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PATENT APPLICATION  
       [0001]     This is a continuation in part of application Ser. No. 10/198,369 (Shock Wave Absorber), and Ser. No. 10/198,369 (shock Wave Absorber), inventor Eric Schmidt. 
     
    
     NO FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT  
     NO INCORPORATION-BY-REFERENCE MATERIALS ARE INCLUDED WITH THIS APPLICATION  
     BACKGROUND OF THE INVENTION  
       [0002]     Air resistance provides a formidable barrier to objects moving at high rates of speed. There have been numerous efforts to minimize the effects of moving air over and around a cylindrical body. It is not only the air that must be pushed aside in order for the body of a cylindrical object to move freely through the air, but air resistance and drag may also be caused by turbulence against the outer skin of a cylindrical body, which diminishes aerodynamic design benefits. When considering the reduction of drag on a leading edge of a moving object, the shape and configuration of the foremost section of the leading edge, is an important aspect to minimizing the resistance of the air of fluid moving around said leading edge.  
         [0003]     Allowing a smooth air airflow around a surface area is well-recognized as a means to reduce drag. For example, in U.S. Pat. No. 4,989,807 (Foreman et al.), the injection of an airflow in the bent portion of an s-shaped air intake allows the airflow to be uniform and minimizes pressure drops within the air intake duct. This is a result of the circulating effect of air between the airflow and the inner walls of the duct, where the injected air actually provides a cushion between the high rate of flowing air and the duct wall.  
         [0004]     High speed projectile technology for items moving through water have encompassed the idea that the shape of the nose may be done in a manner so as to provide a cavitation bubble around the body of the projectile so as to reduce hydro-dynamic drag. This is example in U.S. Pat. No. 5,955,698 (Harkins et al.).  
         [0005]     U.S. Pat. No. 4,522,357 (Bains et al.) And U.S. Pat. No. 4,573,648 (Morenus et al.) examples an attempt to take advantage of the air moving around a high-speed object for purposes of guidance. In this invention, an air inlet is provided in the nose of a missile, where the air moving through the air inlet is directed to a specific outlet port that assists in guiding the missile.  
         [0006]     U.S. Pat. No. 3,995,558 (Travor et al.) examples the type of effort given to use an air intake having an inlet port and outlet ports where onrushing air is allowed to move through the nose down in such a manner that will provided a laminar boundary area of air between the body of the object and the air it is moving through. This cuts down on overall resistance. The ports themselves allow air to be projected rearward along the sides of the object, and attempt to provide a secondary cushion of air between the atmosphere and the skin of the object.  
         [0007]     A recent usage of cavities on the leading edge of airplane wings, and/or propellers, is disclosed in U.S. Pat. No. 5,836,549 (Bushman), in which a cylindrical cavity is defined along the forward edge of a wing or propeller. The cavity is intended only for supersonic speeds, and does not rely on any defining characteristics of using sine wave formation to define the shape and structure of the linear cavity as the present invention does. The Bushman patent utilizes what is effectively half of a cylinder volume to define their cavity, and only disclose a cavity wall that follows a uniform arcual curvature. The present invention defines an open mouth that defines an opening to a cavity within the structure itself, whose circumference exceeds the opening itself. The present cavity is useful for slower speeds, as well as for usage in water and other liquids. Also, the present invention takes advantage of possible multiple cavities, which are neither disclosed or alluded to in the Bushman patent.  
         [0008]     The present invention does not use a separate air outlet, but uses the shape of a linear cavity to cause fluid or gas moving toward it to be redirected outward, so as to create a central high pressure ridge that projects outward from the opening of the linear cavity. This ridge, or what may also be considered a linear pressure spike directs oncoming air around the body of the leading edge.  
