The present application claims priority from GB 2116187.2, filed in the United Kingdom, having a filing date of 10 Nov. 2021. The content of GB 2116187.2 is incorporated herein by reference for all purposes.
The present application relates to wave-propelled vehicles, in particular, to vehicles that generate forward thrust from the action of surface gravity waves present at the surface of a body of fluid.
WO 80/01674 A1 discloses a method of power production whereby the energy of the waves under the water surface in the area where a wave current exists is converted into a kinetic energy by means of blades.
Several wave-propelled vehicles are known. These vehicles exploit the approximately orbital motions of near-surface fluid particles induced by surface gravity waves travelling across a body of fluid, such as wind-induced waves travelling across an ocean, to produce forward thrust.
Both crewed and uncrewed wave-propelled vehicles have been developed. In the case of the latter, it is common to restrict the size of a given vehicle to a few metres for reasons of cost, safety, stealth, and ease of deployment and recovery. Uncrewed vehicles of this sort have application in oceanography, hydrocarbon exploration, and defence and security.
Three main types of vehicle are known.
In the first type (see, for example, WO2014009683), a floating body oscillates in any of its six degrees of freedom (but typically pitch) under the action of waves. A hydrodynamic device attached to the body at the bow or stern experiences a motion relative to the fluid locally, from which thrust may be produced. For example, an oscillating or “flapping” foil mounted to the bow or stern may be allowed to pivot relative to the body about a spanwise pitching axis in response to the local relative flow between the fluid and the body, with end stops, springs, or a combination of end stops and springs adapted to influence the foil's angle of attack to the local flow in order to generate thrust. In embodiments of this type, the floating body typically has a canoe-like hull form, and the hydrodynamic device is typically a flapping foil of a conventional planar shape, akin to an aeroplane's wing.
In the second type (see, for example, U.S. Pat. No. 7,641,524), a floating body subjected to waves experiences oscillatory motion in any of three degrees of freedom (typically heave) leading to vertical displacement of a point on the body, and an elongate member attached to and projecting downward from this point hosts a hydrodynamic device, such as a foil or an array of foils, at a distal position that moves up and down as the attachment point on the body moves up and down at the surface. Typically, the elongate member is much longer than the floating body. Because the orbital particle motions due to a surface gravity wave decay with depth (exponentially in the case of a deep body of fluid), the hydrodynamic device in this type of mechanism may experience a periodic vertical velocity different to the surrounding vertical velocity of the fluid, with the relative velocity related to the length of the elongate member. Implementations of this type of mechanism may feature a floating body designed to closely follow the surface of the fluid, i.e., a body with high hydrodynamic stiffness, such as a low-density, surfboard-like body. The elongate member may be a flexible tensile member, such as a tether.
In the third type (see, for example, WO1980001674A1), a body of significant mass and/or horizontal area is disposed below the surface to such an extent that it has little response to waves. Connected to this body by an elongate member, at a point much closer to the surface, is a hydrodynamic device such as a flapping foil, which responds to the relatively higher orbital velocities nearer the surface to produce thrust.
In relation to vehicles of the first type, it will be appreciated that such vehicles may require implementation at very long lengths in order to produce oscillatory motion that is out of phase with orbital particle velocities at the mounting location of a hydrodynamic device, and hence produce thrust, at higher periods or wavelengths. For example, out-of-phase pitching motions sufficiently vigorous for thrust production in 4 s waves could be expected to require a hull length on the order of 25 m.
In relation to vehicles of the second and third types, one skilled in the art will appreciate that the introduction of an elongate member (necessary to ensure an adequate vertical velocity differential between particles at the body and particles at the hydrodynamic device) will introduce considerable drag to the system. It will also be appreciated that where such a member is made flexible there will be scope for fouling between elements of the system; alternatively, where such a member is made rigid, there will be scope for bending and torsional failure.
