Abstract:
A medical device includes a one-piece resiliently biased band of base material having opposite first and second side surfaces and an adhesive material for temporarily adhesively securing the band to a user&#39;s skin. The band can include a longitudinal axis and a lateral axis that intersects the longitudinal axis. Moreover, the band can include first and second lateral portions disposed on opposite sides of the lateral axis. The lateral portions are mirror images of each other such that the band is symmetrical relative to the lateral axis. Each of the lateral portions include a central portion and first and second extending portions spaced apart from each other on opposite sides of the longitudinal axis of the band and extending away from the central portion. Each of the extending portions further include a perimeter edge defining a portion of an edge of the medical device.

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS 
       [0001]    This is a continuation of U.S. patent application Ser. No. 11/848,132 , filed Aug. 30, 2007, which claims priority to U.S. Provisional Application No. 60/841,403, filed on Aug. 30, 2006, the entire contents of each of which are hereby incorporated herein by reference. 
     
    
     BACKGROUND 
       [0002]    The materials manufacturing industry has been extruding plastic polymer sheeting materials for many years. Such extrusion has included etching steel rollers to imprint a texture, such as a matte finish, onto the plastic sheeting as it is extruded. For example, plastic materials having a “leather-like” finish for automotive interiors are made by imprinting the “leather-like” appearance onto the sheeted polymer material. 
         [0003]    More recently, etched or machined rollers have been used to impart more intricate designs, such as a diamond-shaped pattern, onto sheeted plastic materials, such as those used for truck bed liners. 
       SUMMARY OF THE INVENTION 
       [0004]    The present invention is directed to a material having a desired stiffness, said stiffness resulting from a groove or a plurality of grooves or cross sectional shapes imparted onto one or more surfaces of the material. These grooves may be uniformly continuous across the web or may be discontinuous, providing alternating or varying stiffness throughout the web. The present invention is also directed to a method for making the material. 
         [0005]    The present invention is also directed to a nasal dilator for dilating nasal passages using the material of the present invention. The material is preferably of sufficient stiffness to lift and dilate the nasal passages when secured to the nose. 
         [0006]    The present invention is also directed to medical devices, packaging, or construction materials made from the material described herein. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0007]      FIG. 1  shows a diagram of conventional polymer sheet extrusion. 
           [0008]      FIGS. 2   a - e  are various views of the grooved material of the present invention. 
           [0009]      FIGS. 3   a  and  b  are cross-sectional views of the grooved material of the present invention. 
           [0010]      FIG. 4  is a diagram of an extrusion apparatus suitable for extruding the material of the present invention. 
           [0011]      FIGS. 5   a  and  b  are various views of another embodiment of the grooved material of the present invention. 
           [0012]      FIG. 6   a  is a process diagram of grooves being imparted to an extruded material.  FIG. 6   b  is a process diagram of an adhesive layer and release liner layer being applied to an extruded grooved material. 
           [0013]      FIGS. 7   a - b  are views of an embodiment of a nasal dilator made in accordance with the present invention. 
           [0014]      FIG. 8  is a view of another embodiment of a nasal dilator made in accordance with the present invention. 
           [0015]      FIGS. 9   a - c  are views of various embodiments of a nasal dilator made in accordance with the present invention. 
           [0016]      FIGS. 10   a - c  are diagrams of a nasal dilator of the present invention worn on the user&#39;s nose. 
           [0017]      FIG. 11  is a view of another embodiment of the nasal dilator of the present invention. 
           [0018]      FIG. 12  is a view of another embodiment of the nasal dilator of the present invention. 
           [0019]      FIG. 13  is a view of another embodiment of the nasal dilator of the present invention. 
           [0020]      FIG. 14  is a diagram illustrating variables used in the calculation of a point load on a beam. 
           [0021]      FIG. 15  is a diagram illustrating variables used in the calculation of a distributed load on a beam. 
           [0022]      FIG. 16  is a diagram illustrating variables used in the calculation of a moment of inertia. 
           [0023]      FIG. 17  is a view of the grooved material separated along a groove. 
       
    
    
