1. Field of the Invention
The present invention relates to ships and watercrafts having improved efficiency and seakeeping from underwater submerged displacement hull(s) attached to and part of a vessel that operates at sea level.
2. Background of the Invention
In recent years interest in the use of small waterplane area ships (SWAS vessels) has substantially increased because such vessels have improved hydrodynamic stability, low water resistance and minimal ship motion. Generally such vessels have at least one waterline located below its design draft with a waterplane area that is significantly larger than the waterplane area at its design draft. One form of such vessel is known as a small waterplane area twin hull vessel (a SWATH vessel) which generally consists of two submerged hulls, originally formed of uniform cross-section, connected to a work platform or upper hull by elongated struts which have a cross-sectional area along any given waterplane area that is substantially smaller than a waterplane area cross-section of the submerged hulls. Thus, at the design waterline such vessels have a small waterplane area.
The interest in such vessels has increased in large part because of the development work conducted by Pacific Marine Supply Co., Ltd. A variety of such vessels have been produced using twin submerged hulls or a plurality of submerged hulls, such as shown, for example, in U.S. Pat. No. 5,433,161. In the course of the development work for these vessels, further improvements were made and a so-called Mid-Foil SWAS vessel was developed, as disclosed in U.S. Pat. No. 5,794,558. Such vessels use a submerged underwater displacement hull or lifting body to provide lift to the craft in conjunction with any other parts of the vessel which generate lift. The lifting body differs from a hydrofoil in that the enclosed volume of the lifting body provides significant displacement or buoyant lift as well as hydrodynamic lift whereas the lift of a hydrofoil is dominated by only hydrodynamic lift. In the course of continuing development work, the particular shape of such lifting bodies was studied in detail in order to improve their performance and adapt and integrate their use to a wide range of marine craft.
More specifically, as disclosed in U.S. Pat. No. 6,263,819, it was found that the submerged bodies of marine vessels, when operated at shallow submergence depths, such as is the case for SWAS and Mid-Foil vessels, can be adversely effected by the displacement of the free water surface caused by the body's volume and dynamic flow effects. The interaction of that displacement of the free surface relative to the body's shape had not been adequately accounted for in the prior art structures. It is believed that this inadequacy of existing prior art submerged bodies for marine vessels is the result of the fact that submerged and semi-submerged marine vessels have historically been designed to operate at great depths relative to their underwater body thickness, as with submarines or hydrofoils.
A typical submarine is essentially a body of revolution-shaped hull which has three dimensional waterflow about it, but which is designed to operate normally several hull diameters or more below the free water surface. Thus, the displacement of the free surface of the water by operation of the hull at such depths is minimal and does not effect the operation of the body. On the other hand, hydrofoils are simply submerged wings with predominately two-dimensional flow and are designed typically to produce dynamic lift as opposed to buoyant or hydrostatic lift.
The displacement of water at the free surface by a submerged body is detrimental to a marine vessel's hydrodynamic performance with the impact varying as a function of the body's shape, submergence depth, speed and trim. For example, the free surface effects can significantly reduce lift in the body or even cause negative lift (also referred to as sinkage) to occur. Resistance to movement through the water by free surface effects is generally greater than if the submerged hull were operating at great depths; and pitch movements caused by the displacement of the free water surface vary with speed and create craft instability. With the advent in recent years of marine vehicles (such as the SWAS, SWATH, and Mid-Foil vessels) which use a shallowly submerged body the detrimental effects of free surface water displacement on submerged hulls has been recognized.
Prior to the invention as disclosed in U.S. Pat. No. 4,263,819, submerged displacement watercraft hull body shapes were generally cylindrical or tear-drop shaped bodies of revolution. The simplest variations are bodies with generally elliptical cross-sections, such as are shown, for example, in U.S. Pat. No. 4,919,063 or 5,433,161. Others were simply shaped in a manner similar to an airplane wing, as shown for example, in U.S. Pat. No. 3,347,197. On the other hand, hydrofoil dynamic lift shapes are generally thin-foils with little or no, buoyancy and symmetric foil sections having straight leading and trailing edges. In plan these foils are generally straight, or are swept forward or rearwardly and/or are trapezoidal in shape. Additionally, they can have dihedral or anhedral canting from the horizontal. It was found that the performance of vessels using these shapes is adversely effected by the displacement of the free surface of the water above the bodies during operation of the vessel.