A disadvantage of all three types of vehicle in ocean-going applications is their general lack of suitability for operation from time to time as underwater vehicles. For example, in some applications, such as oceanography or hydrocarbon exploration, it would be advantageous at times to operate a wave-propelled surface vehicle as an underwater glider or as an underwater powered vehicle. Current wave-propelled surface vehicles typically feature bodies with volumes much larger than the onboard systems and payloads carried in order to achieve favourable dynamics in their surface-bound wave-propelled mode, which is undesirable for an underwater vehicle. Furthermore, hydrodynamically efficient surface hull shapes typically perform poorly underwater (and vice versa).
A further disadvantage of all three types of vehicle is their general lack of suitability for aerial gliding flight.
Furthermore, all three types of vehicle employ moving parts, such as flapping foils, within hydrodynamic devices that convert local relative motion into thrust. Disadvantages of employing such moving parts include lower reliability (especially relevant when a vehicle is deployed on long endurance missions in the open ocean) and greater noise (especially relevant when the vehicle is configured to conduct acoustic sensing).
Still further, generally identifiable in wave-propelled vehicles of the prior art is at least one body designed either to maximise or minimise its response to waves, and a separate planar hydrofoil element or elements anchored to the body to convert relative oscillatory motion, between the hydrofoil element or elements and the surrounding fluid, into thrust, via a flapping motion involving resilient deformation, hinged pitching, or winglike flapping of the hydrofoil element or elements.
Allocating the wave-response and thrust-production functions to separate physical components in this manner offers the advantage of being able to optimise each element independently for its function (e.g., by optimising the body for either maximal in-phase or out-of-phase oscillatory response to waves, or for minimal response to waves, and optimising the hydrofoil element or elements for thrust production). However, this separation of functions means that each element does not tend to contribute to, and may in fact interfere with, the function of the other. For example, a body optimised for a desired wave response is, from the perspective of the thrust-production function, purely a source of drag; a planar hydrofoil optimised for thrust production is, from the perspective of the wave-response function, purely a source of damping where maximal response is desired, and purely a source of disturbance where minimal response is desired.
The desire to minimise this mutual interference in the prior art has tended to amplify the distinction in form between the separate elements. For example, a body optimised for a maximal or minimal response to waves whilst minimising drag tends to be long in the direction of travel, and short laterally; a planar hydrofoil that produces thrust efficiently tends to be short in the direction of travel, and long laterally (i.e., it tends to a high aspect ratio).
Examples will now be described, by way of example only, referring to the accompanying drawings.
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Waves travelling through the body of fluid may cause the hull 104 to oscillate in or about any of the axes defined above. At various times during relative motion between the hull 104 and the surface 106, parts of the hull may alternately submerge below or broach the surface 106. An upper extent 114 and a lower extent 116 of this “dynamic immersion” of the hull may be defined, thus defining an upper hull portion 118 of the hull; a lower hull portion 120 of the hull is defined as that portion of the hull below the lower extent 116 of dynamic immersion.
Within the specification and relating to all examples, the upper hull portion can be defined as that portion of the hull that periodically plunges through the free surface of the body of fluid under the action of surface waves; the upper hull portion comprising a hydrofoil portion.
Similarly, within the specification and relating to all examples, the lower hull portion can be defined as that portion of the hull that remains below the free surface despite the action of the surface waves; the lower hull portion comprising a hydrofoil structure; the hydrofoil structure comprising a hydrofoil portion.
The surface waves can have a given character describable, by way of example only, according to any of the following taken jointly and severally in any and all permutations: a peak period; a zero-crossing period; a significant wave height; a mean wave height; a non-directional wave spectrum; and a directional wave spectrum.
Together, the upper hull portion 118 and the lower hull portion 120 of the hull define the operative volume 122 of the hull.
The upper hull portion 118 has a leading position 124; a leading position of the hull or of a portion of the hull is a prominently positioned forward location of the hull, which would be recognised by one skilled in the art as falling, by way of example only, on the leading edge of a hydrofoil portion of the hull. Projected onto a frontal plane of the vehicle, the set of all the leading positions of the hull, or of a continuous portion of the hull, forms a continuous one-dimensional, two-dimensional, or both one- and two-dimensional figure. By way of example, the leading edge of a hydrofoil portion with a rounded or sharp leading edge would form a one-dimensional figure (i.e., a curve) when projected in this way; the leading positions of a longitudinally aligned cylinder would form a circular disc when projected in this way.
