Noise control constitutes a rapidly growing economic and public policy concern for the construction industry. Areas with high acoustical isolation (commonly referred to as ‘soundproofed’) are requested and required for a variety of purposes. Apartments, condominiums, hotels, schools and hospitals all require rooms with walls, ceilings and floors that reduce the transmission of sound thereby minimizing, or eliminating, the disturbance to people in adjacent rooms. Soundproofing is particularly important in buildings adjacent to public transportation, such as highways, airports and railroad lines. Additionally theaters, home theaters, music practice rooms, recording studios and the like require increased noise abatement. Likewise, hospitals and general healthcare facilities have begun to recognize acoustical comfort as an important part of a patient's recovery time. One measure of the severity of multi-party residential and commercial noise control issues is the widespread emergence of model building codes and design guidelines that specify minimum Sound Transmission Class (STC) ratings for specific wall structures within a building. Another measure is the broad emergence of litigation between homeowners and builders over the issue of unacceptable noise levels. To the detriment of the U.S. economy, both problems have resulted in major builders refusing to build homes, condos and apartments in certain municipalities; and in widespread cancellation of liability insurance for builders. The International Code Council has established that the minimum sound isolation between multiple tenant dwellings or between dwellings and corridors is a lab certified STC 50. Regional codes or builder specifications for these walls are often STC 60 or more. It is obvious that the problem is compounded when a single wall or structure is value engineered to minimize the material and labor involved during construction.
It is helpful to understand how STC is calculated in order to improve the performance of building partitions. STC is a single-number rating that acts as a weighted average of the noise attenuation (also termed transmission loss) of a partition across many acoustical frequencies. The STC is derived by fitting a reference rating curve to the sound transmission loss (TL) values measured for the 16 contiguous one-third octave frequency bands with nominal mid-band frequencies of 125 Hertz (Hz) to 4000 Hertz inclusive, by a standard method. The reference rating curve is fitted to the 16 measured TL values such that the sum of deficiencies (TL values less than the reference rating curve), does not exceed 32 decibels, and no single deficiency is greater than 8 decibels. The STC value is the numerical value of the reference contour at 500 Hz. For maximum STC rating, it is desirable for the performance of a partition to match the shape of the reference curve and minimize the total number of deficiencies.
An example of materials poorly designed for performance according to an STC-based evaluation is evident in the case of many typical wood framed wall assemblies. A single stud wall assembly with a single layer of type X gypsum wallboard on each side is recognized as having inadequate acoustical performance. That single stud wall has been laboratory tested to an STC 34—well below building code requirements. A similar wall configuration consisting of two layers of type X gypsum wall board on one side and a single layer of type X gypsum board on the other is an STC 36—only a slightly better result. In both cases, the rating of the wall is limited by poor transmission loss at 125, 160 and 2500 Hz. In many cases, the performance is about five to ten decibels lower than it is at other nearby frequencies. For example, at 200 Hz, the wall performs about 12 decibels better than it does at the adjacent measurement frequency, 160 Hz. Similarly, the same assembly performs five decibels better at 3150 Hz than it does at 2500 Hz.
Additionally, some walls are not designed to perform well with specific regard to an STC curve, but rather to mitigate a specific noise source. A good example is that of home theater noise. With the advent of multi-channel sound reproduction systems, and separate low frequency speakers (termed ‘subwoofers’) the noise is particularly troublesome below 100 Hz. The STC curve does not assess walls or other partitions in this frequency range. Materials or wall assemblies should be selected to isolate this low frequency sound.
Various construction techniques and products have emerged to address the problem of noise control, but few are well suited to target these specific problem frequencies. Currently available choices include: additional gypsum drywall layers; the addition of resilient channels plus additional isolated drywall panels and the addition of mass-loaded vinyl barriers plus additional drywall panels; or cellulose-based sound board. All of these changes incrementally help reduce the noise transmission, but not to such an extent that identified problem frequencies would be considered fully mitigated (restoring privacy or comfort). Each method broadly addresses the problem with additional mass, isolation, or damping. In other words, each of these is a general approach, not a frequency specific one.