According to teaching of U.S. Pat. No. 6,263,819 (hereinafter the “'819 patent”), a low drag underwater submerged displacement hull is defined from two parabolic shapes. The periphery of the hull when viewed in plan is symmetrical and defined by a first parabolic form (or parabolic equation) with the form defining the leading edge of the hull. The longitudinal cross-section of the hull is formed of foil shaped cross-sections which are defined as cambered parabolic foils having a low drag foil shape and providing a generally parabolic nose for the hull. Generally, each longitudinal cross-section of the hull parallel to the longitudinal or fore and aft axis of the hull has a symmetrical cambered parabolic foil shape with the cross-section along the longitudinal axis of the hull having the maximum thickness and the cross-section furthest from the centerline of the hull having the minimum thickness. In plan, the hull has a stern or trailing edge which is defined by either a straight line, a parabolic line, or a straight line fared near its ends to the side edges of the plan parabola shape.
In another embodiment the hull shape is a parabolic body of revolution. In a third embodiment the hull also has a foil shape in longitudinal cross-section which is essentially formed by a parabolic body of revolution cut in half and separated by a uniform midships section, whose longitudinal cross-sections are uniform in shape and correspond to the parabolic shape of the body of revolution.
These body shapes have benign pressure gradients and small stagnation points over the body which make the bodies less sensitive to changes in the body angle of attack relative to the flow so that they are less effected by free water surface disturbance. Parabolic foil embodiments have high Block coefficients which maximize their volume to surface area relationship with the result that they have less frictional drag because of reduced wetted surface area, less structure and thus less cost. With higher Block coefficients, such as the 60-70% coefficients achieved with the lifting bodies of the '819 patent, the volume of the foil relative to its surface area is maximized and, as a result, the foils provide greater buoyancy for the same surface area as compared to the prior art.
Because of their high Block coefficient, high displacements can be achieved with hulls having relatively short bodies. This allows these bodies to operate at high Froude numbers, preferably in excess of 1. This in turn results in less wave making drag and less friction drag from a thinner boundary layer. Wakes formed by these bodies are very uniform and result in minimal disturbance beyond the trailing edge to appendages bodies, or propulsers positioned at the trailing edge or stern. The symmetrical parabolic foils, at critical design submergence depths, displace the free surface of the water in a manner which reduces the pressure coefficient on the bodies and allow higher incipient cavitation speeds. Their dynamic lift can then be varied as a function of camber (i.e. variation of the surface location from the design parabola), submergence, speed and angle of attack. As a result, optimization of lift characteristics for a given craft design speed and draft can be achieved. Further, dynamic lift of these bodies can be varied by the use of integrated trailing edge flaps, which will mitigate appendage drag of non-integral foil stabilizers.
It has been found that the symmetric lifting bodies of the '819 patent operate very satisfactorily for most applications, even for very large vessels of 2000 tons and up. However, it is advantageous to have lifting bodies which are smaller relative to the length of the ship and capable of being positioned outboard of the watercraft hull. Therefore, further development of the lifting bodies of the '819 patent has occurred, particularly for use with monohull vessels.
The symmetrical lifting bodies as disclosed in the '819 patent were primarily used generally directly under the hull. However, if the lifting body is located further from the center of gravity of the ship, it not only can provide lift but greater dynamic control as a result of maximizing dynamic moment. In addition, it has been found useful to tailor the shape of the lifting body to conform to the hull it is used with as well as to accommodate flows under the hull caused by the hull or other underwater structures. It also has been found that while large monohull vessels have very good seakeeping ability, the use of the tailored asymmetric lifting bodies of the present invention with such hulls greatly increase their seakeeping abilities.
It is an object of the present invention to provide a submerged lifting body which can be employed on various marine vessels to maximize performance of the vessel by creating a high lift to drag ratio (L/D), i.e., low drag, at operational speed, while increasing dynamic control.
Another object of the present invention is to provide a submerged lifting body for use on various marine vessels which improves performance of the vessel at operational speed while creating a dynamically stable vessel.
Yet another object of the present invention is to provide submerged lifting bodies for use on various marine vessels which can increase the efficiency of these vessels by reducing hydrodynamic drag.
A further object of the present invention is to adapt these improved submerged lifting bodies to a variety of watercraft (monohulls, catamarans, trimarans, swath, semi-swath, planing and displacement vessels) by optimizing their shape, size, number and location.
Another object of the present invention is to provide submerged lifting bodies for use on various marine vessels that are shaped to reduce the possibility of being damaged when docking or coming alongside another structure.
Yet another object of the present invention is to provide submerged lifting bodies for use on various massive vessels that reduce the wave making and slamming of a vessel.