     DETAILED DESCRIPTION 
       [0024]    The present invention is directed to the unexpected discovery that imparting a functional, structural change to an extruded polymeric material can result in physical changes to the structural geometry of the polymers, thereby providing the effects of mono-axial or multi-axial orientation to the sheeted material. 
         [0025]    Traditionally, bi-axial and mono-axial orientation in a polymeric material have been accomplished by extruding polymers and stretching them as they cool down, which orients the polymers at the molecular level in the direction in which they are stretched (usually the machine processing direction only). Expensive tooling and specialized expertise is often required for this method. A schematic diagram of conventional extrusion is shown in  FIG. 1 . Polymeric material  5  is pumped through extrusion die assembly  6 . As material  5  leaves the die assembly  6 , it is cooled on chill or nip roll  7 , and then further processed as desired. 
         [0026]    The present invention is surprisingly able to achieve the effects of mono-axial orientation in a polymeric material by etching grooves or even discontinuous cross sectional shapes into the polymer sheet or web as it is extruded, rather than by stretching the polymers as they cool. As a result, it is possible to create the effect of molecular reorientation by physical means. Furthermore, by strengthening the material in one direction, the strength is reduced in others, allowing a significant degree of control over the flexural and other properties of the extruded material. In accordance with the present invention, it is possible to create a web of grooved material in which the channels are weakened to a specific degree allow one to tear the web with significantly less force along the channel without tearing outside the channel, resulting in a clean torn edge, substantially without sharp or jagged edges. 
         [0027]    As used herein, the term “grooves” shall be used to include furrows or channels (continuous or discontinuous) having any length or width, and any appearance or design from either a top view or a cross-sectional view of the groove. The shape, dimensions and frequency of the grooves are preferably selected to impart a desired stiffness to the material. The desired stiffness can be selected based in part on the type of material being extruded, the thickness of the material, the flexural modulus of the material, and the cross-sectional design or appearance of the grooves or resultant web. 
         [0028]    “Flexural modulus”, as used herein, shall refer to the ratio, within the elastic limit, of the applied stress on a test specimen in flexure, to the corresponding strain in the outermost fibers of the specimen. 
         [0029]    As used herein, “mono-axial orientation” or “multi-axial orientation” shall refer to the process of stretching a hot polymer film or other article in one or more directions under conditions that result in molecular reorientation. 
         [0030]    One embodiment of the grooved material of the present invention is shown in  FIGS. 2   a - e.  As best seen in  FIG. 2   e , the material  10  has at least one groove  12  imparted onto a surface of material  10 .  FIGS. 3   a  and b show a cross-sectional view of the material  10 , taken along line x-x′ of  FIG. 2   d . As seen in  FIGS. 3   a  and  b,  groove  12  comprises a ridge  13  having a thickness or height, shown as R i , and a width, shown as “X.” Groove  12  further comprises one or more valleys  14 , so that each ridge  13  is flanked on at least one side or on both sides by a valley  14 , shown as  14   a  and  14   b  in  FIG. 3   b . Valley  14  has a floor or base  16  having a thickness R 0 , and a width, shown as “Y,” of about 0.5.X, although these relative dimensions may vary depending on the degree of stiffness desired. 
         [0031]    The widths and heights or thicknesses of the peaks and valleys of the grooves can be calculated to provide an exact stiffness in both the machine processing direction and the transverse direction. For a uniform, flat web of material, the equation is: 
         [0000]      Stiffness=( F   m   ×T   3 )(1/12) 
         [0000]    where F m  is the flexural modulus of the starting material, and T is the thickness of the material. 
         [0032]    The grooves can provide the effects of mono-axial orientation in either the machine or transverse directions. In the embodiment in which grooves are made onto the material in the machine processing direction, thickness (T) is the sum of the peaks of the grooves, plus the thickness of the base of the material, as shown in  FIG. 3 . In the transverse direction, thickness is that of the base of the material. 
         [0033]    The grooves can be imparted onto the material using conventional extrusion technology or any other methods capable of creating grooves, cross sectional shapes or channels in the material, such as by casting, thermoforming or vacuforming the grooves into the material. An example of a suitable extrusion process is shown in  FIG. 4 . As the material  10  exits the extruder  20 , it is fed into nip rollers  22  and  24 . In one embodiment of the present invention, nip roller  22  imparts a first texture onto the material, such as grooves. Optionally, a second texture can be imparted onto the material by adding another nip roller  26 . The second texture imparted by nip roller  26  can be the same as the first texture, or can be different. The second texture can be imparted in the same processing direction as the first texture, or in a different direction, such as perpendicular to the first texture. In addition to the grooved textures described above, examples of other textures suitable for one or more surfaces of the material include a matte texture, a fabric texture, a leather texture, a combination of textures, and the like. 
         [0034]    It is preferred that the nip rollers used to make the grooved material of the present invention are nearly perfectly round, as irregularities may not provide the desired properties achieved by the careful calculations of the groove dimensions. It is preferred that the groove dimensions be imparted to the material with as little deviation from the desired dimensions as possible. If a repeating design, such as a sine wave, is placed in the machine direction, care must be taken to achieve matching of the design onto itself when circumferentially placed around the roll. 
         [0035]    The grooves can be imparted in any configuration. In one embodiment, straight grooves are etched into the material. In another embodiment, sinusoidal grooves are etched into the material. The grooves in the embodiments shown in the Figures are imparted in a either in a parallel or sinusoidal pattern. Other patterns, such as, but not limited to, zig-zags, scallops, flutes, and combinations of patterns are also contemplated by the present invention. The patterns may be continuous or discontinuous, and regular or irregular along the material, and may intersect at one or more locations to provide additional strength or stiffness at the point of intersection. 
         [0036]    The configuration of the grooves can also be etched in other designs, such as words, pictures, a raised watermark or a logo. The grooves can have varying thicknesses in the transverse direction, or there can be ungrooved portions between a groove or series of grooves. An example of a material having grooves with varying thicknesses is shown in  FIGS. 5   a  and  b.    
         [0037]    The grooves, in addition to providing the effects of mono-axial or multi-axial orientation to the material, increase the surface area of the material, and can be used to provide a trough for the application of additional materials, such as, but not limited to adhesives, dyes, medications, fragrances, and the like. 
         [0038]    Materials suitable for use in the method of the present invention include any formable material. Such materials include, but are not limited to, thermoplastic polymeric materials like acrylonitrile-butadiene-styrene (ABS), polyethylenes including high density polyethylene (HDPE), low density polyethylene (LDPE) and high molecular weight polyethylene (HMWPE), polypropylene, polyesters including polyethylene terephthalate (PET) and glycolised polyethylene terephthalate (PETG), polystyrene, polyurethane, vinyl, linoleum, rubber compounds, acrylics, nylon compounds, corn derivatives or other biodegradable resins, such as polylactic acid and polyhydroxyalkanoates, combinations of any of the foregoing, and the like. 
         [0039]    In addition to the formable materials described above, additional components may be added to the formable material, either before, during or after extrusion. Examples of such components include, but are not limited to, fragrances, medications, homeopathic compositions, aromatherapeutic compositions, antimicrobial agents, adhesives, dyes, pesticides, fungicides, herbicides, and combinations thereof. 
         [0040]      FIG. 6   a  is a process diagram of grooves being imparted to an extruded material. After the material passes through the extrusion die  31 , the extruded material  30  passes between an etched nip roller  32  and a matte finish nip roller  33 . The etched nip roller  32  imparts grooves to the extruded material  30  by impressing valleys into said material. The resulting grooved material  35  may then be rolled onto a take-up roller  34 . 
         [0041]    After the grooves are imparted to the material, an adhesive layer and release liner layer may be applied to one side of the grooved material.  FIG. 6   b  is a process diagram of an adhesive layer  40  and release liner layer  46  being applied to the extruded grooved material  35 . The adhesive material passes through an extrusion die  41 , to form adhesive layer  40 . Grooved material  35  and release liner layer  46  are positioned on either side of adhesive layer  40 . The grooved material  35  is positioned so that the grooved side of the material  35  is facing downward, toward the adhesive layer  40 . The grooved material  35 , adhesive layer  40 , and release liner layer  46  pass between nip rollers  42 , to yield a layered product  45 . In this layered product  45 , the adhesive from the adhesive layer  40  is in contact with and/or embedded within the grooves of the grooved material  35 . The layered product  45  may be rolled onto a take-up roller  44 . 
         [0042]    After the material is extruded and the grooves are imparted, further processing can occur. For example, the grooved material can be cut or stamped into desired shapes, and the cut pieces further processed into the final product. A dye laser can be used to impart a desired image or design onto one or both surfaces of the material. 
         [0043]    By using the known flexural modulus of the starting material, the resulting stiffness can be predicted (and adjusted accordingly) to make the desired product. Examples of such products include, but are not limited to, packaging, medical devices and consumer health products, and construction materials. One embodiment of the invention described below is for a nasal dilator. 
         [0044]    The present invention can be used to make any type of product in which the stiffness of one or more materials in the product is preferably controlled and/or controllable within a certain degree of flexure. The method can be used to make, for example, tear-apart products that require sufficient strength to remain intact during manufacture and distribution, but that can be easily separated by the end user as needed. Another application of the present invention is to imprint a grooved design that can then be the beginning of areas that will easily fold into designs like boxes or corners. Other applications utilize the ability to impart a different stiffness in one direction versus another. Further, the grooves can be made to interdigitate with each other if the web is folded back upon itself. Formulation of the polymer may include tackifiers to allow the web to stick to itself upon opposing onto itself or onto another sheet. The increased surface area of the grooves can improve heat sealing of edges when the grooves recess into each other and are heated. 
       Nasal Dilators 
       [0045]    Nasal dilators have provided innumerable people with relief from snoring or nasal congestion. Nasal dilators, such as those shown in U.S. Pat. Nos. 5,533,499, 5,706,800, and 7,114,495, typically include one or more resilient bands. When the resilient band is bent so that the ends of the band are moved closer together, the resilient band has a tendency to return to a planar state. When a nasal dilator is secured to a user&#39;s nose, the tendency of the resilient band to return to a planar state acts to prevent the outer wall tissue of the user&#39;s nasal passages from drawing in during breathing. In addition to a resilient band, nasal dilators often include additional flexible layers, in order to enhance the comfort and efficacy of the nasal dilators. 
         [0046]    As discussed in U.S. Pat. No. 5,476,091, issued to Johnson, a flexible strip of material positioned between the resilient band and the user&#39;s skin spreads out delaminating forces resulting from the resiliency of the dilator that could otherwise cause the nasal dilator to inadvertently become detached from the user&#39;s skin. The separation of the nasal dilator from portions of the user&#39;s skin can cause itching sensations. Therefore, by spreading out the delaminating forces, the flexible strip of material can substantially eliminate itching sensations that would otherwise be felt by the user. 
         [0047]    As described in U.S. Pat. No. 5,611,333, issued to Johnson, a nasal dilator may also include a flexible strip of top material, which covers the top of the resilient band. The flexible strip of top material may be included in order to help to prevent separation of the resilient band from the base material. The top material may also be included in order to increase the stiffness of the nasal dilator. 
         [0048]    There is a continuing need for improved nasal dilators that are able to provide the force needed to lift and open the nasal passages, while being comfortable for extended, often overnight use, and that can be gently and easily removed from the user&#39;s nose. 
         [0049]    Using the methodology of the present invention, it is possible to manufacture a nasal dilator comprising a material having specific flexural properties by imparting a particular set of grooves into the material. The method can use extrusion technology on plastic polymers or other materials to make a nasal dilator having the desired mono-axial flexural stiffness needed to effectively dilate the nasal passages. 
         [0050]    In order to provide sufficient dilation, a nasal dilator is preferably able to lift the tissues of the nasal passages when the dilator is initially secured to the nose, and is preferably able to continue lifting the nasal tissues over a period of time, without significant discomfort to the user. At the end of the desired period of use, the nasal dilator is preferably easily removable from the user&#39;s nose, also without significant discomfort to the user. 