More recently, an alternative building noise control product having laminated structures utilizing a viscoelastic glue has been introduced to the market. Such structures are disclosed and claimed in U.S. Pat. No. 7,181,891 issued Feb. 27, 2007 to the assignee of the present application. This patent is hereby incorporated by reference herein in its entirety. Laminated structures disclosed and claimed in the '891 patent include gypsum board layers and these laminated structures (sometimes called “panels”) eliminate the need for additional materials such as resilient channels, mass loaded vinyl barriers, and additional layers of drywall during initial construction. The resulting structure improves acoustical performance over the prior art panels by ten or more decibels in some cases. However, the described structures are another general frequency approach. In certain of these structures a single viscoelastic adhesive (with damping) is incorporated into the laminated panel. As will be demonstrated later, such adhesive is designed to damp sound energy within a single frequency band with poorer performance in other sound frequency ranges. For this reason, these structures compromise performance in certain frequency ranges in an attempt to best match the STC curve.
Accordingly, what is needed is a new material and a new method of construction that allows for the maximum reduction of noise transmission at low frequencies, high frequencies, or both simultaneously. What is needed is a panel tuned for performance at multiple problem frequencies.
A figure of merit for the sound attenuating qualities of a material or method of construction is the material's Sound Transmission Class (STC). The STC number is a rating which is used in the architectural field to rate partitions, doors and windows for their effectiveness in reducing the transmission of sound. The rating assigned to a particular partition design is a result of acoustical testing and represents a best fit type of approach to a set of curves that define the sound transmission class. The test is conducted in such a way as to make measurement of the partition independent of the test environment and gives a number for the partition performance only. The STC measurement method is defined by ASTM E90 “Standard Test Method Laboratory Measurement of Airborne Sound Transmission Loss of Building Partitions and Elements,” and ASTM E413 “Classification for Sound Insulation,” used to calculate STC ratings from the sound transmission loss data for a given structure. These standards are available on the Internet at http://www.astm.org.
A second figure of merit is loss factor of the panel. Loss factor is a property of a material which is a measure of the amount of damping in the material. The higher the loss factor, the greater the damping. The primary effects of increased panel damping are reduction of vibration at resonance, a more rapid decay of free vibrations, an attenuation of structure-borne waves in the panel; and increased sound isolation.
Loss factor is typically given by the Greek symbol “η”. For simple coating materials, the loss factor may be determined by the ASTM test method E756-04 “Standard Test Method for Measuring Vibration-Damping Properties of Materials.” This standard is available on the Internet at http://www.astm.org. For more complicated structures, such as the ones described in the present invention, a nonstandard test method or computer model must be employed to predict or measure the composite material loss factor. A loss factor of 0.10 is generally considered a minimum value for significant damping. Compared to this value, most commonly used materials, such as wood, steel, ceramic and gypsum, do not have a high level of damping. For example, steel has a loss factor of about 0.001, gypsum wallboard about 0.03, and aluminum a loss factor of about 0.006.
In order to design or assess the damping properties of a laminated panel that uses constrained layer damping, a predictive model is used such as the well known model first suggested by Ross, Kerwin, and Ungar. The Ross, Kerwin, and Ungar (RKU) model uses a fourth order differential equation for a uniform beam with the sandwich construction of the 3-layer laminated system represented as an equivalent complex stiffness.
The RKU model is covered in detail in the article “Damping of plate flexural vibrations by means of viscoelastic laminae” by D. Ross, E. E. Ungar, and E. M. Kerwin—Structural Damping, Section IIASME, 1959, New York, the content of which article is herein incorporated by reference. The topic is also well covered with specific regard to panels by Eric Ungar in Chapter 14, “Damping of Panels” in Noise and Vibration Control edited by Leo Beranek, 1971. An extension of this model to systems with more than three layers has been developed by David Jones in section 8.3 of his book Viscoelastic Vibration Damping. This model is used in all of the predictive calculations used for the present invention.
In accordance with the present invention, a new laminated structure and associated manufacturing process are disclosed which significantly improves the ability of a wall, ceiling, floor or door to resist the transmission of noise from one room to an adjacent room, or from the exterior to the interior of a room, or from the interior to the exterior of a room at both low frequencies and high frequencies.