Yet another object of the present invention is to provide submerged lifting bodies for use on various marine vessels that improve the seakeeping by reducing the vessel's motions while at rest as well as while underway.
Still another object of the invention is to provide submerged lifting bodies for use on various marine vessels that are shaped to result in improved flow to an integrated propulsor yielding high propulsive efficiency.
In accordance with an aspect of the present invention, an underwater lifting body is provided that meets these objectives. Briefly, off vessel centerline mounted lifting bodies are disclosed whose shape has been tailored to the flow at its location to optimize the performance of the body. In cross-section, the lifting body is parabolic foil shaped and in plan view there is no longitudinal plane of symmetry.
Generally, a three-dimensional low drag underwater lifting body for operation in a submerged state is provided which has a fore and aft axis and an outer surface whose shape conforms in plan on one side of the fore and aft axis to a first parabolic curve whose vertex is located on the fore and aft axis, and on the other side of the axis to a second different parabolic curve whose vertex is also located on the fore and aft axis. The parabolic curves together define a leading edge for the lifting body when viewed in plan. The outer surface of the lifting body also conforms, in longitudinal cross-sectional planes parallel to the fore and aft axis, to graduated generally parabolic foil curves having vertices lying on the leading edge defined by said first and second parabolic curves and which extend aft predetermined distances, with the thickness of the parabolic foil shaped longitudinal cross-sectional planes decreasing from the fore and aft axis of the lifting body to the leading edge of the lifting body.
In another aspect of the invention, the three dimensional low drag underwater lifting body for operation in a submerged state has a fore and aft axis and an outer surface whose shape conforms in plan on one side of said axis to a first parabolic curve whose vertex is located on the fore and aft axis, and on the other side of said axis to a second different parabolic curve whose vertex is also located on the fore and aft axis. These parabolic curves together define a leading edge for the hull when viewed in plan. The lifting body also conforms, in longitudinal cross-sectional planes parallel to the fore and aft axis, to graduated generally parabolic foil curves having vertices lying on the leading edge defined by said first and second parabolic curves and which extend aft predetermined distances, with the thickness of the parabolic foil shaped longitudinal cross-sectional planes decreasing from the fore and aft axis of the lifting body to the leading edge of the lifting body. The lifting body has a bow and a stern and a predetermined length extending from the bow to the stern; the first parabolic curve increases in width from said bow to stern with the stern being defined by the segment of a third parabolic curve transverse to the lifting body's length extending from the widest portion of the first parabolic curve to said axis.
In yet another aspect of the present invention, a watercraft includes a first hull having a surface waterline, at least one strut depending from the hull and a three-dimensional underwater submerged lifting body secured to the strut beneath the waterline during operation of the watercraft. The lifting body has a fore and aft axis and an outer surface whose shape conforms in plan on one side of the fore and aft axis to a first parabolic curve whose vertex is located on the fore and aft axis, and on the other side of said axis to a second different parabolic curve whose vertex is also located on the fore and aft axis. The parabolic curves together defining a leading edge for the hull when viewed in plan. The lifting body also conforms in longitudinal cross-sectional planes parallel to the fore and aft axis, to graduated generally parabolic foil curves having vertices lying on the leading edge defined by said first and second parabolic curves and which extend aft predetermined distances, with the thickness of the parabolic foil shaped longitudinal cross-sectional planes decreasing from the fore and aft axis of the lifting body to the leading edge of the lifting body.
In further aspect of the invention, a watercraft includes a first hull having a surface waterline, at least one strut depending from the first hull and a three-dimensional underwater submerged lifting body secured to the strut beneath the waterline during operation of the watercraft. The lifting body has a fore and aft axis and an outer surface whose shape conforms in plan on one side of the axis to a first parabolic curve whose vertex is located on the fore and aft axis, and on the other side of said axis to a second different parabolic curve whose vertex is also located on the fore and aft axis. The parabolic curves together define a leading edge for the hull when viewed in plan. The lifting body also conforms, in longitudinal cross-sectional planes parallel to the fore and aft axis, to graduated generally parabolic foil curves having vertices lying on the leading edge defined by the first and second parabolic curves and which extend aft predetermined distances, with the thickness of the parabolic foil shaped longitudinal cross-sectional planes decreasing from the fore and aft axis of the lifting body to the leading edge of the lifting body. The lifting body also has a bow and a stern and a predetermined length extending from the bow to the stern. The first parabolic curve increases in width from said bow to the stern with the stern being defined by a segment of a third parabolic curve transverse to the lifting body's length and located at the widest portion of the first parabolic curve.