The lower hull portion 120 of the hull has a trailing position 126; a trailing position of the hull or a portion of the hull is a prominently positioned rearward location of the hull, which would be recognised by one skilled in the art as falling, by way of example only, on the trailing edge of a hydrofoil portion of the hull. Projected onto a frontal plane of the vehicle, the set of all the trailing positions of the hull, or of a continuous portion of the hull, forms a continuous one-dimensional, two-dimensional, or both one- and two-dimensional figure. By way of example, a perfectly sharp trailing edge of a hydrofoil portion would form a one-dimensional figure (i.e., a curve) when projected in this way; the trailing positions of a longitudinally aligned cylinder would form a circular disc when projected in this way.
The observations made above relating to the vehicle 102 of
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It will be further appreciated that, as any of the vehicles according to the examples described experiences oscillatory motion, one or more than one hydrofoil portion of the vehicle may generate thrust. For example, a hydrofoil portion may experience a time-varying angle of attack and velocity relative to the surrounding fluid such that, on average, the hydrofoil portion generates thrust in the direction of travel, as one skilled in the art will appreciate from steady-state aerodynamic and hydrodynamic theory. Alternatively, thrust production by an oscillating hydrofoil portion may be considered as being due to the creation of a favourable (i.e., thrust-producing) unsteady wake, such as a reverse von Kármán street of shed vortices.
It will be further appreciated that, for any of the vehicles according to the examples described, the lower hull portion comprises a hydrofoil structure comprising one or more than one hydrofoil portion. The hydrofoil structure of the lower hull portion is substantially non-planar, providing a vertically directed concavity when viewed from the front or rear of the vehicle. By way of example only, such a concavity may exist where, if all leading or all trailing positions of the hydrofoil structure of the lower hull portion are projected onto a frontal plane of the vehicle, there exists two points of equal altitude on the projection, such that an area is generally defined by the projection and a horizontal line segment connecting the two points.
It will be further appreciated that, for any of the vehicles according to the examples described, the non-planar arrangement of the hydrofoil structure of the lower hull portion can improve the efficiency with which a given hydrofoil portion produces thrust, reducing drag or damping that might otherwise be present due to the tip losses generally experienced by thrust-producing, low aspect ratio, planar hydrofoils. This enables efficient realisation of large hydrofoil chords relative to the length of the vehicle, such that small amplitude rotational oscillations of the vehicle may correspond to relatively large trailing edge motions. Large-amplitude trailing edge motions will be recognised as desirable for flapping foil propulsion under various operating conditions of a vehicle.
It will be further appreciated that, for any of the vehicles according to the examples described, the hydrofoil structure of the lower hull portion is substantially rigid, in that no hydrofoil portion of the hydrofoil structure moves relative to any other. However, it will be appreciated that any hydrofoil portion of a hydrofoil structure of the lower hull portion according to the invention may be made resiliently deformable, or allowed to pitch about a spanwise axis, or to flap about a chordwise axis, without departing from the scope or spirit of the invention. Accordingly, any concavity or channel formed by the hydrofoil structure may vary its shape during operation of the vehicle without departing from the scope or spirit of the invention.
It will be further appreciated that a hydrofoil portion having vertical extent of the lower hull portion of any of the vehicles according to the examples described may be conveniently extended to provide an element of the upper hull (for example, by extending said hydrofoil portion up through the equilibrium free surface). This allows the resulting vertically extending hydrofoil portion of the upper hull portion to provide a hydrodynamic stiffness component of the vehicle's wave response dynamics. It will be appreciated that such a vertically extending hydrofoil portion of the upper hull portion may provide hull volume about the free surface with great hydrodynamic efficiency, i.e., low drag in forward motion. It will be appreciated that extending a hydrofoil portion in this way means that a tip of the hydrofoil portion may be prevented from exposure to the fluid, reducing tip losses where the hydrofoil portion is thrust-producing.