         [0051]    A grooved nasal dilator in accordance with the present invention is preferably able to lift the lateral, lesser and greater alar cartilage structures of the nose, and preferably also facilitates the anterior and posterior dilator nares muscles of the nose. The grooved nasal dilator includes some type of engagement means, such as an adhesive, on the surface facing the user&#39;s skin. Preferably, the adhesive can removably adhere to the skin without causing skin irritation. In a preferred embodiment, the adhesive material is one that can absorb or transmit the moisture emanating up from the skin&#39;s surface. One example of such an adhesive includes hydrocolloid adhesives commonly used in ostomy bag adhesion or in wound care. Embedding the hydrocolloid into the grooves provides a larger repository for moisture accumulation without adding significant thickness or bulk to the overall profile of the nasal dilator. The grooved nasal dilator can remain in place over a period of time, without significant discomfort to the user, either while wearing the dilator or when removing the dilator. 
         [0052]    In order to significantly reduce the outer wall tissue of a user&#39;s nasal passages from drawing in during breathing, the nasal dilator of the present invention utilizes a grooved material made with a certain stiffness, adhered directly to the nose. The resilience of the grooved material can reduce or eliminate the need for one or more resilient bands, such as the resilient bands of the nasal dilators described in U.S. Pat. Nos. 5,533,499, 5,706,800, and 7,114,495. Therefore, if the grooved material of the present invention is used in a nasal dilator, a separate resilient band or bands may not be required. 
         [0053]    If a separate resilient band is used in combination with the grooved material of the present invention, the stiffness of the grooved material may make it possible to reduce the size of the resilient band that is necessary to provide sufficient stabilization and lifting of nasal tissue. Therefore, when used with the grooved material, the resilient band may be much smaller, lighter, and less obtrusive than in previous nasal dilators. 
         [0054]    Another advantage of the present invention is that it can simplify manufacturing by eliminating an entire component, namely, the resilient band, of a nasal dilator. Alternatively, if a resilient band is used in conjunction with the material of the present invention, a smaller, finer resilient band can be used, thereby providing a more fine-tuned, less obtrusive nasal dilator. 
         [0055]      FIGS. 7   a - b  show an embodiment of a nasal dilator made in accordance with the present invention.  FIG. 7   a  is a perspective view of the nasal dilator, and  FIG. 7   b  is an exploded perspective view showing the components of the nasal dilator. In this embodiment, no separate resilient band is used. The nasal dilator  50  comprises a grooved material  51 . The grooved material  51  includes an intermediate region  54  and end regions  53  and  55 . The grooved material  51  is sized so that the intermediate region  54  is able to traverse the bridge of a user&#39;s nose, and the end regions  53  and  55  are able to contact the outer wall tissues of the user&#39;s nasal passages. A layer of a biocompatible adhesive substance  52  is disposed on one side of the grooved material  51 . This adhesive secures the nasal dilator to the skin of the user during use. 
         [0056]    When the grooved material  51  is bent so that the end regions  53  and  55  are moved closer together, the grooved material  51  has a tendency to return to a planar state. When the nasal dilator  50  is secured to a user&#39;s nose, the tendency of the grooved material  51  to return to a planar state acts to prevent the outer wall tissue of the user&#39;s nasal passages from drawing in during breathing. 
         [0057]    The nasal dilator  50  may optionally include a release liner or liners  56  which are adhered to the grooved material  51  via the adhesive substance  52 . If included, the release liner or liners are removed prior to use. 
         [0058]    Another embodiment of a nasal dilator made in accordance with the present invention is shown in  FIG. 8 . This nasal dilator  60 , like the nasal dilator  50  of  FIG. 7 , comprises a grooved material  51  and a biocompatible adhesive substance  52 . The grooved material  51  is sized so that the intermediate region  54  is able to traverse the bridge of a user&#39;s nose, and the end regions  53  and  55  are able to contact the outer wall tissues of the user&#39;s nasal passages. The nasal dilator  60  may also include a release liner or liners which are adhered to the grooved material  51  via the adhesive  52 . 
         [0059]    The nasal dilator  60  also includes a resilient band  61 , positioned on either side of the grooved material  51 . In another embodiment, a plurality of resilient bands is used with the grooved material  51 . When the nasal dilator  60  is bent so that the end regions  53  and  55  are moved closer together, both the grooved material  51  and the resilient band  61  have a tendency to return to a planar state. When the nasal dilator  60  is secured to a user&#39;s nose, the tendency of the grooved material  51  and the resilient band  61  to return to a planar state acts to prevent the outer wall tissue of the user&#39;s nasal passages from drawing in during breathing. 
         [0060]    By using a grooved or etched polymer material as described above, nasal dilators of the present invention can be made very efficiently using extrusion techniques to impart the grooves to the material. Further embodiments of the nasal dilator in accordance with the present invention are shown in  FIGS. 9   a - c.    
         [0061]    The dimensions of the grooves, along with the properties of the material, will determine the flexural stiffness of the extruded nasal dilator. By using the methodology of the present invention, the dimensions of the grooves can be selected to optimize the anisotropic flexural properties in the longitudinal direction, as well as the transverse direction. 
         [0062]    The grooves can have a variable cross-section or thickness within the nasal dilator to provide for different stiffness or resiliency depending on the location of the grooves on the nasal dilator. 
         [0063]    For example, looking at a side view of the dilator, the grooves may have ridges that are higher along the center portion of the dilator, and shorter along the edges of the dilator. Alternatively, there may be one or more grooves having a higher profile, separated by one or more grooves that are shorter, followed by another groove or grooves that are higher. In another embodiment, a grooved region, having one or more grooves, may be adjacent to a region that does not have grooves, or has a different profile imparted onto that region. In this way, the relative stiffness and flexibility of the material can be carefully controlled to provide the desired degree of resiliency, comfort and removability. 
         [0064]    The nasal dilator may have any shape suitable for use on the nose or on the nasal passages. Preferably, the nasal dilator has a center region and two extending regions extending outwardly from the center region. By providing the desired resiliency to the nasal dilator, it is possible to convert the peel forces associated with the dilator in its latent, planar configuration to shear forces at the ends of the dilator when the extending regions are curved around the nose, as depicted in  FIGS. 10   a - c.  The “A” arrows in  FIG. 10   a  show the dilating force of the nasal dilator holding the nasal passages open, while the “B” arrows show the effects of shear force to keep the nasal dilator in place. This combination of forces provides the tension and lifting necessary to keep the nasal passages dilated during use. Preferably, the nasal dilator of the present invention provides between about 10 g to about 50 g of dilating force, more preferably, between about 12 g to about 40 g of dilating force, when the ends of the nasal dilator are positioned towards each other to be between about 1 to 1.5 inches apart. In one preferred embodiment, the nasal dilator of the present invention provides between about 14 g to about 30 g of dilating force, when the ends of the dilator are positioned to between about 1 to 1.2 inches apart during the course of use, which may vary from a few minutes to several hours, or preferably, overnight. Those skilled in the art will appreciate that the amount of force provided by the nasal dilator in use may deteriorate as the dilator is used, due to, among other things, relaxation of the dilator material and deterioration of the adhesive, so it is important to ensure that there is sufficient dilating force initially and during the course of use to keep the nasal passages open. It is preferred that the dilating force not deteriorate by more than about 20% over about an 8 hour time period. Yet another embodiment of a nasal dilator of the present invention provides for a greater dilator force initially with a rapid decline in lifting force over 8-12 hours. It has been found that PETG polymer is particularly preferred to maintain sufficient stiffness of the nasal dilator over time. 
         [0065]    The shear force is a function of the type of adhesive used to secure the nasal dilator to the user&#39;s nose, and is therefore related to the amount of dilating force provided by the nasal dilator. Preferably, the shear force is sufficient to keep the nasal dilator in place during use, and can be easily overcome by the user when removal of the nasal dilator is desired. 
         [0066]    The dilator may have any number of shapes, such as those shown in U.S. Pat. Nos. 6,029,658, 6,318,362, or 7,114,495, or as shown in the Figures. 
         [0067]    The nasal dilator of the present invention may be symmetrical along its long axis, or it may be asymmetrical along its long axis. The asymmetrical long axis may facilitate proper positioning of the dilator, and may provide a better fit to the shape of the nose, thereby improving the dilation and comfort of the nasal dilator in use. Preferably, the nasal dilator is symmetrical along its short axis. The symmetry along the short axis provides substantially uniform dilating forces on both sides of the nose. 
         [0068]    In another embodiment of the present invention, the dilator made with the grooved material may have a center aperture or opening, an example of which is shown in  FIG. 11 . This center aperture may be of any size or shape, and may comprise a cut out portion or a narrow slit, as shown in  FIG. 12 . The center aperture may include more than one aperture. The center aperture provides, among other things, an easy way for the user to center the dilator on his or her nose to assure proper placement for the most effective dilation. The center aperture or opening can be made by any conventional process, such as by die cutting the nasal dilator. 
         [0069]    The nasal dilator of the present invention may include a notch or a plurality of notches along the channel or channels of the material. By providing such notches, the size of the material used to make the nasal dilator can be easily laterally adjusted by removing one or more longitudinal groove portions, as shown in  FIG. 13 . 
         [0070]    The stiffness of the grooved material of the nasal dilator can be further adjusted after the extrusion process. In one embodiment, the stiffness of the material on one or more peripheral edges may be reduced to make the dilator more comfortable and easier to remove by the user. The stiffness can be reduced by using various techniques, such as laser cutting, water jet cutting, ultrasonic cutting, electron beam cutting, mechanical abrasion, and the like to remove or thin out portions of the material as desired. 
         [0071]    The nasal dilator of the present invention may include an additional component or components as described above. The additional component may be incorporated into the polymeric material before or after it is extruded. 
         [0072]    For example, a mentholated nasal dilator can be made in accordance with the present invention by providing a grooved nasal dilator having a menthol fragrance delivery system incorporated with the dilator, either before or after extrusion. Examples of suitable fragrance or medication delivery systems are described in U.S. Pat. Nos. 5,706,800; 6,244,265; 6,276,360; 6,550,474; 6,769,428; 7,011,093; and 7,013,889, each of which is fully incorporated herein by reference. 
         [0073]    The nasal dilator of the present invention can include features or elements associated with other nasal dilators, such as a material in contact with the user&#39;s nose under the nasal dilator, a cover, a full or partial adhesive void, a release liner or backing, and the like. Examples of such features and elements are described in U.S. Pat. Nos. 5,476,091; 5,533,499; 5,533,503; 5,549,103; 5,611,333; 5,653,224; and 6,318,362, each of which is fully incorporated herein by reference. 
       Flexural Stiffness Calculations for a Nasal Dilator 
       [0074]    To optimize the flexural properties of the nasal dilator, calculations must be made based on the varying loads that are applied to the dilator. A nasal dilator typically has a downward load on each end, with an upward load in the center. Due to the deflection of about 45.degree. at each end, equations typically used in beam analysis must be used with care. 
         [0075]    One can begin by using common beam equations to model the dilator because the loading herein is not continuously vertical, but remains predominantly lateral. The mechanical design issues at the large flexural strains of this application are then material properties and the effects of the resulting axial loading. This axial compression will somewhat reduce the tensile loading in the upper and increase the compressive loading in the lower fibers of the dilator under load. 
         [0076]    Modeling the dilator as a beam with a concentrated load, rather than a distributed load, will introduce errors in both the geometry of the deflection and the magnitude of the overall force needed at a particular deflection angle. For example, comparing the overall force as a point load at the end of a cantilevered beam to a uniformly distributed load along the beam results in the curvatures being to the third power in the former and the fourth power in the latter, as a function of distance from the support in the center. The deflection on the end of the former is about 2.7 times less than the latter. 
         [0077]    While the equations are not generally valid for the large deflections of the ends of the dilator, one skilled in the art will appreciate the correlation of load modeling with actual loads and deflections. This load modeling and associated load testing method can serve as a means for determining the desired flexibility of the grooved nasal dilators of the present invention. 
         [0078]    In addition to the location of the loading, the deflection of a beam, such as the nasal dilator, is generally related to four parameters: 
         [0079]    Magnitude of the load 
         [0080]    Cross-section of the beam 
         [0081]    Elasticity of the material 
         [0082]    Length of or distance along the beam 
         [0083]    Therefore, deflection at a point on a beam is usually characterized by an equation such as: 
         [0000]      Deflection on the beam=(Load)×(measure of the cross-section)×(measure of the elasticity)×(measure related to position along the beam)
 