In accordance with a still further aspect of the invention, a watercraft includes a first hull having a surface waterline, at least one strut depending from the first hull and a three-dimensional underwater submerged lifting body secured to the strut beneath the waterline during operation of the watercraft. The lifting body has a fore and aft axis and an outer surface whose shape is defined by a leading edge for the lifting body when viewed in plan and, in longitudinal cross-section by symmetrical generally parabolic foil curves having vertices lying on the leading edge of the lifting body and lying in planes parallel to the fore and aft axis. The lifting body has first and second hull sections on opposite sides of the fore and aft axis and a midship section between the first and second hull sections and located to one side of the fore and aft axis. The first and second hull sections conforming in plan to first and second different parabolic curves whose vertexes are respectively located on and define a portion of the leading edge; the midship section having a parabolic foil shape in longitudinal cross-section which is uniform in planes parallel to the fore and aft axis between the first and second hull sections across the width thereof. The foil curves of the first and second hull sections decrease in thickness from the fore and aft axis of the lifting body to the edge thereof.
The lifting bodies of the present invention as described above are asymmetric about their main fore and aft axis. This permits the lifting bodies to be positioned relative to the hull of the ship to conform to the hull, to accommodate water flow characteristics below the hull caused by the hull's shape and to modify the angle of attack of the lifting body. For example, two lifting bodies can be secured to opposite sides of the hull so either of their asymmetric sides are adjacent to the ship's hull so as to present alternative leading edge configurations depending on the ship's hull shape.
By positioning the lifting bodies outboard of the hull, greater dynamic moment is created increasing dynamic control. On multihull vessels the lifting bodies may be placed both inboard and outboard.
The above, and other objects, features and advantages of this invention will be apparent to those skilled in the art from the following detailed description of illustrative embodiments of the invention which is to be read in connection with the accompanying drawings wherein:
FIGS. 5 is a plan view of the embodiment of
a is a front view of the embodiment of
a is a front view of the embodiment of
a is a bottom plan view similar to
b is a sectional view taken along line 25b-25b of
c is a front view of the right lifting body shown in
a is a view similar to
b is a sectional view taken along line 26-26 of
a illustrates another form of a lifting body for use as the bow lifting body of the embodiment of
b is a sectional view taken along lines 28b-28b of
Referring now to the drawing in detail,
The shape of lifting body 10, in cross-section, is generally that of a parabola 15, as seen in
Lifting body 10 is symmetrical, and longitudinal cross-sections taken parallel to its fore and aft axis 14 are generally symmetrical to the parabolic foil shape defining the central cross-section shown in
Lifting body 10 also includes a stern or rear edge 16 which, in the illustrative embodiment, is thin and straight. The parabolic foil curve 15 which defines the longitudinal cross-sectional shape of the lifting body extends from edge 12 towards the stern, as seen in
The components illustrated in
The lifting body 40 shown in
The lifting body 45 shown in
By creating asymmetric lifting bodies in this way, the lifting bodies 30, 40 and 45 maintain substantially all of the advantages of the lifting bodies described in the '819 patent, but in addition have greater flexibility in use, particularly in connection with monohull and catamaran structures of generally conventional construction. Because of the asymmetry of these lifting bodies, they can be positioned at varying angles of the attack with one or the other of their asymmetric sides adjacent the hull to conform to the flows generated by a particular hull beneath the water's surface. In addition, because they are somewhat narrower than the original lifting bodies from which they are formed, they can be conveniently placed close to the hulls, but outboard therefrom in order to produce dynamic control as a result of the increased dynamic moment the lifting bodies produce on the hull. This is shown, for example, in the views of
In the embodiment of the invention illustrated in
In the embodiment of the ship 50 shown in
In the embodiments illustrated in
a and 26b are similar views to
The embodiments of the invention illustrated in
It has been found that asymmetric lifting bodies constructed in accordance with the present invention are particularly suitable for very large vessels, typically above 2000 tons displacement. Smaller vessels are not particularly long in length and thus lifting bodies constructed in accordance with the '819 patent fit those smaller vessels better and have a tremendous impact on their performance ratios. Once vessels get larger than 2000 tons, the proportion of the length of the ship to the length of the lifting bodies becomes greater and the effect of the lifting body's practical size becomes less. However, the lifting bodies are still beneficial since they can replace other appendages on the vessel such as the propulsion pods and stabilizers, while still allowing the vessels to carry larger loads.