In one embodiment the structure comprises a lamination of several different materials. In accordance with one embodiment, a laminated substitute for drywall comprises a first layer of selected thickness gypsum board which is glued to a center constraining material, such as 32 gauge sheet steel. The first adhesive has a shear modulus designed to achieve maximum damping at a target frequency such as 160 Hz. On the second surface of the steel constraining layer, a second layer of selected thickness gypsum board is glued in place using a second adhesive layer. The second adhesive layer has a different shear modulus to achieve maximum damping at a different frequency such as 2500 Hz. In one embodiment, the glue layers are two versions of a specially formulated QuietGlue® adhesive, which is a viscoelastic material available from Serious Materials, 1250 Elko Drive, Sunnyvale, Calif. 94089. In addition to the typical chemicals that make up the QuietGlue® adhesive, additional plasticizing compounds are added to aid the shift of the shear modulus to achieve maximum damping at a different frequency while keeping other adhesive material properties constant.
Formed on the interior surfaces of the two gypsum boards, the glue layer is about 1/16 inch thick. In one instance, a 4 foot×8 foot panel consisting of two ¼ inch thick gypsum wall board panels laminated over a 30 gauge steel sheet using two 1/16 inch thick layers of glue has a total thickness of approximately ⅝ inch. When used on both sides of a standard single wood stud frame, the assembly has an STC value of approximately 54. For comparison, a similar wall assembly constructed with ½ inch thick standard gypsum wallboard has an STC rating of approximately 34. The result is a reduction in noise transmitted through the wall structure of approximately 20 decibels compared to the same structure using common (untreated) gypsum boards of equivalent mass and thickness, and construction effort.
This invention will be more fully understood in light of the following drawings taken together with the following detailed description in which:
The following detailed description is meant to be exemplary only and not limiting. Other embodiments of this invention, such as the number, type, thickness, dimensions, area, shape, and placement order of both external and internal layer materials, will be obvious to those skilled in the art in view of this description.
The process for creating laminated panels in accordance with the present invention takes into account many factors: exact chemical composition of the glue; pressing process; and drying and dehumidification process.
The gypsum board in top layer 101 typically is fabricated using standard well-known techniques and thus the method for fabricating the gypsum board will not be described. Alternately, layer 101 may be any one of a layer of cement-based board, wood, magnesium oxide-based board or calcium silicate board. Next, on the bottom surface 101-1 of the gypsum board 101 is a patterned layer of glue 104 called “QuietGlue®” adhesive. Glue 104, made of a viscoelastic polymer modified with additives to give it a prescribed shear modulus upon curing, optimizes the sound dissipation at a specific range of frequencies. Glue layer 104 may have a thickness from about 1/64 inch to about ⅛ inch although other thicknesses may be used. When energy in sound interacts with the glue which is constrained by surrounding layers, the sound energy will be significantly dissipated thereby reducing the sound's amplitude across a target frequency range. As a result, the sound energy which will transmit through the resulting laminated structure is significantly reduced. Typically, glue 104 is made of the materials as set forth in TABLE 1, although other glues having similar characteristics to those set forth directly below in Table 1 can also be used in this invention.
An important characteristic of the glue composition and the overall laminated structure is the shear modulus of the glue when cured. The shear modulus can be modified from 103 to 107 N/m2 (or Pascals) depending on the frequency range of interest with the given materials of the given ranges listed in Table 1.
Note that as shown in Table 1, the sound frequency which is best attenuated by the glue varies from approximately 160 Hz for a shear modulus of about 103 Pascals (Pa), to approximately 2500 Hz for a shear modulus of about 105 Pa, and to approximately 5500 Hz for a shear modulus of about 106 Pa. The shear modulus is increased by decreasing the percent by weight of acrylate polymer and increasing the percent by weight of acrylic polymer or latex, all other ingredients remaining constant, as shown in Table 1.
Table 1 shows in the fourth column a preferred embodiment of the viscoelastic glue which has an optimum sound attenuation at 160 Hz. The preferred formulation is but one example of a viscoelastic glue. Other formulations may be used to achieve similar results and the range given is an example of successful formulations investigated here.
The physical solid-state characteristics of QuietGlue® adhesive include:
Applied to glue layer 104 is a constraining layer 102 made up of gypsum, vinyl, steel, wood, cement or another material suitable for the application. If layer 102 is vinyl, the vinyl is mass loaded and, in one embodiment, has a surface density of one pound per square foot or greater. Mass loaded vinyl is available from a number of manufacturers, including Technifoam, of Minneapolis, Minn. The constraining layer 102 may improve the sound attenuation and physical characteristics of a laminated panel so constructed.