         [0009]     Prior art does not teach the use of a pressure spike to direct oncoming air flow, nor does it teach multiple chambers, which may be used to encourage rapid creation of the pressure spike within the largest or primary chamber. This also prevents the pressure spike from rapidly dissipating during movement through the air. The cavities defined in this invention are also useful with regard to movement through air or any gas, as well as through water or any liquid, since the cavity chamber can provide a liquid pressure spike that allows the liquid in front of the nose of the object moving through the water more easily as the spike causes a cavitation ridge and stationary liquid such as water is able to be directed around the body of the object.  
       BRIEF SUMMARY OF THE INVENTION  
       [0010]     The wings of aircraft, propellers, bridge supports, and other linear objects encounter resistance as a result of the difference in relative speed between the object and the gas or liquid through which it is moving, or where the gas or liquid is moving around it. Since the object must effectively move a portion of the gas or liquid around it as the gas or liquid moves past it, the gas or liquid creates drag as a result of the friction of the air against the outer skin of the object, but particularly against the leading edge of the object, such as the front edge of a wing, or the portion of a bridge support that is presented toward onrushing water. Certain amounts of drag can be reduced through aerodynamic design, but there exists a continuing problem with how best to direct gas or liquid initially at the front leading edge of the object so as to reduce friction.  
         [0011]     This invention incorporates a linear cavity that is defined in the forward portion, also referred to as the front leading edge of the object, with said cavity defining an interior that is conducive to causing air to rotate within said cavity. Gas or liquid enters into the cavity as a direct result of the object&#39;s relative movement through the air. The gas or liquid enters initially as a result of an increase in pressure against the opening of the cavity as the object moves forward. Typically, this increase in pressure is along the length of the leading edge in a fairly uniform manner. As the relative speed of the object increases, a greater quantity of gas or liquid will be forced into the mouth of the cavity along its length. The shape of the cavity causes the gas or liquid moving against the wall of said cavity to encourage a linear rotation within said cavity. The rotation in a three-dimensional model causes a central ridge or central linear node of increased pressure, where said central node of increased pressure will be significant enough to cause gas or liquid in the central node to be expelled out of the mouth of the cavity along its length, creating a protruding linear pressure ridge or node.  
         [0012]     The air that is expelled out of the cavity creates a pressure ridge that extends forward of the object. The distance of the extension of the pressure ridge is dependent on the speed of the object relative to the media though which it has a differing relative speed, and to the configuration of the cavity creating said pressure ridge.  
         [0013]     The protruding pressure ridge causes the gas or liquid to begin to be redirected so as to move around the body of the object before it has a chance to physically impact the outer skin of the leading edge of the object. This reduces drag on the front part of the object, since the previously redirected gas or liquid has less turbulence caused by the object itself, as it begins to move around the object. The turbulence is lessened further by the pressure ridge which modifies the direction of air relative to the object using relative pressure differentials, as opposed to a physical barrier such as the outer skin of the object. Gas or liquid moving around the ridge or leading edge of the object has a significant drop in turbulence, which likewise reduces the overall drag.  
         [0014]     The optimal shape of the cavity is dependent on the medium through which the object is traveling. Water presents a different criteria than does air, since the mass of the water is greater than the air, and the relative speed of the object through water is generally lower than the relative speed of an object through the air. Airborne objects encounter atmospheric pressure differentials at various altitudes, and this may also play a factor in determining the optimal cavity configuration. For example, an object intended to move at high altitudes with greater speed than an object at lower altitudes, will have different optimal cavity configurations. Objects in the water will exhibit a protruding wave ridge, in some aspects similar to the pressure wave ridge provided by the bow of a moving boat.  
         [0015]     The cavity is defined by an opening centrally located on the leading edge of an object such as a wing or leading edge of a flap, propeller edge, support, pylon, or other similar structure. This would typically be a wing, or other support means, having a length that also defines a flattened side edge. The cavity itself is a linear trough, and generally spherical in design when viewed from a cross sectional viewpoint. The walls of the cavity may define a single linear cavity, having curved side walls, as well as multiple linear cavities, where the successive cavities are connected to each other. In this situation, the forwardmost cavity comprises the cavity with the largest volume, and where the back wall of the forwardmost cavity defines an opening that leads into a successive cavity having similar shape, but which is greatly reduced in size and volume as compared to the forwardmost cavity.  
