The present invention generally relates to hull designs for watercraft such as sailboards, surfboards and so-called personal watercraft (PWC) and, more particularly, to a step design for a planing surface thereof.
Many watercraft are designed to operate in a planing mode as well as in a displacement mode, particularly watercraft designed for recreational use. In a planing mode of operation, lift is derived from a downward deflection of water by the shape of the hull at relatively higher speeds than hulls operating in a displacement mode where lift is derived from the mass of water displaced by the hull. It is well-recognized that the force required to propel watercraft increases sharply with speed during displacement mode of operation and through a transition mode of operation where the watercraft speed causes the onset of planing. When planing is achieved, much of the wave drag is lost. The total drag force then decreases and increases only slightly with increased speed until reduction of the wetted surface decreases and then the wetted surface increases. Accordingly, to further reduce the wetted surface area, and drag at higher planing speeds, hulls have sometimes incorporated a step, generally formed as a substantially vertical surface following a planing surface. For a sailboard, these steps are generally near the back or stern of the board. As lift from planing increases with speed, the portion of the hull behind the step would be lifted clear of the water and was (or was assumed to be) substantially dry.
For small planing hulls such as those of sailboards, such steps and their location were a compromise of having the planing surface further forward, i.e. near the center of gravity when planing fast and a larger planing surface when the hull is starting to plane, i.e. when the board is moving slower and an attempt is being made to transition it from the displacement mode to a planing mode by exceeding a speed hereafter called the transition speed. Also, prior art steps on a sailboard hull had a flat or slightly rockered planing surface in front of the step.
From Bernoulli's theorem, since the water speed is greater at this step than it is after any expansion past the step, there is a vacuum that tends to form behind the step. Such a vacuum, of course, forms a drag force on this vertical surface in the sailboard hull or other watercraft hulls. This is why these prior art steps need to be ventilated as taught in U.S. Pat. No. 6,595,159 B2. However, it was not known how deep to make the step and there was little, if any, lift behind these prior art steps when the hull was transitioning from displacement to planing mode.
The main purpose of the steps, when there is sufficient wind or power, is to allow the hull to plane at a higher, more optimum attack angle thus reducing the wetted surface, decreasing the drag and increasing the hull speed. Generally for any planing hulls with a fixed center of gravity, the attack angle of the hull starts out above the optimum at transition speed then decreases to below the optimum as speed increases. Conversely the optimum angle is smallest at transition speed, due to some displacement lift, and then increases to 4 or 5 degrees as planing speed increases to about 30 mph where the displacement lift is essentially zero.
For sailboards, a sailboarder can change their position on the board or hull thus changing the center of gravity. However, almost all sailboarders lack the skill to achieve the optimum attack angle from transition speed to very fast planing speed on prior art sailboards with prior art steps, particularly since foot straps are provided in one location.
In many prior art steps, the step is across the whole planing surface as in the step on a flying boat, airplane pontoons and some boats. In other cases, the step may be formed by the end of a sponson. In either case, substantial drag at transition speeds is presented.
There are a number of additional problems with the prior art step.
Ventilation of a fin as on a sailboard is when air is drawn in to the low pressure side of the fin. The resistance of a sail board fin to ventilation depends on the distance from the fin to the back of the board and the width of the planing surface to the side of the fin. In the prior art, the region behind the step is recessed deeper into the hull or board than the region next to the fin and the vortex which then forms can ventilate the planing surface back to the side of the step thus reducing the ventilation resistance of the fin.
Note: that NACA uses depth of step to denote the height of the step into the hull, see for instance NACA TN 1062 (1946), rocker is a term used in water craft, particularly in surf boards and sailboards, of slight positive 2nd derivative and camber is a term used in wings, hydrofoils or planing surfaces of negative 2nd derivative. The camber at the end of a planing surface either toward the rear or toward a chine is called cupping.
It is therefore an object of the present invention to provide a step for a planing surface of a watercraft which provides increased dynamic lift behind the step at or near the transition speed and is located to provide more nearly optimal angle of attack at planing speeds.
It is another object of the invention to provide a step having reduced wetted surface and vortex drag and which converts the inherently created vacuum into a forward thrust, as well as to increase effective aspect ratio of the wetted surface in front of the step as well as to resist ventilation of a fin.