         [0084]    This can be represented as: 
         [0000]        y=Px (1/ I)×( 1/ E )×(function of x)
 
         [0000]    where P is the force, I is the moment of inertia (second moment) of the beam cross-section, E is the modulus of elasticity, and x is the distance from the support, with the loading geometry/distribution determining the particular function of x. 
         [0085]    Once a dilator configuration is defined, the geometry value of I and the material property of E can be combined into “EI” (stiffness) or 1/(EI) (flexibility.) Then various loading scenarios can be evaluated. 
         [0086]    For a cantilevered beam loaded laterally at its end (with small deflections), deflection at x is 
         [0000]        y= ( Px   2 )(1/ EI )[(1/6)(3 L−x )] 
         [0000]    where L is the beam length 
         [0087]    The maximum deflection is at the end (x=L): 
         [0000]        y   max =( P )(1/ EI )[(1/3)L 3 ] 
         [0088]    Reference can be made to stiffness as: 
         [0000]      Stiffness=(1/12)( F   m   ×T   3 ) 
         [0000]      Or  E/= (1/12)( F   m   ×T   3 ) 
         [0089]    Again, the value of El will change if the geometry of the beam cross-section changes. The above equation actually derives from a simple rectangular beam cross-section, which has an I value of: 
         [0000]        I= (1/12)× b×h   3  
 