         [0016]     Where multiple cavities are provided, the initial cavity is preferably the largest in maximum circumference, with the successive cavities having a reduced circumference in relation to the successive status of the particular cavity.  
         [0017]     The walls of the cavities, where multiple cavities are arranged from the largest to the smallest, the side walls preferably follow a diminishing sine wave orientation, when describing the side walls of the cavity in a cross-sectional orientation view. The sine wave comprises a wave form contained within a particular set of radii, where said radii have an angle in relation to a central zero degree vector. The zero degree vector preferably runs through the center of the object body from forward to aft, and defines the center point of each cavity defined within the object body.  
         [0018]     While the walls of the cavity, when viewed from a cross sectional viewpoint, may define a single spherical shape. Multiple cavity walls follow a diminishing sine wave configuration. Therefore, multiple cavities may comprise two successive cavities, three successive cavities or more depending on the sine wave configuration used.  
         [0019]     Successive cavities assist in promoting the rotational configuration in the cavity before it. The successive cavity operates in a similar manner as does the primary or foremost cavity, so that when a pressure ridge or node extends out of the secondary cavity, it will assist in promoting rotation of the air in the primary cavity, with a pressure node encouraged to develop outward through the opening.  
         [0020]     Cavities may be defined on both the forward and aft ends of the object, and the cavities themselves may all be connected to each other through a vent defined between the forward and aft cavities.  
         [0021]     It is an object of this invention to provide a means for reducing drag on a length of an object that contacts moving gas or liquid, whereby a high pressure node is projected outward from the forward portion along the length of the object that is intended for rapid movement through gas or liquid.  
         [0022]     It is a further object of this invention to provide a means whereby a primary cavity has a secondary cavity situated therein, where the secondary cavity assists in the rotation of gas or liquid within the primary cavity, to rotate and form a central high pressure node that functions as a high pressure ridge along the length of the cavity.  
         [0023]     It is a further object of this invention to provide a means whereby a modified leading edge, having a defined cavity, can be substituted on existing aircraft, missiles, or any other airborne or underwater objects that require higher levels of speed with reduced drag.  
         [0024]     It is a further object of this invention to provide a means whereby a leading edge of an object can provide a forward projecting pressure node on a land vehicle, such as an automobile.  
         [0025]     It is a further object of this invention to provide a means whereby a leading edge of an object can provide a forward projecting pressure node using a linear cavity, where the pressure node reduces turbulence for either stationary objects such as bridge supports, or on a land vehicles, such as automobile ends.  
     
    
     DESCRIPTION OF THE DRAWINGS  
       [0026]      FIG. 1  is a perspective view of typical linear object, having a leading edge, intended for rapid movement through air or water.  
         [0027]      FIG. 1   a  is a cross sectional view of the linear object shown in  FIG. 1 , having a defined primary and secondary cavity with the direction of airflow through the cavity and around the nose cone shown, where a central higher pressure node is created projecting the high-pressure node forward of the leading edge.  
         [0028]      FIG. 2  is a cross sectional view of the typical linear object intended for rapid movement through air or water, as depicted in  FIG. 1 .  
         [0029]      FIG. 2   a  is a cross sectional view of the leading edge of the linear object depicted in  FIG. 1 , where the leading edge is moving at a lower speed relative to water and/or atmosphere, with the airflow or water flow into the cavity being at a lower rate than that shown in  FIG. 1 .  
         [0030]      FIG. 3  is a cross sectional view of a leading edge having a single primary cavity, with the gas or water flow is a low rate, prior to a central high-pressure node being created within the cavity.  
         [0031]      FIG. 4  is a cross sectional view of the leading edge, as shown in  FIG. 3 , where the leading edge is moving at a higher rate of speed and the flow of water or atmosphere through the cavity is sufficient to create a high pressure node in ridge of the leading edge.  