It is a further object of the invention to provide a step that causes reduced variation in the optimum location of the center of gravity to maintain near-optimum angle of attack over a range of planing speeds.
In order to accomplish these and other objects of the invention, a step shape for a planing hull is provided, wherein the surface immediately in front of a step makes up only part of the beam of the planing surface and the remainder of the beam includes a planing surface, the step shape including a planing surface, a small step depth at the end region of said planing surface followed by a surface region having a contour that approximates a trajectory or wake of water which would occur directly off of said planing surface near but above the transition speed and desired attack angle and will cause water to contact a further surface region behind or on the surface region having said contour when the hull is at transition speed, but does not contact said surface region at a faster high planing speed, said further surface region being at such a depth to have dynamic planing lift on the surface behind the said small step depth when the hull is at a transition speed from a displacement mode to a planing mode and which, at higher planing speed, the main water flow from the step does not contact the said surface region behind the said step depth, said step being located in the back 40% of the hull.
In accordance with another aspect of the invention, a step shape for a planing hull is provided comprising a first planing surface with an end region adjacent to said planing surface with a positive second derivative shape on the order of 1.0 (cm−1) to form an angle at the end of the end region which is considerably less than 90° and on the order of 20°, a second region of the hull directly behind said end region with depth into the hull surface of 5±4 mm measured from a line, which starts on the planing surface 20 cm in front of the end region and is tangent to the end region, and extending backwards up to 20 cm.
In accordance with a further aspect of the invention, a step for a planing hull is provided including a side part of the step extending back toward the end of the hull of a sailboard or watercraft, and a planing surface which abuts the side part of the step to form a butted surface, said planing surface being cupped such that the attack angle of the butted surface is increased at the side part of the step.
In accordance with a yet further aspect of the invention, a hull of a sailboard, surfboard or personal water craft is provided with at least one step, where the region near the fin or the like for which ventilation is undesirable includes a planing surface which is substantially flat in a transverse direction of the hull and a region immediately in front of said step is at a greater depth than an adjacent region that is in front of the fin or the like.
The foregoing and other objects, aspects and advantages will be better understood from the following detailed description of a preferred embodiment of the invention with reference to the drawings, in which:
Referring now to the drawings, and more particularly to
In
This 2nd region B is followed by a 3rd region C of much less or negative second derivative of y with respect to x or rocker. The depth into the hull of this 3rd region is 5±4 mm as shown by the dotted line depths 5 in
For a sailboard, the location of the step or steps of this invention is in the last 40% of the hull. For other types of vessel it could be near the center of gravity. As shown in
Also shown in
Also shown in
If desired, the planing surface 9, just in front of step 2, may be cupped, here by 2 degrees. (The term cupped or cupping as used herein is intended to connote a slight bending or downward curving, along the direction of water flow, of the surface in a direction toward the water for purpose of adjusting the direction of water flow.) It has been shown that this cupping of surface 9 along with cupping 22, at the end of region D of the step design 1, and contact with water in region D and/or C can give the same lift at transition speed as if there were no step 2. This substantially equal lift has been verified by data for drag on the 98 cm wide sailboard both with this preferred step design 1 and without any steps, as shown in
From the theory and equations in Payne, Peter R.; J. Hydronautics, Vol. 8, no. 2, (1974) appendix A, the optimum camber, cupping 9 or hook angle “δ” is about 4-7 degrees depending on the planing attack angle “τo” of the board and the wetted length “lm” in front of the step. Larger optimum camber angles “δ” are appropriate for fast speeds that produce smaller attack angles “τo”. A sailboard was tested with this optimum cupping or camber angle 9 and was consistently 15% to 20% faster than a smaller board, even though, for the wind and wave conditions of this test, it would be expected the small board to have been faster (see also
Thus not only is it preferred that this surface 9 is cambered/cupped, the optimum “δ” angle can be estimated as well as the cup depth at the step 2. From the above theory of Payne for the lift and drag of a cambered surface “δ” is given by:
δ=−4Ctto+{(4Ctτo)2+200Ct}1/2 (1)
By assuming the water flow off of the step is along line 11 at step 2 and the depth above line 11 at the end of the hull is <0.0015×(length)2, where the depth below line 11 and the length from the step to the end are in centimeters, the optimum cup depth at the step 2 is given by;
y2<y1={20×0.0015×(length)2}/(20+length) (2)
or
y2˜2/3y1
For a step 40-45 cm from the end of the board this gives:
y2˜0.6 cm or <0.9 cm.