         [0000]    where b is the lateral base of the rectangular cross-section and h is the height of the cross-section. 
         [0090]    In the abbreviated equation above [Stiffness=(1/12)(F m ×T 3 )], F m  is actually (E×b), and T is h. 
       Calculation of Load on a Beam 
       [0091]    The following equations describe the calculations of a point or concentrated load on a beam, and a distributed load on a beam. As noted previously, while neither approach completely represents the actual load on a nasal dilator, one skilled in the art will recognize that models based on these approaches will be useful in determining the desired flexibility of the grooved nasal dilators of the present invention.  FIG. 14  is a diagram illustrating variables x, y, L, P 1 , and P 2  used in the calculation of a point load.  FIG. 15  is a diagram illustrating variables x, y, L, w 1 , and w 2  used in the calculation of a distributed load. 
       Calculation of a Point Load (P) 
       [0092]    
       
         
           
             
               
                 
                   y 
                   = 
                     
                    
                   
                     
                       
                         Px 
                         2 
                       
                       
                         6 
                          
                         
                             
                         
                          
                         EI 
                       
                     
                      
                     
                       ( 
                       
                         
                           3 
                            
                           
                               
                           
                            
                           L 
                         
                         - 
                         x 
                       
                       ) 
                     
                      
                     
                       y 
                       max 
                     
                   
                 
               
             
             
               
                 
                   = 
                     
                    
                   
                     
                       PL 
                       3 
                     
                     
                       3 
                        
                       
                           
                       
                        
                       EI 
                     
                   
                 
               
             
           
         
       
     
         [0000]    to achieve the same deflection at 
         [0000]    
       
         
           
             x 
             = 
             
               
                 
                   3 
                   4 
                 
                  
                 L 
                  
                 
                   : 
                 
                  
                 
                     
                 
                  
                 
                   
                     
                       
                         P 
                         1 
                       
                        
                       
                         ( 
                         
                           
                             3 
                             4 
                           
                            
                           L 
                         
                         ) 
                       
                     
                     2 
                   
                   
                     6 
                      
                     EI 
                   
                 
                  
                 
                   ( 
                   
                     
                       3 
                        
                       L 
                     
                     - 
                     
                       
                         3 
                         4 
                       
                        
                       L 
                     
                   
                   ) 
                 
               
               = 
               
                 
                   
                     
                       P 
                       2 
                     
                      
                     
                       ( 
                       
                         
                           3 
                           4 
                         
                          
                         
                             
                         
                          
                         L 
                       
                       ) 
                     
                   
                   3 
                 
                 
                   3 
                    
                   EI 
                 
               
             
           
         
       
       
         
           
             
                 
             
              
             
               
                  
                 
                   P 
                   2 
                 
               
               = 
               
                 
                   ( 
                   1.5 
                   ) 
                 
                  
                 
                   P 
                   1 
                 
               
             
           
         
       
     
       Calculation of a Distributed Load (w) 
       [0093]    
       
         
           
             
               
                 
                   y 
                   = 
                     
                    
                   
                     
                       
                         Wx 
                         2 
                       
                       
                         24 
                          
                         
                             
                         
                          
                         EI 
                       
                     
                      
                     
                       ( 
                       
                         
                           x 
                           2 
                         
                         + 
                         
                           6 
                            
                           
                               
                           
                            
                           
                             L 
                             2 
                           
                         
                         - 
                         
                           4 
                            
                           
                               
                           
                            
                           Lx 
                         
                       
                       ) 
                     
                      
                     
                       y 
                       max 
                     
                   
                 
               
             
             
               
                 
                   = 
                     
                    
                   
                     
                       wL 
                       4 
                     
                     
                       8 
                        
                       
                           
                       
                        
                       EI 
                     
                   
                 
               
             
           
         
       
     
         [0000]    to achieve the same deflection at 
         [0000]    
       
         
           
             x 
             = 
             
               
                 
                   ( 
                   
                     3 
                     4 
                   
                   ) 
                 
                  
                 L 
                  
                 
                   : 
                 
                  
                 
                     
                 
                  
                 
                   
                     
                       
                         
                           W 
                           1 
                         
                          
                         
                           ( 
                           
                             
                               3 
                               4 
                             
                              
                             L 
                           
                           ) 
                         
                       
                       2 
                     
                     
                       24 
                        
                       EI 
                     
                   
                    
                   
                     [ 
                     
                       
                         
                           
                             ( 
                             
                               
                                 3 
                                 4 
                               
                                
                               L 
                             
                             ) 
                           
