US20050167194A1

US20050167194A1 - Accoustical Absorption Coating and Process

Info

Publication number: US20050167194A1
Application number: US10/708,019
Authority: US
Inventors: Gerry Arner
Original assignee: Arner Investments Inc
Current assignee: Arner Investments Inc
Priority date: 2004-02-03
Filing date: 2004-02-03
Publication date: 2005-08-04

Abstract

A process for dampening sound and a material for effecting that process have been developed. The process involves applying multiple layers of a coating that then transmits that sound into very small cavities. These cavities perform several functions, they further transmit the sound, they absorb some of the sound through the random cancellation of reflecting waves, and they contain sound attenuation media such as closed cell cavities and projection particles. The projection particles act in at least two ways, they perform a baffling function, and they act as sympathetic resonators. The material which has been developed to effect this process consists of a lattice structure with vacant and non vacant cavities. The non-vacant cavities contain structures and mechanisms for altering, redirecting, reflecting, and absorbing the incident acoustical waves. The invention may be extended to hot gas environments and electrically and thermally conductive surface coating applications.

Description

BACKGROUND OF INVENTION

Many Coating manufacturers are currently claiming acoustical reduction in coatings due to the inclusion of ceramic particles in architectural paint. These claims are largely inaccurate and misleading. Paints form a continuous polymer film over a surface. This continuous polymer film reflects sound. The inclusion of sound absorbing materials in such a coating is irrelevant as the sound absorbing material is not directly impacted by the acoustical waves, rather the encompassing coating reflects the incoming waves before any acoustical damping takes place. In fact NONE of these manufacturers have an acoustical rating as defined by a noise reduction coefficient associated with their products which is greater than that offered by a standard paint. The current invention differs from the prior art in the use of a lattice work structure rather than a continuous film. The lattice work structure is applied as a coating and may be of a variety of densities or porosity, but the exposure of attenuation material to the incident sound is critical.
The field of the invention is the process of damping or attenuating sound incident upon an architectural surface. The control and engineering of sound levels has been regarded as an independent discipline for at least 100 years. In Residential environments, the quality of life has been directly tied to the ambient noise levels (consider for instance studies done regarding airline flight paths) In industrial environments there are critical concerns regarding productivity of employees and incident stress on equipment which is related to the ambient noise level. This invention is directed at the process of economically reducing noise levels in these environments. ART A sound source produces pressure variations in the air moving outward from the source in a progressive wave at a speed of about 1100 feet per second. In free space, the energy intensity in the wave decreases as the distance from the source increases. Sound waves indoors are reflected many times by the enclosing surfaces, the intensity remaining more or less uniform throughout a room. The sound wave carries energy from the source to the ear or other receiver. The present invention is specifically directed towards usefully reducing the intensity of these sound waves. The amount of sound energy that reaches the listener depends on the paths by which the sound has traveled, on the distance from the source, the power of the source, and the nature of such intervening barriers as walls, doors, windows, and sound-absorbing ducts. Qualities that characterize a desirable acoustic environment vary widely, depending on how the space is to be used, how particular the users are, and how the specific space involved relates to other parts of the building. When a sound wave strikes a sizable surface, such as a wall or ceiling, part of it is reflected, part of it is absorbed, and part of it may be transmitted to some adjoining space. The relative magnitudes of the three parts of the original sound are determined by the physical properties of the surface. A hard-surfaced, painted sheet of drywall reflects most of the sound that strikes it, while a soft surface such as a heavy carpet reflects little sound. Absorption and reflection are important only in connection with the space in which the sound originates. Useful sound absorption is provided by porous material such as carpets, draperies, glass-fiber blankets, clothing, and specially-made sound-absorbing materials. An essential property of a sound-absorbing material is that it have a porous structure into which the molecules in the air carrying sound energy can dissipate that energy in the form of heat. This porous structure CANNOT be supplied by a traditional paint where the resin binder of the coating develops a continuous film. Sound energy so dissipated is never recovered as sound. When sound-absorbing materials are placed within a room, the reflection of energy is greatly reduced and the sound dies away rapidly. Good hearing conditions for an audience listening to speech or music, whether in an auditorium, courtroom, church, theater, or living room, depend on four basic conditions. The space must be quiet, the sounds to be heard must have adequate loudness, there must be a good dispersion of sound, and the sounds must be properly blended, with adequate separation for good articulation of music or speech. The velocity for a sound wave is directly proportional to frequency and the medium of transport. It follows that any substance that absorbs sound will tend to absorb high frequencies more than low frequencies. However, the principle of resonance in physics can be used to increase the velocity in a sound wave at or near a resonant frequency and thus to increase absorption at low frequencies by design of suitable resonators. The present invention addresses the difficulties typically found in absorption media by providing absorbers for lower frequency sound waves.
It is an object of the present invention to absorb both high and low frequency sound in industrial and residential architectural environments. is further an object of the present invention to provide an economical method to reducing unwanted noise in existing structures. It is a further object of the present invention to reduce the structural stresses associated with extreme acoustical vibration in hot gas environments. It is a further object of the present invention to enable a process of absorbing sound where the set up of the mechanism through which the process of absorbing the sound is effected involves nothing more than the application of a coating. These and other objects and advantages of the present invention will become apparent from a reading of the attached specification and appended claims.