It should be noted that
This camber in front of the steps increases the dynamic water pressure not only on surface 26 in
Referring now to
At higher planing speed the main water flow from the step 2 does not contact the surface region behind the step in region B. Since different watercraft and different total weight could have different step depths “a small step depth” as used herein means a step depth smaller than that where the ventilated flow at 2 mph above the transition speed, for an attack angle, τo, of 3.5°, reconnects with the hull is below the “y” position of the step 2. That is, if the step is deeper, the flow will curve upwardly to a greater degree and the y depth of the point where the flow reconnection occurs will be above the y depth of the step 2.
Referring now to
The fact that regions 23 are not significantly recessed into the board near the rear portion thereof but approach the depth of planing surface 24 at the rear of the board increases the water pressure near the fin and thus increases the ventilation resistance of the fin. That is, at and near transition speeds, there is little vortex flow at the side of the step because there is water contacting surfaces 24 and 23 on opposite sides of the step and both surfaces are at essentially the same depth. Instead, the planing regions in front of steps 2 are set deeper into the water than the adjacent part of region 24. This difference in depth is shown by line 31 in
Step 2 need not be perpendicular to the water flow. As shown in
In contrast with this unique combination of consistently beneficial features, U.S. Design Pat. Des 258,516 may appear somewhat similar to the invention but the surface region behind the step is not recessed nor is there a cupping adjacent this region to keep water off of this region at higher planing speeds. U.S. Pat. No. 5,191,853 and U.S. Pat. No. 5,588,389 are perhaps the closest description in prior art of the surface region behind the step. However, in '853 and '389 the planing area behind the step is designed to, in '853, “stay in the water and provide lift” and in '389 must be in the water because of the location of the step and center of gravity. Both also have vertical steps (step 4 in '583 and step 23 and 102 in '389) giving a step depth which is much larger than that of the invention. Mote importantly, both teach steps extending across the whole beam of the hull. That is, they do not have a smooth planing surface for a substantial distance in front of a fin or other desirably non-ventilated structure.
At the higher planing speeds this cup 19 reduces the vortex of the water coming off of side step 12, thus reducing the water flow onto the area 23 behind the step 2. Such water flow is, of course, undesirable for high planing speed, since this will add both drag and lift at the back of the board and thus reduce the planing angle below the optimum.
Further, as alluded to above, this cup angle can be larger for side portions of the step which are more aligned with the length of the hull or where the area behind step 2 is wide. That is, if the water flow is at a very obtuse angle to cross section BB then cupping near “12” in
Referring now to
The back planing surfaces 23 shown in
The step height consists of a downward curved section (cup 9 of
The board's bottom can be essentially flat near the fin, except for the increased attack angle the intersection between regions 23 and 24. In this way the board and fin will have more resistance to ventilation of the fin at transition speeds, while the increased bottom depths near the front of the step will increase the attack angle of the sailboard closer to optimum when the board is planing fast.
Series 2 was for one embodiment of a step design in accordance with the invention, again the step was 35 cm long, an average of 9 cm wide and having a depth of 0.3 cm at a location 5 cm behind the step 2 and a depth of about 0.6-0.08 cm at the end of the regions 3 and 4. For this step, the board transitioned to planing at 7.4 mph and only 29.7 pounds of force were required to maintain planing speed. Moreover, during high speed planing at 14 to 22 mph the force was the same or possibly slightly less.
These series 1 and 2 data show that the step in accordance with the invention has lift behind the step to get the board to plane with both less drag force and lower board transition speed. Yet at high speed it reduced the planing area behind the step(s) as effectively as the theoretical operation of a normal (prior art) step including a vertical surface but which cannot achieve such low drag because of wave drag due to vortices and other effects such as wetting of theoretically dry surfaces. Note that there was a 20 to 25% reduction in the drag force at transition speed achieved by the invention even though the step area represents only about 10% of the board planing area. This could be due to the rocker in this board or the wave and turbulence drag behind the normal prior art step with a vertical 2 cm depth.