                           2 
                         
                         + 
                         
                           6 
                            
                           
                             L 
                             2 
                           
                         
                         - 
                         
                           4 
                            
                           L 
                         
                       
                       = 
                       
                         
                           ( 
                           
                             3 
                             4 
                           
                           ) 
                         
                          
                         L 
                       
                     
                     ] 
                   
                 
               
               = 
               
                 
                   
                     
                       W 
                       2 
                     
                      
                     
                       ( 
                       
                         
                           3 
                           4 
                         
                          
                         L 
                       
                       ) 
                     
                   
                   4 
                 
                 
                   8 
                    
                   EI 
                 
               
             
           
         
       
       
         
           
             
                 
             
              
             
               
                  
                 
                   W 
                   2 
                 
               
               = 
               
                 
                   ( 
                   2.1 
                   ) 
                 
                  
                 
                   W 
                   1 
                 
               
             
           
         
       
     
       Calculation of Moment of Inertia (Second Moment, I) 
       [0094]    The grooved nasal dilator&#39;s cross-section is not a simple, rectangular beam. The variations during design can significantly change the value of I, and thus the stiffness of the beam. 
         [0095]    The total I of a particular design is calculated relative to the “neutral axis”, which passes through the centroid of the composite cross-sectional area. The centroid location will vary with each design&#39;s cross-section. The following shows the equation for the distance (y) from the “base” of the product to the neutral axis. Also shown is the equation for determining the actual I, using this distance.  FIG. 16  is a diagram illustrating variables h 1 , h 2 , b, b 1 , and b 2  used in the calculation of a moment of inertia. 
         [0000]    
       
         
           
             
               
                 
                     
                 
                  
                 
                   
                     
                       b 
                       
                         1 
                         = 
                       
                     
                      
                     
                       ( 
                       n 
                       ) 
                     
                   
                    
                   
                     ( 
                     b 
                     ) 
                   
                    
                   
                       
                   
                    
                   
                     ( 
                     
                       total 
                        
                       
                           
                       
                        
                       width 
                        
                       
                           
                       
                        
                       of 
                        
                       
                           
                       
                        
                       ridges 
                     
                     ) 
                   
                 
                  
                 
                     
                 
               
               _ 
             
             _ 
           
         
       
       
         
           
             
                 
             
              
             
               
                 ∑ 
                 
                   ( 
                   
                     
                       A 
                       i 
                     
                     · 
                     
                       y 
                       i 
                     
                   
                   ) 
                 
               
               = 
               
                 
                   [ 
                   
                     ∑ 
                     
                       ( 
                       
                         A 
                         i 
                       
                       ) 
                     
                   
                   ] 
                 
                  
                 y 
               
             
           
         
       
       
         
           
             
                 
             
              
             
               
                 
                   
                     ( 
                     
                       h 
                       1 
                     
                     ) 
                   
                    
                   
                     ( 
                     
                       b 
                       1 
                     
                     ) 
                   
                    
                   
                     ( 
                     
                       
                         h 
                         2 
                       
                       + 
                       
                         ( 
                         
                           
                             h 
                             1 
                           
                           2 
                         
                         ) 
                       
                     
                     ) 
                   
                 
                 + 
                 
                   
                     ( 
                     
                       h 
                       2 
                     
                     ) 
                   
                    
                   
                     ( 
                     
                       b 
                       2 
                     
                     ) 
                   
                    
                   
                     ( 
                     
                       
                         h 
                         2 
                       
                       2 
                     
                     ) 
                   
                 
               
               = 
               
                 
                   [ 
                   
                     
                       
                         ( 
                         
                           h 
                           1 
                         
                         ) 
                       
                        
                       
                         ( 
                         
                           b 
                           1 
                         
                         ) 
                       
                     
                     + 
                     
                       
                         ( 
                         
                           h 
                           2 
                         
                         ) 
                       
                        
                       
                         ( 
                         
                           b 
                           2 
                         
                         ) 
                       
                     
                   
                   ] 
                 
                  
                 
                   y 
                   _ 
                 
               
             
           
         
       
       
         
           
             
                 
             
              
             
               y 
               = 
               
                 
                   
                     
                       ( 
                       
                         h 
                         1 
                       
                       ) 
                     
                      
                     
                       ( 
                       
                         b 
                         1 
                       
                       ) 
                     
                      
                     
                       ( 
                       
                         
                           h 
                           1 
                         
                         + 
                         
                           2 
                            
                           
                             h 
                             2 
                           
                         
                       
                       ) 
                     
                   
                   + 
                   
                     
                       
                         ( 
                         
                           h 
                           2 
                         
                         ) 
                       
                       2 
                     
                      
                     
                       ( 
                       
                         b 
                         2 
                       
                       ) 
                     
                   
                 
                 
                   Z 
                    
                   
                     [ 
                     
                       
                         
                           ( 
                           
                             h 
                             1 
                           
                           ) 
                         
                          
                         
                           ( 
                           
                             b 
                             1 
                           
                           ) 
                         
                       
                       + 
                       
                         
                           ( 
                           
                             h 
                             2 
                           
                           ) 
                         
                          
                         
                           ( 
                           
                             b 
                             2 
                           
                           ) 
                         
                       
                     
                     ] 
                   
                 
               
             
           
         
       
       
         
           
             
                 
             
              
             
               
                 I 
                 
                   
                       
                     x 
                   
                    
                   1 
                 
               
               = 
               
                 
                   
                     ( 
                     
                       I 
                       
                         
                             
                           x 
                         
                          
                         1 
                       
                     
                     ) 
                   
                   1 
                 
                 + 
                 
                   
                     ( 
                     
                       I 
                       
                         
                             
                           x 
                         
                          
                         1 
                       
                     
                     ) 
                   
                   2 
                 
               
             
           
         
       
       
         
           
             
               
                 
                   I 
                   
                     
                         
                       x 
                     
                      
                     1 
                   
                 
                  
                 
                   { 
                   
                     
                       
                         ( 
                         
                           1 
                           12 
                         
                         ) 
                       
                        
                       
                         ( 
                         
                           b 
                           1 
                         
                         ) 
                       
                        
                       
                         
                           ( 
                           
                             h 
                             1 
                           
                           ) 
                         
                         3 
                       
                     
                     + 
                     
                       
                         ( 
                         
                           b 
                           1 
                         
                         ) 
                       
                        
                       
                         
                           
                             ( 
                             
                               h 
                               1 
                             
                             ) 
                           
                            
                           
                             [ 
                             
                               
                                 h 
                                 2 
                               
                               + 
                               
                                 
                                   ( 
                                   
                                     h 
                                     1 
                                   
                                   ) 
                                 
                                 2 
                               
                               - 
                               y 
                             
                             ] 
                           
                         
                         2 
                       
                     
                   
                   } 
                 
               
               + 
               
                 { 
                 
                   
                     
                       ( 
                       
                         1 
                         12 
                       
                       ) 
                     