         [0032]      FIG. 5  is a cross sectional view of a leading edge depicting the flow of air, or water into the cavity with the high pressure node indicated as an elongated triangle that protrudes forward out above the cavity mouth.  
         [0033]      FIG. 5   a  is a perspective view of  FIG. 5 .  
         [0034]      FIG. 6  is a cross sectional view of the leading edge in which the moving air and/or water has not yet entered the cavity.  
         [0035]      FIG. 7  is a cross sectional view of the leading edge in  FIG. 6 , in which the moving air and/or water is being diverted through a projecting high pressure node.  
         [0036]      FIG. 8  is an example of a diminishing sine wave.  
         [0037]      FIG. 9  is an example of a diminishing sine wave, having an angle of magnitude greater than the sine wave in  FIG. 8 .  
         [0038]      FIG. 10  is a cross sectional view of a leading edge having multiple cavities, in which the walls of the cavities are defined through the sine wave as shown in  FIG. 8 .  
         [0039]      FIG. 11  is a cross sectional view of a leading edge having multiple cavities, in which the walls of the cavities are defined through the sine wave as shown in  FIG. 9 .  
         [0040]      FIG. 12  is a cross sectional view of a leading edge having multiple cavities forward and aft, where the cavities are connected by a single vent.  
         [0041]      FIG. 13  is a perspective view of an object such as a bridge support, having a cavity that causes a pressure node to extend forward of the cavity, where the cavity is linear rather than spherical.  
         [0042]      FIG. 14  is a cross sectional view of the object shown in  FIG. 13 .  
     
    
     DETAILED DESCRIPTION OF THE INVENTION  
       [0043]     Referring now to  FIG. 1 , a perspective view of a leading edge  10 , where said leading edge  10  comprises a typical wing, pylon strut, or propeller. The leading edge  10  defines a back end  11 ′, and a front end, where said front end comprises a mouth  48  that is defined as to opening size by an upper  47  lip and a lower  46  lip. The cavity  20  has a depth that exceeds the mouth opening size  48 , and an internal circumference that also exceeds the size of the mouth  47 . The typical forward edge of a wing is shown by dashed lines  49 .  
         [0044]     The dimensions of the cavity are further shown in  FIG. 1 , in which the measurable depth  43  of the cavity  20  exceeds that of the vertical height  44  of the cavity  20 , and where both the depth  43  and height  44 , exceed the space defined between the upper lip  47  and lower lip  46 . It should be understood that the defining words regarding vertical and depth, when referring to the cavity  20 , are being used with the orientation as shown in  FIG. 1  through  FIG. 12 , which is the most common anticipated orientation. Where the leading edge  10  is orientated perpendicular, as shown in  FIG. 13 , the cavity  20  is also orientated perpendicular, however the terminology will still apply, if the cavity  20  is referenced in the same orientation as the rest of the Figures.  
         [0045]     Referring now also to  FIG. 15 , the height  44  is greater than the depth  43 , defined within the cavity  20 . This does not follow the sine wave formation described below, but is an alternative structural design that may be usable with different relative speeds of gasses and/or liquids.  
         [0046]     Referring to  FIG. 2 , a perspective view of the cavity  20  is shown. The cavity  20  would extend virtually the entire length of the forward leading edge of the wing, or other structure. Referring now to  FIG. 6 , a typical leading edge  10  is shown, with the direction of air in relation to the leading edge  10  also shown. It should be understood that reference to air and water are interchangeable with regard to the scope of this invention. This invention was intended for use on objects that are to move efficiently through air and/or water. Therefore, the terminology directed toward air should be understood to mean water as well. The term gas is also interchangeable with liquid.  