As briefly discussed above,
In can be readily seen that this 98 cm sailboard loses its wave drag at 6.0 mph due to its winglets (see US 2003/0003825 A1) not discussed here. All data series show essentially the same drag, within experimental error; from 6-8 mph. Starting at about 9 mph of board speed the series 2 & 3 data show less drag. At 15 mph the series 2 drag is about 20% less than the series 1 data with no step.
Series 3 is for the step embodiment at 45 cm from the end of the board with a camber/cup 9 depth of 6 mm. These data show 30% less drag for board speeds of 12-19 mph from that of no step and up to 20-25% less than series 2 data. This is because the increased lift in front of the step, due to the increased camber 9, allows the board to sail at a more optimum attack angle, which produces a greater lift to drag ratio. The increase in drag in the series 3 data from 10 to 19 mph is less than the increase of drag on the two fins between these speeds, while above 19 mph the major increase may be due to a decrease in attack angle τ or wake from the boat.
Those skilled in the art will appreciate that two or more applications of the step in accordance with the invention can be used in a direction longitudinally of the hull in accordance with the invention. It should be appreciated that the step in accordance with the invention can be used with known hydrofoils nearer the front or middle of the hull to better maintain an optimum planing angle at even faster planing speeds.
In view of the foregoing, it is readily seen that the step and related bottom surface features associated with and collectively referred to as a step in accordance with the invention provides a step for a planing hull, said step having a shape that includes a planing surface, preferably cambered/cupped, which ends in a small step depth followed by a surface region having a contour that approximates a trajectory or wake of water which would occur directly off of said planing area and when the hull has a speed and desired attack angle through the water at a speed between the transition speed (e.g. transitioning from a displacement mode to a planing mode) and high planing speed, which trajectory will contact the surface region behind the step when the hull is at transition speed, but does not contact said surface region at the faster high planing speed. The said step surface region being at such a depth to have dynamic planing lift on the said surface behind the said small step depth when the said hull is at a transition speed from a displacement mode to a planing mode.
In this invention the step is confined to only part of the beam of the planing surface in front of the step and the beam of the planing surface of the hull behind the step, for high planning speed or fast planing, is reduced by the width of the steps. The other part of the bottom hull surface is a continuous planing surface to the fin or other non ventilated means between the steps or on the sides of the step. Since the design of this step in this invention may not appear to be a step or to be recognized as such in view of known, vertical surface transition step designs, to one who is not skilled in the art of hydrodynamics, the step is hereby defined as that point at high planing speed where the water flow disconnects from the hull surface but at which point there is planing lift behind said point at slower speeds.
In this invention, the step and the trailing surface consists of a first planing surface, 2nd region of positive second derivative of “y” with respect to “x”, where “y” is a distance from a horizontal plane into the hull and “x” is a longitudinal distance along the plane, on the order of 1.0 (cm−1) (a range of about 0.3 to 3 cm−1), i.e. positive rocker or negative camber, directly followed by a 3rd region of much less or negative second derivative or rocker. The angle at the end of this 2nd region should only be on the order of 20 degrees (a range of about 5 to 60) from the horizontal as opposed to the 90 degrees of the prior art. That is, the angle at the end of the 2nd section should be considerably less then 90°.
The integration of the 2nd derivative shape across this 2nd region gives the angle at the end i.e. the angle on the order of 0.35 radians or 20 degrees. A second integration gives the depth, into the board at the end of this 2nd region 2A.