As a further example, constraining layer 102 can be galvanized steel of a thickness such as 30 gauge (0.012 inch thick). Steel has a higher Young's Modulus than vinyl and thus can outperform vinyl as an acoustic constraining layer. However, for other ease-of-cutting reasons, vinyl can be used in the laminated structure in place of steel. Cellulose, wood, plastic, cement or other constraining materials may also be used in place of vinyl or metal. The alternate material can be any type and any appropriate thickness. In the example of
A second layer of viscoelastic glue 105 is applied to the second surface of constraining layer 102. Glue 105 is similar to glue 104 in all ways except for the shear modulus of glue 105 in the cured state. As with glue 104, a prescribed shear modulus allows for optimization of the sound dissipation at a specific range of frequencies. By setting the shear modulus (and therefore target frequency) of glue 105 different from the shear modulus (and therefore the target frequency) of glue layer 104, the laminated panel is able to dissipate two frequency regions simultaneously and improve the overall acoustical attenuation of the panel. By adding one or more additional constraining layers and the required one or more additional glue layers, the laminated panel can be tuned to attenuate three or more target frequency ranges.
Gypsum board layer 103 is placed on the bottom of the structure and carefully pressed in a controlled manner with respect to uniform pressure (measured in pounds per square inch), temperature and time. Alternately, layer 103 may be any one of a layer of cement-based board, wood, magnesium oxide-based board or calcium silicate board.
Finally, the assembly is subjected to dehumidification and drying to allow the panels to dry, typically for forty-eight (48) hours.
In one embodiment of this invention, the glue 104, when spread over the bottom surface 101-1 of top layer 101 or of any other material, is subject to a gas flow for about forty-five seconds to partially dry the glue. The gas can be heated, in which case the flow time may be reduced. The glue 104, when originally spread out over any material to which it is being applied, is liquid. By partially drying out the glue 104, either by air drying for a selected time or by providing a gas flow over the surface of the glue, the glue 104 becomes a sticky paste much like the glue on a tape, commonly termed a pressure sensitive adhesive (“PSA”). The gas flowing over the glue 104 can be, for example, air or dry nitrogen. The gas dehumidifies the glue 104, improving manufacturing throughput compared to the pressing process described for example, in U.S. Pat. No. 7,181,891 wherein the glue 104 would not be dried for an appreciable time prior to placing layer 103 in place.
The second panel, for example the constraining layer 102, is then placed over the glue 104 and pressed against the material beneath the glue 104 (as in the example of
A second layer of glue 105 is applied to the surface of the constraining material 102 on the side of constraining material 102 that is facing away from the top layer 101. In one embodiment, glue layer 105 is applied to the interior side of bottom layer 103 instead of being applied to layer 102. A gas can be flowed or forced over glue layer 105 to change glue 105 into PSA, if desired. Bottom layer 103 is placed over the stack of layers 101, 104, 102 and 105. The resulting structure is allowed to set under a pressure of approximately two to five pounds per square inch, depending on the exact requirements of each assembly, for a time which can range from minutes up to hours, depending on the state of glue layers 104 and 105 in the final assembly. Other pressures may be used as desired.
In one embodiment the glue layers 104 and 105 are about 1/16th of an inch thick; however other thicknesses may be used. The glue layers 104 and 105 may be applied with a brush, putty knife, caulking gun, sprayed on, applied using glue tape or well known other means.
In fabricating the structure of
It is important to note that the viscoelastic adhesive material properties also vary tremendously as a function of temperature much like their dependence on frequency. For example, for a given viscoelastic material, the modulus and loss factor might be the same at 10 Hz and 25 degrees C. as it is at 700 Hz and 50 degrees C. Viscoelastic materials behave “colder” at high frequencies and “warmer” at low frequencies. In other words, there is a direct and proportional relationship between temperature and frequency. In fact, there are several ways to demonstrate the properties of a given viscoelastic material. The temperature could be held constant and the material tested over a very wide frequency range. Or, the temperature could be varied and the material tested over a much narrower frequency range. Then, temperature/frequency equivalence is applied to finally “reduce” the data and characterize the material. This phenomenon is reviewed in David Jones' book Viscoelastic Vibration Damping, the content of which is herein incorporated by reference.