         [0047]     As  FIG. 6  shows, air directly in ridge of the leading edge  10  moves directly against the ridge leading edge of the leading edge  10 . The leading edge skin  11  comprises the outer surface of the leading edge  10 . As the moving air  81  impacts the leading edge of the leading edge skin  11 , it is pushed to one side as a result of the physical impact of the leading edge skin  11 . Redirected air  81  goes along the surface of the skin  11  following route  83 . Air moving in close proximity to the skin  11  will react by creating some turbulence, which dramatically increases drag. Air  83  acts somewhat as a buffer in  FIG. 6  between moving air  82  and skin  11 .  FIG. 6  shows a cavity  20 , but the interaction of the air within said cavity  20  is not depicted in  FIG. 6 .  
         [0048]      FIG. 7  depicts the same leading edge  10  as shown in  FIG. 6 . The cavity  20  is again depicted, but the movement of the air within the cavity  20  is further described below.  FIG. 7  depicts a protruding high pressure node  55 , comprising an area of air or water that has a higher pressure then the air or water around it. The difference in the effects of the existence of the high pressure node  55  are clearly seen in the different pathways the moving air takes. Moving air  81  now contacts the high-pressure node  55  in ridge of the leading edge  10 , and is redirected as flow  83 . The air flow  83  is not modified as to direction of flow by the skin  11  of the leading edge  10  as significantly in  FIG. 7  as it is in  FIG. 6 . The air flow  83  will have less turbulence in the configuration shown in  FIG. 7 , as compared to a leading edge  10  without a protruding high pressure node  55 . Therefore, the benefits of this invention are realized when the relative difference in speed between the leading edge  10  and the air  81  becomes significant enough to create a high pressure node  55 .  
         [0049]     Referring now to  FIG. 3  and  FIG. 4 , a leading edge  10  is shown, and having a similar configuration to that shown in  FIGS. 1   a  and  2 . The cavity  20  is showing its most basic form, comprising a generally spherical shape that is slightly elongated as defined by the cavity wall  21  and where a circular mouth  22  defines the opening into the cavity  20 .  
         [0050]     As shown in  FIG. 3 , some of the air  81  moves into the cavity  20 , while other air  82  and  83  is directed around leading edge  10 . As air  81  moves into the cavity  20 , the configuration of the cavity  20  will cause the air to begin to rotate as the air moving along the walls  21  of cavity  20  is forced to move from the outer area towards the central area the cavity  20 . As the air begins to rotate, it will follow the circular rotational path  84 . At this point, the movement of air within the cavity  20  has not yet had an opportunity to create a high-pressure node. Redirected air  82  continues to move past the leading edge  10  with air path  83  providing a turbulent buffer as it is compressed against the skin  11 .  
         [0051]     As the relative speed of the air and leading edge  10  increase in relation to each other, a higher pressure area or node is formed by the air  81  as it enters the cavity  20 . The air pathway  81  follows the cavity wall  21  so that a circular rotation pathway  84  develops, and where all rotation pathways  84  meet, a node of higher pressure is created, and the air pathway  85 , having a higher pressure than air existing outside the cavity  20 , air pathway  85  will be pushed out of the cavity  20 , exiting centrally through the circular mouth  22 . The exiting air  85  briefly exhibits a pressure ridge node that extends forward of the mouth  22  of cavity  20 . This causes a pressure projection that redirects air around the leading edge  10 , following pathway  83 , of the area of redirecting air and accomplished forward of the leading edge  10 , so that redirected air  83  is subject to less turbulence and pressure against the skin  11  of leading edge  10 .  
         [0052]     Referring now also to  FIG. 5 , a pressure node  55  is shown, in relation to the cavity  20  and the cavity mouth  22 . As is shown in  FIG. 5 , the pressure node  55  projects forward of the leading edge  10 , in providing a wedge which causes oncoming air to be diverted.  FIG. 5  also shows a secondary cavity  30 , which will be discussed in detail below.  
         [0053]     As  FIG. 5   a  shows, a pressure node  55  extends along the length of the cavity  20 . This pressure node  55  is in the general form of a wedge, and defines a protruding ridge at its most forward point  45 . If the cavity  20  extends along the length of the structure, said cavity  20  will provide a pressure node  55  along the same length of the structure.  