It will be further appreciated that, for any of the vehicles according to the examples described, one or more than one hydrofoil portion, having vertical extent, horizontal extent, or a combination of vertical and horizontal extents, of the upper hull portion may account for all of the volume of the upper hull portion. This has the benefit that time-varying hydrodynamic, hydrostatic, or combined hydrodynamic and hydrostatic forces applied to the upper hull portion due to the action of waves may act on the upper hull portion with minimal resistance to forward motion. It will be appreciated that further examples of the invention may be realised wherein simply a substantial proportion of the volume is accounted for by said hydrofoil portion or portions of the upper hull portion, for example, a majority of the volume. Therefore, it will be appreciated that the examples can provide a blended body that simultaneously performs the dual functions of providing a wave-responsive body and thrust-producing hydrofoils. The blended body can be a unitary body.
It will be further appreciated that a hydrofoil portion of any of the vehicles according to the examples described may have an aerofoil cross-section, for example, a NACA symmetrical aerofoil cross-section, such as a NACA0015 aerofoil cross-section. It will be further appreciated that a hydrofoil portion of any of the vehicles may have some other fine cross-section, that is, a cross-section that has a low ratio of thickness to chord, such as a thin plate cross-section. Such cross-sections may, for example, have thickness to chord ratios of 2% to 30%. One skilled in the art will appreciate that for hydrofoil portions bisected by the free surface in operation, it may be desirable to adopt a cross-section with a sharp (rather than a rounded) leading edge, to minimise wave-making resistance.
It will be further appreciated that, as a converter of wave power to oscillatory motion, the vehicle may be roughly considered a bandpass filter on the waves, with the effective upper and lower cut-off frequencies dependent, in the example of heave, on: the density of the fluid (D_F); a representative waterplane area (A_W) of the upper hull portion during dynamic immersion; the mass (M_V) of the vehicle; and the added mass (M_A) of the vehicle in heave, taking care to account for the endplate-like effects of the concavity of the lower hull portion; the foregoing being taken jointly and severally in any and all permutations. For heave, the frequency of minimum attenuation, (OMEGA), in radians per second (which is the natural frequency of the vehicle in heave), can be approximated by the following relation: OMEGA=SQUARE_ROOT (D_F*A_W/(M_V+M_A)). OMEGA should be designed to fall close to the vehicle's frequency of encounter, in radians per second, with the waves in which the vehicle is to operate. One skilled in the art will appreciate that the formula provided above is an approximation, and that, in particular, the approximation of the hydrodynamic stiffness by the term D_F*A_W does not account for changes to waterplane area during heave motion. It will be appreciated that another method for the determination of an approximate natural frequency, such as a method based on numerical analysis, may provide greater accuracy. It will also be appreciated that natural frequencies in other oscillatory modes, such as roll and pitch, respectively, may be determined using similar approximate formulae (based on rotational rather than translational stiffness in the numerator term, and the summation of vehicle and added inertias rather than masses in the denominator term, in the case of a rotational oscillatory mode), or using other established methods of the art, and that the observations made above in relation to heave may be applied mutatis mutandis to these other modes of oscillation.
It will be further appreciated that, for any of the vehicles according to the examples described, a vertically directed concavity of the lower hull portion may act to increase added mass and/or inertia, relative to a vehicle without such a concavity. The effect of added mass or inertia is to reduce the resonant frequency of the vehicle in a given mode of oscillation, so this property may be desirable when a relatively small vehicle is intended to operate in waves of relatively large wavelength and correspondingly long period. One will appreciate that the potential benefits of added mass in this sense may be realised without a large drag penalty in forward motion, as fluid may flow freely through the concavity longitudinally.
It will be further appreciated that, because the centre of gravity of any of the vehicles according to the examples described may be disposed closer to the front than to the rear of the lower hull portion, heave oscillation may be coupled to, for example, pitch oscillation (due to the centre of hydrodynamic pressure in heave tending to act behind the centre of gravity). Further features may act to synchronise the phases of oscillatory modes. For example, the centre of volume of the upper hull portion may be disposed ahead of the centre of gravity, so that restoring forces tend to act forward of the centre of gravity on a downward heave motion, synchronising the downward and nose-down phases of heave and pitch oscillation respectively. Enhancing the degree of coupling between, and synchronising the phase of, for example, heave and pitch motions as described will be recognised as desirable for flapping foil propulsion It will be appreciated that other motions could be coupled such as, for example, roll and sway motions or yaw and sway motions in addition to the foregoing heave and pitch motions.