For these reasons, the present invention may also be considered useful for providing improved acoustical isolation for assemblies subject to multiple temperature exposures. In such a case, a first layer of glue could be designed to have maximum damping at 0 degrees C. (probable winter temperatures in a cold climate) and a second layer of glue designed to have maximum damping at 25 degrees C. (probable summer temperatures) in the same panel.
Referring to
Referring to
The dimensions given for each material in the laminated structures of the present invention can be varied in view of cost, overall thickness, weight, and desired sound transmission properties. For example, two or more non-overlapping patterns of glue with different shear moduli can be used in the embodiment of
An embodiment of this invention uses two or more glues with different shear moduli in each glue layer in the structure of
As will be apparent from the above description, the structures of that pattern can be tailored to give desired sound attenuation in selected frequency ranges.
The patterns of glue making up each glue layer can be applied in strips or squares or other shapes using brushes or glue applicators of well-known design.
The above-described embodiments and their dimensions are illustrative and not limiting. In addition, further other embodiments of this invention will be obvious in view of the above description.
Accordingly, the laminated structure of this invention provides a significant improvement in the sound transmission class number associated with the structures and thus reduces significantly the sound transmitted from one room to adjacent rooms while simultaneously providing specific additional sound dissipation at multiple frequencies.
Other embodiments of this invention will be obvious in view of the above description.
The present application is a continuation-in-part of U.S. patent application Ser. No. 11/772,197 filed Jun. 30, 2007 by Brandon D. Tinianov entitled “Acoustical Sound Proofing Material With Improved Damping At Select Frequencies And Methods For Manufacturing Same” which is incorporated herein by reference in its entirety.
Number | Name | Date | Kind |
---|---|---|---|
2811906 | Chappell | Nov 1957 | A |
3092250 | Knutson et al. | Jun 1963 | A |
3160549 | Caldwell et al. | Dec 1964 | A |
3215225 | Kirschner | Nov 1965 | A |
3336710 | Raynes | Aug 1967 | A |
3399104 | Ball, III et al. | Aug 1968 | A |
3424270 | Hartman et al. | Jan 1969 | A |
3462899 | Sherman | Aug 1969 | A |
3579941 | Tibbals | May 1971 | A |
3642511 | Cohn et al. | Feb 1972 | A |
3828504 | Egerborg et al. | Aug 1974 | A |
4003752 | Osohata et al. | Jan 1977 | A |
4112176 | Bailey | Sep 1978 | A |
4156615 | Cukier et al. | May 1979 | A |
4347912 | Flocke et al. | Sep 1982 | A |
4364017 | Tokunaga et al. | Dec 1982 | A |
4375516 | Barrall | Mar 1983 | A |
4487793 | Haines et al. | Dec 1984 | A |
4618370 | Green et al. | Oct 1986 | A |
4642951 | Mortimer | Feb 1987 | A |
4663224 | Tabata et al. | May 1987 | A |
4678515 | Green et al. | Jul 1987 | A |
4685259 | Eberhart et al. | Aug 1987 | A |
4759164 | Abendroth et al. | Jul 1988 | A |
4778028 | Staley | Oct 1988 | A |
4786543 | Ferm | Nov 1988 | A |
4924969 | K'Heureux | May 1990 | A |
4956321 | Barrall | Sep 1990 | A |
4967530 | Clunn | Nov 1990 | A |