                      
                     
                       ( 
                       
                         b 
                         2 
                       
                       ) 
                     
                      
                     
                       
                         ( 
                         
                           h 
                           2 
                         
                         ) 
                       
                       3 
                     
                   
                   + 
                   
                     
                       ( 
                       
                         b 
                         2 
                       
                       ) 
                     
                      
                     
                       
                         
                           ( 
                           
                             h 
                             2 
                           
                           ) 
                         
                          
                         
                           [ 
                           
                             y 
                             - 
                             
                               
                                 ( 
                                 
                                   h 
                                   2 
                                 
                                 ) 
                               
                               2 
                             
                             - 
                             y 
                           
                           ] 
                         
                       
                       2 
                     
                   
                 
                 } 
               
             
              
             
               
 
             
              
             
               
                 
                     
                 
                 _ 
               
               _ 
             
           
         
       
     
         [0096]    With these equations, one can calculate and compare the predicted stiffnesses of beams with any particular number of grooves and thicknesses or cross-sectional areas. If the material is defined, then comparing composite/total I values (or I total  values) will be sufficient. 
       EXAMPLE 1 
     Determination of Moment of Inertia (Second Moment) of the Cross-Sectional Area of a Grooved Nasal Dilator 
       [0097]    Using the equations above, the values of the nasal dilator configuration shown in  FIG. 9   a  yields the values shown in Table I: 
         [0000]    
       
         
               
               
               
               
               
               
               
               
               
               
               
               
             
           
               
                 TABLE I 
               
               
                   
               
               
                   
                   
                   
                   
                   
                   
                   
                   
                   
                   
                   
                 P test   
               
               
                 L 
                 b 1   
                 h 1   
                 b 2   
                 h 2   
                 
                   y 
                 
                 I 1   
                 ΔI 1   
                 I 2   
                 ΔI 2   
                 I total   
                 Actual 
               
               
                 mm 
                 mm 
                 mm 
                 mm 
                 mm 
                 mm 
                 mm 4   
                 mm 4   
                 mm 4   
                 mm 4   
                 mm 4   
                 gm 
               
               
                   
               
             
             
               
                 60 
                 3.34 
                 0.216 
                 10.00 
                 0.254 
                 0.179 
                 0.0028 
                 0.0174 
                 0.0137 
                 0.0069 
                 0.0408 
                 64.0 
               
               
                   
               
             
          
         
       
     
         [0098]    The loading goal for a nasal dilator having a length of 46 mm is about 27 grams. The proportional I total  to achieve this on a nasal dilator having a length of 46 mm is about 0.0171 mm 4 . 
         [0099]    Table II shows some calculated values. The first row represents a ridge height, English units, of 0.0012 inch and a base or valley thickness of 0.0035 inch. The second row shows a trial reduction of the grooves from 33% of the width to 30%. The third row shows instead a reduction of the ridge height from 0.012 inch to 0.0105 inch. Since neither resulted in an I total  near 0.171 mm 4 , both changes were employed, yielding I total  of 0.0173 in 4 . The proportional load predicted on a nasal dilator having a length of 46 mm with this I total  is about 27.2 grams. 
         [0000]    
       
         
               
               
               
               
               
               
               
               
               
               
               
               
             
           
               
                 TABLE II 
               
               
                   
               
               
                   
                   
                   
                   
                   
                   
                   
                   
                   
                   
                   
                 P test   
               
               
                 L 
                 b 1   
                 h 1   
                 b 2   
                 h 2   
                 
                   y 
                 
                 I 1   
                 ΔI 1   
                 I 2   
                 ΔI 2   
                 I total   
                 Predicted 
               
               
                 mm 
                 mm 
                 mm 
                 mm 
                 mm 
                 mm 
                 mm 4   
                 mm 4   
                 mm 4   
                 mm 4   
                 mm 
                 gm 
               
               
                   
               
             
             
               
                 46 
                 3.34 
                 0.305 
                 10.00 
                 0.089 
                 0.150 
                 0.008 
                 0.009 
                 0.0005 
                 0.010 
                 0.0271 
                 42.6 
               
               
                 46 
                 3.00 
                 0.305 
                 10.00 
                 0.089 
                 0.144 
                 0.007 
                 0.008 
                 0.0006 
                 0.009 
                 0.0244 
                 38.3 
               
               
                 46 
                 3.34 
                 0.267 
                 10.00 
                 0.089 
                 0.134 
                 0.005 
                 0.006 
                 0.0006 
                 0.007 
                 0.0192 
                 30.2 
               
               
                 46 
                 3.00 
                 0.267 
                 10.00 
                 0.089 
                 0.129 
                 0.005 
                 0.006 
                 0.0006 
                 0.006 
                 0.0173 
                 27.2 
               
               
                   
               
             
          
         
       
     
