WO2002023099A1

WO2002023099A1 - Sound absorbent

Info

Publication number: WO2002023099A1
Application number: PCT/SE2001/001982
Authority: WO
Inventors: Mats ÅBOM; Claes-Göran Johansson
Original assignee: Fläkt Woods AB
Priority date: 2000-09-18
Filing date: 2001-09-17
Publication date: 2002-03-21
Also published as: NO321542B1; NO20031212L; US20040099477A1; EP1319156A1; DE60118221D1; DE60118221T2; ATE321248T1; AU2001288177A1; NO20031212D0; SE0003349D0; EP1319156B1

Abstract

A light absorbent for hygienic spaces comprising a porous mat. The normalized flow resistance of the mat is in the interval of 0.5-2.

Description

Sound absorbent

TECHNICAL FIELD

The present invention relates to an absorbent for a dissi- pative absorption of sound. In particular, the invention relates to a sound attenuator incorporating the absorbent and to a method for sound reduction in a system for transport of a gaseous medium. In a first application of the invention, such a transport system comprises a ventilation system. In a second application, the gas transport system comprises an exhaust gas system and in particular an exhaust gas system for an internal-combustion engine, for example in a ship. In both applications, the device and the method relate to a channel, from the wall or outlet of which noise is generated, which may be subjected to acoustic requirements. However, the invention is also advantageously applicable to other elongated gas transport systems, such as in exhaust gas plants in, for example, vehicles with internal-combustion engines or in flue-gas cleaning devices for plants for, for example, production of electric power.

BACKGROUND ART

By sound is meant a physical phenomenon which gives rise to hearing sensations. Usually, sound is regarded as a wave motion in a gaseous medium. Sound may, however, also be transported in other media, such as fluids and solid materials. In air, the sound propagates as a longitudinal wave motion at a velocity of about 340 m/s. However, the velocity is dependent on the temperature of the medium. The audible sound comprises frequencies from about 20 Hz to about 20,000 Hz. The wavelength of the audible sound in air with a normal temperature thus varies from the order of magnitude of 3 m at low frequencies (-100 Hz) , 30 cm for sound at intermediate frequencies (-1000 Hz) , and 3 cm for sound at high frequencies (-10,000 Hz). In addition, the sound may vary greatly with both amplitude (sound intensity) and time.

In a traditional absorbent, sound energy is transformed into heat by flow resistance of the absorbent. Such an absorbent substantially exhibits resistive attenuation. Other words for this are dissipative or viscous attenuation. The ratio of the thickness of the absorbent to the length of the sound waves which are included in the sound has proved to be decisive for the attenuation at lower frequencies in such a traditional absorbent. A satisfactory attenuation is attained at these absorbents for sound frequencies at which the thickness of the absorbent is larger than a quarter of a wavelength of the sound. The sound attenuating properties then decrease drastically for sound with lower frequencies, which has a larger wavelength. Even at a ratio of wavelength to absorbent thickness of about 1/8, the absorption is only half as great, and at a ratio of 1/16 it is only 20 % of the absorption which is obtained at a ratio of % . Since a certain absorption capacity still remains, in many cases a satisfactory absorption may be obtained by increasing the surface of the total absorbent.

Well-known materials for the manufacture of a resistive absorbent are mineral wool and glass wool. Usually, the wool is retained by an adhesive which causes a homogeneous structure in the absorbent. Under normal conditions, such an absorbent is very good from several points of view. In environments with hygienic requirements, however, these absorbents are less suited since bacteria may develop in the absorbent fibres may loosen. A common requirement in such hygienic environments is that an absorbent shall be capable of being flushed. In this context, the known absorbent has proved to be less resistant and may retain moisture for a long period of time. After repeated flushing, the absorbent is gradually dissolved. The known wool is built up of brittle fibres, in which case a less good mechanical strength is obtained in the absorbent. In case of heavy vibrations, the structure is decomposed in course of time.

A large number of porous absorbents are available on the market and their sound-absorbing properties are known by measurements. Usually, the porous absorbents are characterized by thickness and density. One problem in the manufacture of circular attenuators for, for example, ventilation systems is that the absorbent, which is usually made flat, must be bent to fit into the attenuator. Depending on the original thickness of the absorbent, it will have a varying density in the circular design. On the inside of the sound attenuator, the density will be high and tendencies to folding will arise. On the outside, cracks will sometimes arise as a result of the hard bending.