5016413 | Counihan | May 1991 | A |
5026593 | O'Brien | Jun 1991 | A |
5033247 | Clunn | Jul 1991 | A |
5063098 | Niwa et al. | Nov 1991 | A |
5110660 | Wolf et al. | May 1992 | A |
5125475 | Duchame et al. | Jun 1992 | A |
5158612 | Savoly et al. | Oct 1992 | A |
5240639 | Diez et al. | Aug 1993 | A |
5256223 | Alberts et al. | Oct 1993 | A |
5258585 | Juriga | Nov 1993 | A |
5334806 | Avery | Aug 1994 | A |
5342465 | Bronowicki et al. | Aug 1994 | A |
5368914 | Barrett | Nov 1994 | A |
5439735 | Jamison | Aug 1995 | A |
5473122 | Kodiyalam et al. | Dec 1995 | A |
5474840 | Landin | Dec 1995 | A |
5502931 | Munir | Apr 1996 | A |
5585178 | Calhoun et al. | Dec 1996 | A |
5603192 | Dickson | Feb 1997 | A |
5629503 | Thomasen | May 1997 | A |
5643666 | Eckart et al. | Jul 1997 | A |
5664397 | Holz | Sep 1997 | A |
5691037 | McCutcheon et al. | Nov 1997 | A |
5695867 | Saitoh et al. | Dec 1997 | A |
5768841 | Swartz et al. | Jun 1998 | A |
5824973 | Haines et al. | Oct 1998 | A |
5867957 | Holtrop | Feb 1999 | A |
5910082 | Bender et al. | Jun 1999 | A |
5945208 | Richards et al. | Aug 1999 | A |
5945643 | Casser | Aug 1999 | A |
5954497 | Cloud et al. | Sep 1999 | A |
6077613 | Gaffigan | Jun 2000 | A |
6123171 | McNett et al. | Sep 2000 | A |
6213252 | Ducharme | Apr 2001 | B1 |
6240704 | Porter | Jun 2001 | B1 |
6266427 | Mathur | Jul 2001 | B1 |
6286280 | Fahmy et al. | Sep 2001 | B1 |
6290021 | Strandgaard | Sep 2001 | B1 |
6309985 | Virnelson et al. | Oct 2001 | B1 |
6342284 | Yu | Jan 2002 | B1 |
6381196 | Hein et al. | Apr 2002 | B1 |
6389771 | Moller | May 2002 | B1 |
6443256 | Baig | Sep 2002 | B1 |
6632550 | Yu et al. | Oct 2003 | B1 |
6676744 | Merkley et al. | Jan 2004 | B2 |
6699426 | Burke | Mar 2004 | B1 |
6715241 | Gelin et al. | Apr 2004 | B2 |
6758305 | Gelin et al. | Jul 2004 | B2 |
6790520 | Todd et al. | Sep 2004 | B1 |
6800161 | Takigawa | Oct 2004 | B2 |
6803110 | Drees et al. | Oct 2004 | B2 |
6815049 | Veramasuneni | Nov 2004 | B2 |
6822033 | Yu | Nov 2004 | B2 |
6825137 | Fu et al. | Nov 2004 | B2 |
6877585 | Tinianov | Apr 2005 | B2 |
6913667 | Nudo et al. | Jul 2005 | B2 |
6920723 | Downey | Jul 2005 | B2 |
6941720 | Deford et al. | Sep 2005 | B2 |
7041377 | Miura et al. | May 2006 | B2 |
7068033 | Sellers et al. | Jun 2006 | B2 |
7181891 | Surace et al. | Feb 2007 | B2 |
7197855 | Della Pepa | Apr 2007 | B2 |
20030006090 | Reed | Jan 2003 | A1 |
20040016184 | Huebsch et al. | Jan 2004 | A1 |
20040168853 | Gunasekera et al. | Sep 2004 | A1 |
20040214008 | Dobrusky et al. | Oct 2004 | A1 |
20050050846 | Surace et al. | Mar 2005 | A1 |
20050080193 | Wouters et al. | Apr 2005 | A1 |
20050103568 | Sapoval et al. | May 2005 | A1 |
20060048682 | Wagh et al. | Mar 2006 | A1 |
20060057345 | Surace et al. | Mar 2006 | A1 |
20060059806 | Gosling et al. | Mar 2006 | A1 |
20060108175 | Surace et al. | May 2006 | A1 |
20070094950 | Surace et al. | May 2007 | A1 |
20070107350 | Surace et al. | May 2007 | A1 |
Number | Date | Country |
---|---|---|
2219785 | Oct 1996 | CA |
1154087 | Nov 2001 | EP |
09-203153 | Aug 1997 | JP |
WO 9634261 | Oct 1996 | WO |
WO 9719033 | May 1997 | WO |
WO 0024690 | May 2000 | WO |
Number | Date | Country | |
---|---|---|---|
20090004448 A1 | Jan 2009 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 11772197 | Jun 2007 | US |
Child | 11849150 | US |