption coefficient as described previously and for the supply of air/gas the inflatable frame portions described in connection with some of the embodiments.
  • Each individual absorbing device may be provided with its own valve means as described, or valve means may be provided for certain groups of devices.
  • the valve means may be remote controllable (infrared, Bluetooth etc.) for instance from a central control console, from which the inflation/deflation of the devices may be controlled.
  • the system may comprise sensors for measuring the pressure of the devices, thereby providing for the possibility to supervise the correct functioning of the system from the control console.
  • the system may comprise means for measuring the reverberation time of the room, for instance before and after inflation of the absorbing devices. It is even possible using a system of absorbing devices according to the invention to tune the devices to different resonance frequencies, for instance to attain a broader effective frequency region for altering the reverberation time of the room.
  • the absorbing devices could be tuned to resonance frequencies of 63 Hz or 125 Hz, but this is only to be regarded as typical resonance frequencies.
  • a system could comprise for instance one hundred absorbing devices according to the invention and be controllable from a dedicated control console.
  • control and supervision could take place from a portable personal computer provided with appropriate software to be delivered with the system.
  • This software could provide for the possibility to measure the reverberation time as described above and furthermore comprise an algorithm which - based on entered physical dimensions of the room and the expected number of listeners - could calculate the total number of absorbing devices necessary in order to attain optimal reverberation time.
  • previous data for instance pre and post reverberation times of other rooms in which the system has been used) could be stored in appropriate data storage means for later analysis and retrieval.
  • an alternative embodiment of the device according to the invention comprising means for self-inflation (or self- extension) of the air or gas-filled bodies of the devices would also fall within the scope of the present invention.
  • This embodiment would correspond somewhat to the self-inflating mattresses used for instance for camping etc. and could comprise an outer air of gas impermeable envelope internally provided with for instance a sponge rubber structure facilitating the extension of the device to its proper depth/dimensions, when it is not prevented from such extension.
  • This embodiment of an absorbing device could thus for instance form part of the device described above as the seventh embodiment although it may also be used in many other connections.
  • any valve means in the supply lines to the bodies may be left open during operation of the devices, assemblies and systems according to the invention.
  • FIG 10a there is shown a practical design of the supporting/suspension structure 41 of the seventh embodiment of the invention described above.
  • This structure is according to the shown implementation formed as a housing 55 accommodating the rollers for the low- and high-frequency absorbing devices such that these devices - or one of these - may be housed partially or completely within the housing.
  • the provision of the housing may serve both as a general protective means for the devices, when these are not in use and also as a fire protection means.
  • the assembly or system may be provided with means for detecting fire/smoke, which means will activate the drive mechanism in the assembly and thereby retract either one or both of the absorbing devices 42, 46 into the housing.
  • the housing may be provided with an upper portion 55 pivotally connected to the main body of the housing 54 such that the upper portion 55 will automatically rotate to the closed state of the housing shown to the left of figure 10b in case of fire.
  • the housing may of course also be closed by the upper portion 55 as a general protective measure for the absorbers accommodated by the housing.
  • FIG 11 there is finally as an illustrative example shown a computer simulation of a system of sound-absorbing assemblies according to the invention suspended along one boundary of a concert hall for altering the reverberation time of the hall.
  • the inflatable/extendable and collapsible/compressible bodies according to the invention must be able to absorb acoustic energy from a surrounding sound field.
  • this ability relates to the impedance ratio of the internal losses of the flexible material of the absorptive bodies and the external radiation resistance of the absorptive bodies.
  • Rianyl ® which is a PVC material with a density of 2,96 kg/m 2 , has been applied.

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  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
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  • Building Environments (AREA)
  • Soundproofing, Sound Blocking, And Sound Damping (AREA)

Abstract

L'invention concerne des dispositifs, des ensembles et des systèmes d'absorption de son, ainsi que des méthodes correspondantes, pour modifier le temps de réverbération d'une pièce, et ce spécifiquement bien que non exclusivement nécessairement dans les basses fréquences. Un dispositif d'absorption de son selon l'invention comprend, fondamentalement, un corps présentant une ou plusieurs cavités (4), au moins une partie de la surface extérieure au corps étant en contact avec ledit champ sonore S et ledit corps étant gonflable/extensible ou contractile/compressible pendant l'apport de gaz ou l'évacuation du gaz de ladite ou desdites cavités (4), respectivement, le coefficient d'absorption (a) et/ou la fréquence de résonance dudit corps pouvant être modifiés, déterminant ainsi le coefficient d'absorption et/ou la plage de fréquences pour lesquels l'absorption maximale se produira.
PCT/DK2005/000322 2004-08-06 2005-05-13 Methode, dispositif et systeme pour modifier le temps de reverberation d'une piece WO2006119763A1 (fr)

Priority Applications (9)