The attack angle of the end of the 3rd section should be on the order of zero degrees of attack angle. If desired or preferred, the last or 4th section can then have a region of positive camber, negative second derivative of “y” with respect to “x”, to an attack angle that can, if desired, approximate or exceed the average attack angle of line 11 of
The general shape of most of the 3rd and 4th regions should be close to that which the water would take if there were not a surface behind the step, or only a vertical surface as in known step designs but no further surface to the rear of the vertical surface, for a hull speed between that of the transition speed and the high planing speed. The final height of the last section should be such that it is dry or unwetted, i.e. it is not in the main water flow, at the desired high planing speed. This can be predicted by the standard equations for the wake behind a planing surface given, for example, in “Hydrofoil Handbook” Vol. II, Hydrodynamics Characteristics, of Components, chapter 6, Bath Iron Works Corp., Gibbs and Cox, Inc. New York, N.Y. (1954), or “Hydrodynamics of High-Speed Marine Vehicles” by O. D. Faltinsen, section 6.2, pp. 344-358, Cambridge Univ. Press. It is preferred that the region just in front of the defined step point has added camber/cupping.
Thus at transition speed much of the entire region behind the step is in the flow of water and the last camber region has lift, as it turns the water flow downward and the dynamic drag of such a region is very small while at the desired high planing speed, except for possible spray, this region is completely out of the water, thus increasing the attack angle of the hull and reducing the wetted area.
The lift in this 4th region behind the step point will compensate the lift near the front of the board near the transition speed when the rear of this region is wetted, while the lack of lift in this area at high planing speed will compensate for the front of the wetted planing surface moving back. Thus the optimum location of the sailboarder will be confined to a smaller region near or at the foot straps. Since the region of the step can now be considerably in front of the end of the board's tail, this invention will stabilize the porpoiseing effect.
In accordance with the invention, porpoiseing is limited by the fact that the step may now be further forward thus making the width of the front part of the wetted planing surface considerably wider than that at the rear at high planing speed. Thus for a given attack angle where porpoiseing occurs, the planing surface is longer. During a heave motion of porpoiseing, this reduces the force near the front of the planing surfaces in a nonlinear amount, while any contact of the end region with the water will increase the force in the rear, in a nonlinear amount. This increased length and these nonlinear effects are what decrease the porpoiseing and tail walking. The tail walking is limited by the third region behind the step point coming in contact with the water flow when the optimum attack angle is sufficiently exceeded.
The step in accordance with the invention essentially eliminates the need for step ventilation other than that which will occur from the back of the board at higher planing speeds due to its small depth. If for some applications it is desired to ventilate this step from above or from the side, the region between the 2nd depth region and 3rd region can be modified in the normal way to add a ventilation region. However, as much as possible of this 3rd region should be preserved, as shown in
This step design preferably has no vertical surface, except for a small region if further ventilation is desired, thus it produces less drag. Indeed the Bernoulli vacuum results in a forward force rather than a drag force when there is no additional ventilation and when the hull is in at the optimum planing attack angle such that there are no regions with negative attack angles, except for a few centimeters. Irregularities in the water flow such as vortices, however, may still present significant lift and drag unless mitigated or eliminated by cupping of the planing surface at the edge or side of the step.
That is, in order to reduce the vortex from a side section and its drag or lift on the surface behind the step, the planing surface just before any side section of the step should be cupped or cusped like a chine flare or recurvature. This cusp or cupping will give the water some increased downward motion, as it passes off of this edge. This cusp or cupping will reduce the vortices and reduce the amount of water going to the surface behind the step, thus reducing the lift (which may alter angle of attack) and drag during high speed planing from the surface behind the step, which would be caused by too much vortex flow directing water flow up onto the last region. This cupping length is only a few centimeters long so that it does not appreciably increase the lift of the said planing surface before the side step.
While the invention has been described in terms of a single preferred embodiment, those skilled in the art will recognize that the invention can be practiced with modification within the spirit and scope of the appended claims.
This application is a United States national-stage filing from Patent Cooperation Treaty (PCT) application PCT/US2009/057138 filed Sep. 16, 2009, which claims benefit of U.S. Provisional Applications 61/097,836 filed Sep. 17, 2008 and 61/165,472 filed Mar. 31, 2009, all of which are herein incorporated by reference.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/US2009/057138 | 9/16/2009 | WO | 00 | 3/5/2011 |
Publishing Document | Publishing Date | Country | Kind |
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WO2010/033579 | 3/25/2010 | WO | A |
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Number | Date | Country | |
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20110197798 A1 | Aug 2011 | US |
Number | Date | Country | |
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61097836 | Sep 2008 | US | |
61165472 | Mar 2009 | US |