DETAILED DESCRIPTION

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The present invention details a article of manufacture and a process of acoustical absorption which utilizes that article. The article to be described below as the preferred embodiment uses a carrier system which generally involves a binder which may be a water borne polymer system or a solvent borne polymer system, additionally the binder may be an inorganic adhesive, or an inorganic salt. The preferred embodiment uses a water borne single component vinyl acrylic. It should be understood that the vinyl acrylic could be any one of the multitude of acrylic″s, polyurethane″s, epoxies, polyurea″s, etc which are typically used for coating applications. The binder system in the preferred embodiment requires a coalescing solvent. Each binder system has a variety of coalescing solvents which work with varying degree″s of effectiveness and which impart a number of application oriented properties such as dry time, viscosity etc. One skilled in the art would generally know the specific coalescing solvent for each binder system. For the preferred embodiment texanol coalescing solvent is used at a ratio recommended by the manufacturer of the resin. The preferred embodiment uses a binder to volume ratio such that the final composition forms a substantially continuous lattice, network or porous structure. This structure or framework having vacant and non vacant cavities. preferred embodiment chemically or mechanically retains a plurality of mechanisms for altering, attenuating, reflecting, or absorbing sound. The mechanisms that alter, attenuate, reflect or absorb sound in some cases may be mechanically attached in the network structure, and in other cases may be chemically bound to the aforementioned lattice work. The preferred embodiment contains projection surfaces which act as mechanisms for projecting acoustical waves towards the absorbing or attenuating means. In the preferred embodiment the projection surfaces are composed of either one or a plurality of plate like ceramic particles selected from the group of platelet clays, platelet talc, mica, or plate like zirconium carbide. It is presumed that a number of materials may be available which due to plate like geometry are able to perform this function. These plate like materials serve a dual function, some of the plate like material will be exposed as a reflection surface, for example with the thin dimension of the plate perpendicular to the incident sound, in this case the plate like structures will reflect the sound. A portion f the incident sound will be immediately redirected, and some will be absorbed immediately. The means for absorbing the sound may operate as the sound is first incident or it may operate after the sound has been redirected by the plate like structures which are operating as reflectors. Some of the plate like material will have an exposed (of small relative dimension) edge. This exposed edge allows the same plate like material to act as a stub tuner would in traditional vibration damping applications, where such stub tuners are extended into vacant areas defined within said lattice structure; said stub tuners being non uniform in extended length. In the preferred embodiment the stub tuner mechanisms are composed of ceramic particles having a high aspect ratio in either one of three or two of three dimensions such as rods or plates, a plurality of these same exposed edges arranged together function as a baffle for the incoming acoustics. In the preferred embodiment these absorption particles may be composed of either one or a plurality of plate like ceramic particles selected from the group of platelet or rod like clays, platelet talc, mica, or plate like zirconium carbide. Additionally there are absorber means comprised of ceramic microspheres. Ceramic microspheres are generally known in the art and independent of a coating these microspheres are known to provide acoustical damping. In many recently developed coatings these microspheres are simply added to a traditional paint and the paint is then claimed to have sound absorbing properties. In fact as the microspheres are then covered by a sound reflecting material the bulk of their sound absorption properties are not retained in the coating. the preferred embodiment fibrous reinforcement is also utilized. The fibrous reinforcement may add a great deal of functionality to the coating. In the preferred embodiment these fibrous reinforcements add a method of crack propagation resistance. The novelty of the current invention is not only resident in the article of manufacture, but additionally the manner in which sound is attenuated. Sound is damped by economically applying multiple layers of a coating which uses means for