Application Number Priority Date Filing Date Title
JP2008510408A JP4782193B2 (ja) 2005-05-13 2005-05-13 空間の残響時間を変更する方法、装置、及びシステム
PCT/DK2005/000322 WO2006119763A1 (fr) 2005-05-13 2005-05-13 Methode, dispositif et systeme pour modifier le temps de reverberation d'une piece
PCT/IB2005/052580 WO2006016321A2 (fr) 2004-08-06 2005-08-02 Procede, dispositif et systeme permettant de modifier le temps de reverberation d'une piece
ES05773193T ES2400912T3 (es) 2004-08-06 2005-08-02 Método, dispositivo y sistema para modificar el tiempo de reverberación de una sala
PL05773193T PL1779375T3 (pl) 2004-08-06 2005-08-02 Sposób, urządzenie i system do zmieniania czasu pogłosu pomieszczenia
PT57731937T PT1779375E (pt) 2004-08-06 2005-08-02 Método, dispositivo e sistema para a alteração do tempo de repercussão de uma sala
US10/587,898 US7905323B2 (en) 2004-08-06 2005-08-02 Method, device and system for altering the reverberation time of a room
SI200531676T SI1779375T1 (sl) 2004-08-06 2005-08-02 Postopek, naprava in sistem za spreminjanje odmevnega äśasa v prostoru
EP05773193A EP1779375B1 (fr) 2004-08-06 2005-08-02 Procede, dispositif et systeme permettant de modifier le temps de reverberation d'une piece

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
PCT/DK2005/000322 WO2006119763A1 (fr) 2005-05-13 2005-05-13 Methode, dispositif et systeme pour modifier le temps de reverberation d'une piece

Publications (1)

Publication Number Publication Date
WO2006119763A1 true WO2006119763A1 (fr) 2006-11-16

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PCT/DK2005/000322 WO2006119763A1 (fr) 2004-08-06 2005-05-13 Methode, dispositif et systeme pour modifier le temps de reverberation d'une piece

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WO (1) WO2006119763A1 (fr)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009130685A1 (fr) * 2008-04-24 2009-10-29 Flexacoustics Aps Dispositif et système d'absorption de son
US11610572B2 (en) 2016-02-10 2023-03-21 James G. Pilaar Enhanced inflatable sound attenuation system

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5672801B2 (ja) * 2010-07-02 2015-02-18 横浜ゴム株式会社 水中用遮音装置
KR102109790B1 (ko) 2019-09-11 2020-05-13 음향컨설팅그룹라라(주) 잔향 가변 장치, 방법 및 시스템
KR20210031351A (ko) 2020-02-13 2021-03-19 주식회사 엘티에스 잔향 가변 시스템
KR20210153255A (ko) 2020-06-10 2021-12-17 주식회사 엘티에스 다목적 공간의 잔향 가변을 위한 장치, 방법 및 시스템
KR20210153257A (ko) 2020-06-10 2021-12-17 주식회사 엘티에스 전기 활성화 폴리머를 이용한 잔향 가변 장치, 방법 및 시스템
KR20220078239A (ko) 2020-12-03 2022-06-10 주식회사 엘티에스 아코디언 또는 자바라 형태를 기반으로 한 잔향 가변 장치, 방법 및 시스템

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2615549A1 (fr) * 1987-05-20 1988-11-25 Caire Claude Const Metalliq Ca Plafond acoustique pour salle de spectacle
US5299522A (en) * 1993-03-09 1994-04-05 Dixon Jr Henry R Inflatable acoustic buffer for boat hulls
US6332027B1 (en) * 1996-06-28 2001-12-18 Bertin & Cie Noise-absorption structures and walls constituted thereby
EP1353025A1 (fr) * 2002-04-12 2003-10-15 Benedict George Morris Elémentes de batiment
WO2004106663A1 (fr) * 2003-05-28 2004-12-09 Art Andersen A/S Systeme de recouvrement souple et modules correspondants pour parois, plafonds et autres elements de limite

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2615549A1 (fr) * 1987-05-20 1988-11-25 Caire Claude Const Metalliq Ca Plafond acoustique pour salle de spectacle
US5299522A (en) * 1993-03-09 1994-04-05 Dixon Jr Henry R Inflatable acoustic buffer for boat hulls
US6332027B1 (en) * 1996-06-28 2001-12-18 Bertin & Cie Noise-absorption structures and walls constituted thereby
EP1353025A1 (fr) * 2002-04-12 2003-10-15 Benedict George Morris Elémentes de batiment
WO2004106663A1 (fr) * 2003-05-28 2004-12-09 Art Andersen A/S Systeme de recouvrement souple et modules correspondants pour parois, plafonds et autres elements de limite

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009130685A1 (fr) * 2008-04-24 2009-10-29 Flexacoustics Aps Dispositif et système d'absorption de son
US11610572B2 (en) 2016-02-10 2023-03-21 James G. Pilaar Enhanced inflatable sound attenuation system

Also Published As

Publication number Publication date
JP4782193B2 (ja) 2011-09-28
JP2008545900A (ja) 2008-12-18

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