In environments with high gas velocities, the known absorbent is also less good. A surface-wiping gas tears with it fibres and particles from the absorbent. Successively, these end up in channels and spaces where they have a negative influence on the environment. The torn-off particles also result in the absorbent being gradually worn down and, in the end, disappearing entirely. In these contexts, it is known to coat the absorbent with a more stable layer, for example of thin plastic or a- perforated sheet. These coatings involve extra operations during manufacture and thereby tend to increase the cost.

For the purpose of reducing the sound emitted from, for example, the orifice of a ventilation system or an exhaust gas system, it is known to arrange one or more sound attenuators in the gas channel of the system. The designation sound attenuator here means a device which is capable of consuming sound energy. This may occur by transforming the sound energy into some other form of energy, such as, for example, heat. In the following text, the designation resistive attenuator refers to a device which is capable of absorbing sound in a gas channel, that is, to transform the sound energy into another form of energy. The designation attenuator, in the following text, means a device which is capable of reducing sound, and attenuation means the property of reducing sound.

One typical embodiment of a resistive attenuator is a circular or square tube, the sides of which, exposed to the gas flow, are coated with an absorbent or a porous medium of small coupled cavities . A common such sound attenuator intended for a ventilation system is described in the patent document GB 2,122,256. From the patent document US 2,826,261, another resistive attenuator intended for an exhaust system is previously known. As absorbent there is used a resistive absorbent of the type described above. The absorbent may also be protected by an air-permeable surface layer, for example a perforated sheet, to attain a longer service life and better mechanical stability at high gas speeds. Such a resistive attenuator will have a sound-attenuating property which covers a wide frequency range. The attenuation is also dependent on the thickness and flow resistance of the absorbent, the exposed absorbent surface, any surface protection such as, for example, a perforated sheet and the dimen- sions of the attenuator, such as the length and the diameter thereof .

One problem with the traditional resistive attenuator is thus that the absorbing layer must be made very thick to be able to attenuate low frequencies. This entails a large space for housing the attenuator. Another problem is that a traditional resistive sound attenuator gives rise to a pressure drop across the attenuator itself. This results in an increased resistance to driving the gas through the system. To compen- sator for this pressure increase, the cross-section area of the channels in the system is often increased. In that con- text, it is known that the absorption decreases in the upper frequency register of the sound. In certain cases, this is compensated for by arranging a sound absorbent in a central body in the sound attenuator. This again results in the pressure drop across the attenuator increasing. The sound- attenuating properties are also dependent on where in the system the sound attenuator is placed. It often turns out that the properties which are achieved in a laboratory, especially at low frequencies, and which are described in pamphlets, are seldom achieved in practice. This often leads to oversizing in order to attain a desired sound attenuation with sufficient certainty.

Another known way of reducing the sound emission from a gas transport system is to prevent the sound from propagating in the channel. This may be achieved by arranging a reflecting obstacle in the gas channel. Such an obstacle is obtained by creating a sound which is in opposition to the sound in the channel, thus achieving extinction. One such technique is active sound attenuation. In connection with active sound attenuation, a sound is added which is directed in a direction opposite to the sound progressing in a channel. This oppositely directed. sound is then created by a loudspeaker placed in the channel. However, controllable conditions are required for an active system to function well.

Still another known way of reducing the sound emission from a gas transport system is to arrange a passive obstacle to an acoustic wave progressing in a channel. This type of sound attenuator actually consumes no energy and is usually referred to as a reactive attenuator. A reactive attenuator substantially operates according to two principles. The first type is a reflection attenuator. This comprises an increase of the cross-section area, whereby the area increase gives rise to a reflection wave which propagates in a direction opposite to the propagation of the sound. The function is a broadband function. The second type is a resonance attenuator. Here, the function is a narrow-band function and may almost be regarded as a filter which eliminates pure tones from the sound. To obtain maximum attenuating effect, the orifice of a resonance attenuator must be placed in a pressure maximum of the sound field in the channel. The resonance attenuator is thus very sensitive to the position in the channel .

There are also a large number of devices which in various ways combine the methods mentioned above. However, the problem is usually that the various components end up in locations where they are not effective. To compensate for the unforeseeable properties, conventional sound attenuator systems are therefore often greatly oversized, which leads to expensive, heavy and space-demanding plants with high pressure drops .

Sound attenuator devices in transport systems for gas, where the gas changes temperature, implies further complications since the wavelength of the sound is changed with the temperature. If, for example, the temperature of the gas is increased from 20°C to 900°C, the sound velocity and hence the wavelength increase twofold. An attenuator which operates well at normal temperature therefore suffers deteriorated properties, especially at low frequencies when the gas is heated. This usually results in sound attenuating devices in transport systems with hot gases becoming very bulky.