transmitting sound incident upon a surface. In the preferred embodiment this means for transmitting sound is a loosely bound ceramic particles forming a non continuous highly porous layer. Within the first layer and within the second layer are means for absorbing sound and means for redirecting sound by means of plate or rod like structures once that sound has been transmitted. These plate like structures substantially perform a baffling function and they act as sympathetic resonators. The plate like structures in the preferred embodiment are comprised of various forms of plate like kaolin and talc, however it should be understood that most plate like ceramic particles could be incorporated to serve this function. Also absorbing sound in the first absorbing portion is effected by the use of hollow ceramic particles as resonant cavities. There are a wide variety of these particles which are known in the art and provided they are fit the definition of hollow ceramic spheres, they will appropriately aid the process of sound absorption. The sound having been partially absorbed by the initial surface and partially directed into the cavities of a coatings first absorbing portion may then run into a second absorbing portion where said incoming sound is further transmitted against an applied substrate. The substrate will act as a sound reflecting surface as it is situated directly after the second absorbing portion. This second absorbing portion may be substantially comprised of closed cell cavities in which incoming sound is damped by its own reflection and a plurality of sound attenuation media for absorbing acoustical energy. Further this second absorbing portion is comprised of a porous structure with adhesive bonding capability substantially integral with the lattice work previously mentioned. This adhesive bonding mechanism causes attachment of said second absorbing layer to a surface of interest. The surface of interest may be acoustically reflective or it may provide additionally sound attenuation properties. Within the scope of the preferred embodiment it may be desirable to apply either a single layer or a plurality of substantially equivalent layers. The fibrous reinforcement in the preferred embodiment may be used to add additional sound attenuation properties, or they may be used to enhance thermal or electrical conduction. Additionally the preferred process used may further utilize a lattice work which enables the damping of sound in a hot gas environment. Reinforcing the lattice structure with a thermal conduction mechanism may further assist this hot gas capability. It may also be desirable to utilize this coating as a smart coating surface where electrical conduction for either the dissipation of static electric charge, or the conduction of electrical currents for sensing applications or low power transfer. To effect this a number of ceramic materials which also may act as acoustical reflectors or as acoustical absorbers as generally known in the art may be used such as Indium tin oxide or Antimony tin oxide may be used. A particularly interesting embodiment involves the use of a piezoelectric material such as barium titanate to convert the acoustical energy incident on the coating into electrical energy to be dissipated or transmitted by the coating. Alternately the process described in the preferred embodiment may be extended where the process additionally involves the resistance of mildew growth through the retention of sufficient porosity to enable a permeability rating or flame spread equivalent to a class 1fire rating.

Claims

1. A sound attenuation material which comprises; A Lattice structure; said lattice structure comprising a substantially continuous framework; said framework having vacant and non vacant cavities; said structure further chemically or mechanically retaining a plurality of mechanisms for altering, attenuating, reflecting, or absorbing sound; material further comprising Projection surfaces mechanisms for projecting acoustical waves towards absorbing or attenuating means; further said projection mechanisms being retained by said lattice structure material further comprising Absorber or attenuation means

2. A sound attenuation material as in claim 1 where lattice structure is primarily resin based

3. A sound attenuation material as claimed in claim 1 where said lattice structure is completely inorganic in composition

4. An article of manufacture as claimed in claim 1 where said lattice structure is reinforced with thermal conduction means.

5. A sound attenuation material as claimed in claim 1 where Said Projection surfaces are composed of a a plurality of plate like ceramic particles selected from the group of platelet clays, platelet talcs, mica, or plate like zirconium carbide.