         [0054]     In some instances, a better shaped wedge, being the increased pressure node  55 , is enhanced through the use of a secondary cavity  30 , which assists in redirecting the rotational air  84  toward a central high pressure node area  55 .  FIG. 2   a  shows a leading edge  10  that has a primary cavity  20 , with the rear most portion of its cavity wall  21  defining a secondary cavity mouth  32 , which allows access into a cavity  30  having similar dimensions, but on a smaller scale than the primary cavity  20 . Pressurized air  81  enters the primary cavity  20 , and moves along the walls  21 , with the air beginning to rotate along lines  84 . Some of the air flow along lines  84  are able to move through the secondary mouth  32  following air flow  86 . The secondary cavity  30  has similar dimensions as the primary cavity  20 , and the airflow  86  will be directed along the secondary walls  31  to a central pressure point.  
         [0055]     Referring now also to  FIG. 3 , the air flow  86  in the secondary chamber is forced to meet at a central pressure point, with the air pathway  87  directed back out centrally through the mouth  32  to form a small pressure node that protrudes into the confines of the primary cavity  20 . The secondary pressure node area  88  causes air pathway  84  to more easily converge with other similar air flow paths to form a higher pressure area pathway  55  that is directed out of the cavity  20  and forward of the leading edge  10 . Referring also again to  FIG. 5 , the secondary cavity may be quite small in comparison to the primary cavity  20 , or may be larger in relation, as shown in  FIG. 1   a  and  FIG. 2   a.    
         [0056]     The side walls of multiple cavities are defined using a diminished sine wave configuration. Referring now to  FIG. 8  and  FIG. 9 , diminished sine waves are shown, in which the sine wave  60  follows a mathematical trajectory. For example, using axis x  65  and axis y  61 , the diminished sine wave  60  will follow a diminishing wave amplitude where the magnitude of x will be zero at point  63 .  
         [0057]     The diminished sine wave  60  in  FIG. 8  is shown where the angle  64  of maximum wave height is approximately 15 degrees from the y axis  61  to the angled limitation  62 , so that the total degree for the maximum wave height is twice that of angle  64 , or approximately 30 degrees.  
         [0058]     The diminished sine wave  60  in  FIG. 9  is shown where the angle  65  of maximum wave height is approximately 22.5 degrees from the Y axis to the angled limitation  62 , so that the total degree for the maximum wave height is twice that of angle  65  or approximately 45 degrees.  
         [0059]     Referring now to  FIG. 10 , in which a diminishing sine wave  60  is used to define the structure of the cavity walls in a multiple cavity situation, the sine wave configuration shown in  FIG. 8  is seen in the side walls  21 ,  31  and  41  or cavities  20 ,  30  and  40 .  FIG. 10  depicts the use of a diminishing sine wave  60 , as used in  FIG. 8 , to define the wall  21 ,  31 ,  41  configuration, where the diminishing sine wave in both Figures decreases in amplitude of x axis  65  along the y axis  61  to point  63 .  FIG. 11  shows the wall configuration for cavity walls  21 ,  31 , and  41  where a diminishing sine wave, having a greater reduction in amplitude of the x axis  65  along the y axis  61  to point  63  is used. As  FIG. 10  shows, a diminishing sine wave  60  with a smaller angle causes multiple cavities  20 ,  30  and  40  to be elongated, as compared with the diminishing sine wave  60  having a larger angle, as shown in  FIG. 11 , where the multiple cavities  20  and  30  are not defined as far along the length of the leading edge  10 .  
         [0060]      FIG. 8  depicts a diminishing sine wave  60 , where the angle of maximum wave height is contained within an angle  65  of 22.5 degrees.  