         [0100]    There are many configurations (b&#39;s and h&#39;s) that can yield the desired I. This is one example of the iterative approach to finding a configuration that also meets other design and processing criteria. 
         [0101]    In the embodiment of the present invention shown in  FIG. 9   a , the total thickness=R 0 +R i , where R 0  is the thickness of the base or valley of the groove, and R i  is the thickness of the ridge of the groove. The valley width is defined in this embodiment to be about half the width of the ridges. The stiffness of the nasal dilator will be an addition of the component related to R 0  plus the component related to R i  The base or valley width can be defined simply as the entire width of the lifting portion of the bracket. 
         [0102]    The polymer material can be extruded as shown in  FIG. 6   a  at a temperature of about 400° F., under a pressured nip roller, at a rate of about 25 feet/minute, then laminated with an adhesive material and a release layer as shown in  FIG. 6   b , at a temperature ranging from about 180° F. to 215° F., through a pressured nip roller, and at a rate of 25 feet/minute. After the laminated material leaves the extruder, it can be subjected to further processing, such as laser cutting, to form nasal dilators having the desired size and shape. 
         [0103]    Preferably, the adhesive material is applied to the grooved surface of the material, so that adhesive can be applied within each groove. In one embodiment, the adhesive is applied to partially or substantially fill the grooves. In another embodiment, the adhesive is applied to only the top portions of the grooves. 
         [0104]    As described herein, any suitable adhesive material may be used, such as acrylate-based adhesives or hydrocolloid adhesives. The amount of adhesive material applied will vary depending on the dimensions of the grooves and the type of adhesive material or materials used. For example, in one embodiment of a nasal dilator of the present invention, each groove is filled with about a 10 mil thick layer of adhesive, such as a rubber-based adhesive. 
         [0105]    For a nasal dilators without a central opening, such as those shown in  FIGS. 9   a - c,  preferably the length of the nasal dilator may range from between about 35 mm to about 60 mm, the width may range from about 10 mm to about 25 mm, the valley thickness may range from between about 3 mil to about 10 mil, and the ridge thickness may range from between about 8 mil to about 15 mil. In one preferred embodiment, the ridge thickness was about 14 mil, the valley thickness was about 3.5 mil, and the total thickness of the ridge plus the valley thicknesses was about 17.5 mil. 
         [0106]    For nasal dilators with a central opening, and two lifting brackets, such as the nasal dilator shown in  FIG. 11 , the length may range from between about 40 mm to about 55 mm and the width may range from between about 25 mm to 30 mm, with the same ranges for the ridge and valley thicknesses described above. 
         [0107]    As noted previously, the valley width is preferably about half of the ridge width. In one preferred embodiment, the ridge width and valley width each range from between about 0.5 mm to about 1.0 mm, although these values can change depending in part on the material being used and the desired stiffness of the extruded material. The ratio of valley width to ridge width may also vary, again, depending in part on the material used and the desired stiffness of the extruded material. 
         [0108]    The grooved and laminated material for nasal dilators can be laser cut to provide nasal dilators having the desired size and shape. In addition, the edges of the cut material can be further processed to increase comfort and ease of use. Preferably, the stiffness of the edges is reduced by about 85% compared to the center portions of the material. In one preferred embodiment, the edges are reduced from 14 mil to 4 mil in thickness. In another preferred embodiment, the edges are reduced to about 2 mil to 3 mil in thickness. 
         [0109]    The size, shape and stiffness of nasal dilators made as described above were suitable for comfortably lifting the tissues of the nasal passages for a desired period of time. 
         [0110]    In another embodiment of a nasal dilator made in accordance with the present invention, rather than embedding adhesive material within each groove, a thin layer of adhesive is applied to the top of one or more ridges of the grooves. For example, one or more ridges can be coated with about a 0.5 mil thick layer of adhesive, such as an acrylate adhesive. 
         [0111]    In this embodiment of a nasal dilator, because only the top of the ridge or ridges is in contact with and adhered to the user&#39;s skin, there will be a partially or substantially open channel between the groove and the user&#39;s skin, running longitudinally from one end of the dilator to the other, or from one end of the dilator to another location along the length of the dilator. The plurality of channels can alternatively criss-cross to form a “dimpling” to the surface of the nasal dilator in contact with the user&#39;s skin. The adhesive is applied to only the top most “islands” or ridge junctions created by the criss-crossing channels. 
         [0112]    The channel or plurality of channels permit gases, fluids or liquids, such as water, air, oil or perspiration, to enter or collect in the channel, under the nasal dilator. The channel or channels may therefore increase the user&#39;s comfort when wearing the nasal dilator by permitting the evaporation of accumulated body moisture out of the channels, or by providing a reservoir in which oil secreted from the user&#39;s skin can accumulate away from the skin&#39;s surface. 
         [0113]    The channel or channels may additionally or alternatively make it easier to remove the nasal dilator, by permitting water to enter the channel or channels when the user applies water to his or her face to remove the nasal dilator. When water is flushed into the space within the channels under the nasal dilator, air can then escape from under the dilator in any direction as determined by the position of the channel or channels. The channel or channels help facilitate the removal of the nasal dilator by increasing the surface area under the nasal dilator that can be put in contact with water, thereby deactivating more of the adhesive in contact with the user&#39;s skin. 
       Packaging Materials 
       [0114]    As described above, the present invention can be used to make packaging materials having improved handling properties. Specifically, it has been surprisingly discovered that by using the grooved material described herein, package opening regions can be created which require far less force to tear apart, and have no sharp or irregular edges, as commonly associated with plastic packaging, such as PVC clamshell packaging. In one embodiment, it is possible to reduce the force required to open the package by about 98% using the grooved material of the present invention. 
         [0115]    The use of the grooved material as packaging can reduce the amount of resin needed, in some cases by about 15% to 20%, thereby reducing the cost and environmental impact of the packaging. The grooved material surprisingly does not exhibit a reduction in blunt force resistance under compression as compared to the same material in an ungrooved form. The grooved material maintains its resistance to tearing across the grooves as compared to the ungrooved material, but by initiating a cut or notch along a groove, the grooved material can be torn apart safely and easily, as shown in  FIG. 17 . 
         [0116]    The grooved material may also provide regions of improved flexibility, making it suitable for bending into a box or other shape. 
         [0117]    The grooved material can be made more optically appealing, comparable to a “clear plastic” packaging material, by varying the cross-sectional appearance of the grooves, such as a “V” shaped groove rather than a squared groove. In addition, it may be possible to polish the etched roller&#39;s channel to remove the acid etch matte finish in the grooves to reduce the opacity of the material, making it more transparent. 
         [0118]    The channels or valleys in the grooved material can be used to transfer fluids or gases into or out of a package or from one end of the channel to the other. 
         [0119]    The grooved material can be covered with a second film to create a fluted plastic “cardboard-like” material for greater rigidity. Open-ended fluted corrugated plastic has not been readily used in medical or agricultural applications due to the possibility of entrapping dirt or unwanted biological materials. The present invention can be used to imprint closed, transverse brackets into the web of material, in either a repeatable design or at random. These closed brackets function by closing off the fluted ends of the material, thereby eliminating the possibility of dirt or biological contamination. 
       Medical Uses 
       [0120]    In addition to the medical packaging application described above, the grooved material of the present invention can be used as a supportive material in a cast or splint. The grooved material can be rolled around an extremity, then scored and cut to size. The ability of the material to be easily cut to size makes it suitable for use in triage, emergency or battlefield situations. Again tackifiers such as polybutene, can be added to allow the material to attach to itself after reflecting back over a digit or extremity and on to itself. The channel or channels created by the grooves permit the transmission of gases, fluids or liquids, such as water, blood, oil or perspiration, into or out from under the grooved material in contact with the wearer&#39;s skin. 
       Construction Materials 
       [0121]    The grooved material of the present invention can be used to make construction materials, such as flooring, or as sheeting material for containment purposes. 
         [0122]    One example of a type of flooring that can be made with the present invention is linoleum flooring. The grooves can be made into flutes (as mentioned above) in the material and can facilitate the passage of warmed liquids or gases to heat or cool flooring. 
         [0123]    Current containment sheeting is very difficult to handle on site to position and size appropriately. The grooved material of the present invention permits unrolling the material along a surface, such as a wall or floor, to the desired size, then scoring and tearing the material along a groove. 
         [0124]    The grooved material can include polybutene or similar adhesive to provide the material with a degree of tackiness or stickiness to facilitate its use. 
         [0125]    Anti-microbial agents, such as anti-fungal or anti-spore treatment compounds, can be added to the web of material for use in situations in which moisture damage needs to be controlled. Other applications include the use of the grooved material to set up or contain designated “clean rooms”. 
         [0126]    Insect repellant agents can be added to the material for use in infested areas, either as temporary shelter, or as part of a permanent structure. Examples include DEET, Permethrin, or Picaridin. 
         [0127]    Although the foregoing examples and embodiments describe various aspects and applications, they are not intended to limit the scope of the present invention, which is set forth in the following claims.