6. A sound attenuation material as claimed in claim 1 where said projection surfaces are composed of one of the following group: platelet clays, platelet talcs, mica, or other ceramic particles available in platelet form.

7. A sound attenuation material as claimed in claim 1 where said absorber means comprises ceramic microspheres;

8. A sound attenuation material as claimed in claim 7 where said absorber means additionally comprising extended stub tuning apparatus where such stub tuners are extended into vacant areas defined within said lattice structure; said stub tuners further being non uniform in extended length

9. A sound attenuation material as claimed in claim 8 where said stub tuner means are composed of ceramic particles having a high aspect ratio in at least two of three dimensions such as rods or plates.

10. A sound attenuation material as claimed in claim 1 where said material additionally comprising crack propagation resistance means;

11. An article of manufacture as claimed in claim 10 where said crack resistance means is thermally conductive

12. An article of manufacture as claimed in claim 10 where said crack resistance means are electrically conductive

13. A sound attenuation material as claimed in claim 10 where said crack propagation resistance means consists of fibrous reinforcement; said fibrous reinforcement also possessing sound attenuation properties.

14. An article of manufacture as claimed in claim 1 where said lattice structure is electrically conductive

15. An article of manufacture as claimed in claim 1 where one or a plurality of components including the lattice, the acoustical reflectors, and the acoustical absorbers are electrically conductive

16. A Process for dampening sound involving the application of multiple layers of a coating comprising: for transmitting sound incident upon a surface; for Absorbing sound once it has been transmitted into the cavities of a coatings first absorbing portion; a second absorbing portion where said incoming sound is further transmitted said sound transmission surfaces being situated directly after said second absorbing portion; Said second absorbing portion being substantially comprised of closed cell cavities in which incoming sound is damped by its own reflection and a plurality of sound attenuation media for absorbing acoustical energy;

17. A process for dampening sound as claimed in claim 16 where said means for transmitting sound is a porous layer of loosely bound ceramic said loosely bound ceramic forming a non continuous highly porous first coating layer.

18. A process for dampening sound as claimed in claim 17 wherein said non continuous highly porous first coating layer also comprises sound redirection means

19. A process for dampening sound as claimed in claim 18 wherein said redirection means comprises plate or rod like structures;

20. A process for dampening sound as claimed in claim 19 wherein said plate or rod like structures substantially act as sympathetic resonators

21. A process for dampening sound as claimed in claim 18 wherein said plate or rod like structures substantially perform a baffling function.

22. A process for dampening sound as claimed in claim 18 where said plate or rod like structures are comprised of various forms of plate like kaolin and talc.

23. A process for dampening sound as claimed in claim 16 where said means for absorbing sound in said first absorbing portion is effected by the use of hollow ceramic particles as resonant cavities.

24. A process for dampening sound as claimed in claim 16 where said means for absorbing sound in said first absorbing portion is effected by the use of baffles formed by the positioning within said transmission means of particles performing a baffling function.

25. A process for dampening sound as claimed in claim 16 where said second absorbing portion is comprised of a porous structure with adhesive bonding means substantially integral with network formation means; said adhesive bonding means causing attachment of said second absorbing layer to a surface;

26. A process for dampening sound as claimed in 24 where said surface is required to be acoustically reflective;

27. A process for dampening sound as claimed in claim 24 where said surface may additionally provide sound attenuation means;

28. A process for dampening sound as claimed in claim 16 where said second absorbing layer is comprised of any number of a plurality of substantially equivilent layers;

29. A Process as claimed in claim 16 where said lattice work enables the damping of sound in a hot gas environment

30. A process as claimed in claim 16 where one or a plurality of components including the lattice, the acoustical reflectors, and the acoustical absorbers exhibit electrical conductivity.

31. A process as claimed in claim 16 where the process additionally involves the resistance of mildew growth by application means which retains sufficient porosity to enable a permeability rating.

32. A process as claimed in claim 16 wherein the process additionally involves a resistance to flame spread

33. A process as claimed in claim 16 wherein said incident acoustical energy is alternately transformed into electrical energy through the auspices of a piezoelectric material such as barium titanate.