SUMMARY OF THE INVENTION

The object of the present invention is to suggest ways and means of achieving an absorbent which has good absorbing properties within a wide frequency range and which is inex- pensive to manufacture. It shall be less space-demanding than prior art absorbents and be applicable to environments L J t t

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material which is resistant to deformation, such as plastic. The inventive concept also comprises threads formed of other solid materials, such as, for example, metal. The thickness of the absorbent should be smaller than about 5 % of the cross-section area of the channel. Such a small limitation of the channel area only entails a minor pressure increase. In an advantageous embodiment, the mat is reinforced with a net of, for example, metal. In another advantageous embodiment, the absorbent is arranged elongated and penetrates through a greater part of the channel system. In a further advantageous embodiment, the absorbent is shaped as a guide vane, for example at bends and descents in the channel system.

In still another advantageous embodiment, the absorbent according to the invention is also adapted to be placed in a resistive attenuator. In yet another advantageous embodiment, such an attenuator is arranged in- combination with one or more reactive attenuators. In this embodiment, the sound field in the channel may be locally controlled and optimized attenuating properties be obtained.

BRIEF DESCRIPTION OF THE DRAWINGS

The invention will be explained in greater detail by descrip- tion of embodiments with reference to the accompanying drawings , wherein

Figure 1 shows the specific flow resistance versus the frequency of an absorbent according to the invention,

Figure 2 shows a cross section of an absorbent according to the invention, Figure 3 shows the absorption versus the frequency of a few embodiments of an absorbent according to the present invention,

Figure 4 shows a cross section in the longitudinal direction of part of a system for transport of a gaseous medium according to the invention, and

Figure 5 shows alternative cross section shapes of part of a system for transport of a gaseous medium according to the invention.

DESCRIPTION OF THE PREFERRED EMBODIMENT

The dynamic flow resistance, as previously mentioned, has one resistive part and one reactive part. The resistive part of the resistance is a viscous attenuation which is independent of the frequency of the sound. The reactive part is mass- dependent and exhibits a resistance which increases with the frequency. For the majority of known absorbents, the reactive resistance dominates in the frequency range of interest, that is, the frequency range where a good absorption is desired. For these absorbents, it is thus the frequency-dependent reactive flow resistance which determines the absorption properties. Since the absorption decreases with increased flow resistance, the absorption in the frequency range of interest decreases. Experiments have shown that a majority of known porous absorbents have a great reactive resistance in the frequency range where absorption is desired. The known absorbents thus do not fulfil the condition that the normalized flow resistance is limited between one and two within a wide frequency range .

Figure 1 shows the specific flow resistance versus the frequency of a porous absorbent. In the diagram, the resistive flow resistance is designated z and the reactive flow u> t t ¹ H¹

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adjustable diameter. The properties of the absorbent thus manufactured are adjustable and optimizable for a desired purpose .

When heating a gas, the gas particles move away from each other while at the same time the thermal movement increases, whereby the density decreases and the viscosity increases. This results in an increase of the resistive part of the flow resistance and a decrease of the reactive part. In the dia- gram of Figure 2, this is represented by the arrows A and B. An absorbent which, at normal temperature, has less good absorption properties will thus receive much better properties at higher temperatures . One absorbent which has this property is perforated sheet. Such an absorbent is suitably manufactured from a sheet with a thickness of 1 mm or less, with a degree of perforation which is less than 10 % and with holes which are about 1 mm or less. For a normal temperature, the holes would need to be smaller than one-tenth of a millimetre. Such a perforated sheet is difficult and costly to manufacture.