Using asymmetric lifting bodies constructed in accordance with the present invention on larger ships, significantly improves performance for their size relative to the size of the ship. They not only provide additional lift, they can be tailored and trimmed to reduce wave effects to the least resistance to passage of the vessel through the water with the best sea keeping characteristics. An example of such an effect occurs in monohull vessels which have sharp chines that are designed to reduce roll fitted with lifting bodies constructed in accordance with the present invention. In that case the lifting bodies can be formed to produce enough lift when the vessel is underway that the vessel is raised enough the chines come out of the water. As a result, the chines can be made larger to resist roll even more when the vessel is at rest, but when they are lifted out of the water there is less slamming of the vessel as it moves over the waves.
A large vessel 100, fitted with lifting bodies constructed in accordance with the present invention is shown in
Finally, at the aft of the vessel, a pair of lifting bodies 30, constructed in accordance with the embodiment of
Instead of connecting the bow lifting body to vessel 100 with a single strut, the lifting body can be connected by a blended wing arrangement as shown in
The shapes of the lifting bodies of the present invention result in minimal disturbance beyond their trailing edge through appendages, bodies or propulsers may be positioned behind them. These bodies displace the free surface in a manner which reduces the pressure coefficient on the body, allowing higher incipient cavitation speeds. Their dynamic lift can be varied as a function of camber, submergence, speed and angle of attack to optimize the lift characteristics for a given craft design speed. For motion control and stabilization, the dynamic lift of the bodies can be varied by the use of integrated trailing edge flaps.
Referring again to the vessel shown in
The second positive attribute is that a lifting body typically has a higher efficiency than that of a hull alone. By adding a component with a higher efficiency (lift to drag ratio, L/D) the L/D of the entire system increases. The inventors' studies have quantified these positive effects of adding a lifting body to the bow of a large ship using the method of computational fluid dynamics (CFD). To find the optimum location on the hull for placement of the lifting body relative to the bow, four different locations, as shown and numbered 0 through 3 were considered through a speed range of 30-50 knots, as shown in
Because the lifting body is intended to reduce the bow wave by wave cancellation and to elevate the hull and increase the overall efficiency, it is preferable that the area of low pressure on the upper surface of the lifting body not be interrupted by large struts or other appendages. By attaching the lifting body as shown in
It is known from previous studies that the Serter hull has a natural tendency to trim bow up over a speed range. By adding a lifting body in accordance with the present invention, the positive trimming moment will be increased and the resulting dynamic trim will also increase.
The maximum lift achieved by the lifting body while attached to the ship at 50 knots, two degrees, was determined to be 193 lton. Since the lifting body creates approximately 30,000 ft-lton trimming moment at 50 knots, the resulting dynamic trim of the vessel will be more than one degree.
To counteract this positive moment and achieve a level trim for best efficiency, a lifting hydrofoil or body should also be added somewhere aft of the ship's center of gravity, for example, as shown in
1) balance the trimming moments of the hull and the lifting body
2) provide enough lift to achieve an optimum displacement for the hull
It can be established that the point of maximum efficiency for this particular hull occurs at a displacement of 1600 lton. Since the lifting body tested provides 193 lton at 50 knots, it would be desirable to place a second lifting body or hydrofoil aft of the center of gravity to provide 207 lton lift, to produce the optimum 1600 lton lift on the hull for a total 2000 lton ship.
Integrating the lifting body at the bow and an aft foil or lifting body into the design of the ship allows the introduction of a motion control system such as control trailing edge flaps on the lifting body and aft foil. With the implementation of a control system motion damping can be affected withe benefits to added resistance in a sea way and crew effectiveness. With reduced motions speeds can be maintained and range is less affected by higher sea states. The lifting body of the bow and the aft foil individually add damping to the overall ship, but the addition of an active control system will substantially increase their benefits to ship operations.
It should be noted that the new configuration with the lifting body on the bow and aft foil is more efficient than the hull when each arrangement is free to trim as well when fixed at zero degrees. This proves that the drag reduction wasn't due to the trim of the hull but rather the addition of the lifting body bow used in conjunction with a transom foil.
Although illustrative embodiments of the present invention have been described herein with reference to the accompanying drawings, it is to be understood that various changes and modifications may be effected therein by those skilled in the art without departing from the scope or spirit of this invention.
This application claims the benefit of U.S. Provisional Application No. 60/466,787, filed May 1, 2003.
Number | Date | Country | |
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60466787 | May 2003 | US |