         [0061]     Use of multiple cavities is also shown in  FIG. 12 , in which multiple cavities  20 ,  30 ,  40 , and  50  are shown, defined on both the forward and aft end of a leading edge  10 . The cavity groups on each end may be linked together using a passageway  75  that allows air and/or fluid to pass between each chamber group. This leading edge  10  in  FIG. 12  is capable of rapid movement forward or aft, with the passageway capable of being closed off as necessary. In all situations where multiple chambers are used, the secondary cavity, being the cavity that is smaller than the one it is adjoined to, will assist in promoting a pressure node  55  as described for  FIG. 1   a  and  FIG. 2   a.  Where multiple cavities are used, with three or more cavities defined to create a cavity group, the largest cavity  20  will have a secondary cavity  30 , with a sub secondary cavity  40  available if so defined, with each successively smaller cavity supporting the larger cavity before it, in providing a means to urge the rapid creation of a pressure node  55 .  
         [0062]     Referring now to  FIGS. 13 and 14 , a leading edge  10  is shown, I which a pressure node  55  is defined along a linear distance. The vertical nature of this leading edge  10  would be an example of a bridge support, or other vertical structure. As stated above, the cross sectional view of the pressure node  55  in  FIG. 14  would extend along the entire length of the object  10 , as shown in  FIG. 13 , provided that the flow of liquids or gases into the cavities  20  and  30  are at a sufficient rate. The creation of the pressure node  55  is accomplished by allowing the flow of air and/or liquids to move into the cavity  20 , where the flow vectors meet and provide an central strip of increased pressure. The pressure node is enhanced by the secondary cavity  30 , which allows secondary pressure node to protrude out of the second cavity area into the primary cavity  20 . The flow of liquids and gasses as described for  FIG. 1   a  are duplicated with this linear cavity, in that the cross sectional view of  FIG. 1   a  extends the length of the linear cavity in  FIGS. 13 and 14 . The example of the benefits for this configuration would be clearly seen for use on automobiles, where the cavity configuration would extend linearly and horizontally across the ridge of an automobile, the leading edge of a wing, or extend vertically, as in the instance of a bridge support, which must maintain position against a constant current. In both situations, the linear cavity protects the surface of the object from unnecessary friction caused by turbulence.  
         [0063]     This method of creating a pressure node  55  has the ability to provide a smoother transition from subsonic to supersonic. In subsonic speeds, pressure waves flow over and around the leading edge of an object as well as the outer skin  11 , with a dramatic increase in turbulence as the speed approached supersonic. As the object breaks through the sound barrier from subsonic to supersonic, the pressure waves tend to flatten out, and are angled from the leading edge of the object, as opposed to flowing around the surface skin  1  of the object from the leading edge on toward the rear. The pressure node  55  provides an artificial extension of the leading edge, that cushions the object itself from the violent turbulence that is consistent with speeds as they move into the supersonic range.  
         [0064]     From the foregoing statements, summary and description in accordance with the present invention, it is understood that the same are not limited thereto, but are susceptible to various changes and modifications as known to those skilled in the art and we therefore do not wish to be limited to the details shown and described herein, but intend to cover all such changes and modifications which would be encompassed by the scope of the appended claims.

Summary:
A linear cavity is provided on the leading edge of an object that is subject to the flow of liquids or gasses, where said cavity preferably has a wall that follows the curvature of a diminishing sine wave, although other configurations are possible that do not follow a specific sine wave. The cavity accepts the flow of liquids or gasses that enter into the cavity, and where the dimensions of the cavity cause the flow of liquids or gases within it to form a pressure node that extends forward of the cavity. The pressure node provides a wedge means to cause oncoming gasses or liquids to divert around the object body ahead of the object body itself, decreasing turbulence around the periphery of the object. The cavity may be spherical, in the instance of a missile, plane, or underwater transportation means, or may be linear, in the instance of an automobile grill that is subject to wind, or a bridge support, where the bridge support has to maintain position against the flow of current. The cavities may also be defined only on the ridge or leading edge, or concurrently on the ridge leading edge and the rear aft edge of the object to allow efficient movement both forward and aft.