Figure 2 shows a typical absorbent according to the invention. It consists of a thin mat 1 of long elastic fibres, which cross each other in all directions in an irregular pattern. In the shown example, the threads are manufactured of a plastic such as, for example, polyester. An advantage of this material is that, in case of fire, it is decomposed into water and carbon dioxide. However, other materials of elongated bendable threads or fibres are also possible. The figure also shows an advantageous embodiment of the absorbent in which a thin foil 2 is attached as protection in front of the thin mat. In the shown example, the foil is fused to the mat in a line pattern 3. The foil primarily consists of a polyethylene film but may also be another plastic material or a metal foil. Figure 3 shows the influence of a covering foil on the absorbent. Depending on the thickness or weight of the foil, an absorption - decreasing with the frequency - is obtained at high frequencies . The figure shows a typical basic absorption of a porous absorbent and the effect of three different thicknesses, 5, 10 and 20 μm, of such a foil. It should be mentioned in this context that the foil, across the greater part of the absorbent surface, should lie loosely adjacent to the mat. In the shown case, this problem is solved in that the foil is fixed to the mat in lines only. In the case of direct contact, such as by gluing or if the foil is pressed against the absorbent of, for example, perforated sheet, the absorption is deteriorated at high frequencies. A foil prevents particles from penetrating into the absorbent. It is thus suitable for use in environments involving environmental requirements. The foil-clad absorbent will also have better long-term properties since particles do not penetrate into and stop up the porous channels .

Figures 4 and 5 show a transport system designed for a gaseous medium with a first 4, a second 5 and a third 6 channel section containing an absorbent 1 according to the invention. Since the absorbent is thin, it has very little influence on the cross-section area and thus gives rise to an extremely small pressure drop across the channel section. Because of its plasticity, the absorbent is suited to be arranged as a guide vane in the system, as shown in the example. The length of the absorbent is not, as in known sound attenuators, limited to the length of the attenuator itself but may be arranged optionally along the channel system. Figure 5 shows a few examples of how the absorbent is intended to be arranged in the transverse direction of the channel. In the channel 7, which may be of optional shape, the absorbent 1 is arranged in a laminated pattern 8, in a cross pattern 9, and in a circular pattern 10. Other shapes are also possible within the scope of the invention. The absorbent according to the invention is exceedingly suited to be arranged as a resistive attenuator together with a reflection or reaction attenuator in a channel system. By suitably dimensioning the properties of such attenuators, a very efficient attenuation may be obtained over a frequency interval such as, for example, a third octave band.

Although advantageous, the channel system is not limited to comprise a channel system with a circular-cylindrical cross section. The invention may, with an equivalent result, be applied to systems with a multi-edge cross section as well as to systems with longitudinally bent sections.

Claims

1. A sound absorbent for hygienic spaces comprising a porous mat (1) , characterized in that the normalized flow resistance of the mat is in the interval of 0.5-2.

2. A sound absorbent according to claim 1, characterized in that the mat (1) comprises a plurality of long threads compressed into a thin sheet.

3. A sound absorbent according to claim 2, characterized in that the threads are manufactured from a plastic material.

4. A sound absorbent according to claim 3 , characterized in that the plastic material is a polyester.

5. A sound absorbent according to any of the preceding claims, characterized in that the sheet is reinforced by a net of a shape-permanent material .

6. A sound absorbent according to any of the preceding claims, characterized in that the absorbent comprises a foil making free. contact with the mat.

7. A sound absorbent according to claim 1, characterized in that the absorbent, at high gas temperatures, comprises a perforated sheet.

8. A transport system for a gaseous medium comprising a plurality of channel sections, whereby at least a first channel section comprises an absorbent, characterized in that the absorbent is thin and its normalized flow resistance is in the interval of 0.5-2.

9. A transport system according to claim 8, characterized in that the thickness of the absorbent is smaller than one- twentieth of the channel dimension.

10. A transport system according to claim 8, characterized in that absorbent comprises a mat of compressed long threads of polyester.

11. A transport system according to any of claims 8-10, characterized in that absorbent is reinforced by a net of a shape-permanent material .

12. A transport system according to any of claims 8-11, characterized in that absorbent is placed at a distance along the walls of the channel.

13. A transport system according to any of claims 8-12, characterized in that absorbent forms guide vanes in the channel section.

14. A method for manufacturing an absorbent for hygienic spaces comprising a porous mat, characterized in that the normalized flow resistance of the mat is arranged in the interval of 1-2.

15. A method according to claim 14, characterized in that the mat is arranged from a plurality of long threads which are compressed into a thin sheet.

16.. A method for manufacturing an absorbent comprising a plurality of channels with a characteristic diameter influencing a resistive part of the normalized flow resistance and a characteristic length influencing a reactive part of the normalized flow resistance, characterized in that, within a desired frequency range, the characteristic diameter is influenced such that the resistive part of the normalized flow resistance is within the interval of 0.5 to 2, and that the characteristic length is influenced such that the reactive part of the normalized flow resistance is limited by the resistive part.

17. Use of an absorbent according to claims 1-7, a transport system according to claims 8-13, a method according to claims 14-15, or a method according to claim 15 in a ventilation plant .