It will be further appreciated that, for any of the vehicles according to the examples described, the centre of gravity may be disposed by a distance above or below the centre of buoyancy in order to tune an oscillatory mode of the vehicle, in particular the roll or pitch mode of the vehicle, to a given wave condition. This distance may be predetermined, or it may be configured during operation using, for example, a buoyancy control system or a mass shift system.
It will be further appreciated that, in addition to tuning oscillatory modes of any of the vehicles according to the examples described to a given wave condition, it may be desirable to tune such modes to each other, for example, to set the parameters of the vehicle in terms of translational hydrodynamic stiffness in a given axis, rotational hydrodynamic stiffness about a given axis, mass, added mass in a given axis, inertia about a given axis, and added inertia about a given axis, such that natural frequencies in two or more than two modes of oscillation coincide with each other, for maximal wave excitation at their common natural frequency; the foregoing being taken jointly and severally in any and all permutations.
It will be further appreciated that it may, as an alternative, be desirable to offset the natural frequencies of two or more than two oscillatory modes, in particular, heave and pitch. It may be desirable, for example, to position the centre of gravity above the centre of buoyancy in order to produce a vehicle that is relatively tender in pitch. As the vehicle heaves, coupling due to, for example, a forwardly disposed centre of gravity, as described above, causes the vehicle to pitch; if the vehicle is relatively tender in pitch, restoring moments in pitch are relatively weaker, and the vehicle may pitch and heave more under certain conditions than it would if it were relatively stiff in pitch. Under these conditions, this may result in higher amplitude motions of the trailing edge of a hydrofoil portion, which will be recognised as desirable for flapping foil propulsion.
It will be appreciated that the corollary of the desirability of tuning the vehicle and controlling the coupling of its modes in the ways described above is that it may be particularly undesirable not to do so. For example, attempting to operate the vehicle in waves of period substantially longer than a natural period of the vehicle, particularly in heave, may yield little appreciable wave propulsion. By way of further example, attempting to operate the vehicle in waves of period substantially shorter than a natural period of the vehicle, particularly in heave, may also yield little appreciable wave propulsion. In particular, in the latter case, Stokes drift may overwhelm the vehicle's ability to make headway in head seas. These observations in relation to heave may be applied mutatis mutandis to other modes of oscillation, particularly roll and pitch, taken jointly and severally.
It will be further appreciated that vehicles according to the invention may comprise further features beyond the operative volume of the hull. For example, a vehicle may comprise a superstructure that never plunges through the free surface during operation at a design wave condition. One skilled in the art will appreciate that, other than contributing mass and inertia to the vehicle as a whole, such features will not appreciably influence wave propulsion. Such features may, however, be important in eliminating the possibility of capsizing during extreme weather events.
Finally, it will be appreciated that vehicles according to the examples described are capable of efficiently combining the wave-response and thrust-production functions in a single form, reducing the need for moving parts and providing a hydrodynamically cleaner vehicle better adapted to other modes of locomotion, including sub-surface and above-surface flight, relative to the prior art.
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An example has been realised, based on the vehicle depicted in
In the example, the aerofoil section used is a NACA0015 section, and the approximate mass of the vehicle is 53.4 kg. The example makes good headway in regular waves of period 2.0 s and amplitude 0.1 m.
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The heaving and pitching of, in particular, the lower hull portion 506 of the vehicle 502 generates thrust. Examples can be realised in which the thrust is associated with an unsteady wake such as, for example, a reverse von Kármán street of vortices, four of which vortices 710 to 716 are shown in
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Examples can be realised in which the thrust is associated with an unsteady wake from at least one hydrofoil portion of the hull, such as, for example a reverse von Kármán street of vortices, two examples 818 and 820 of which are shown in
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The set of solar energy harvesting panels 1012 is arranged to generate and store electricity from sunlight in a battery (not shown). The stored energy can be used to drive any onboard electrical or electronic systems of the vehicle 1010.
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It will be appreciated that providing an empennage supports an aerial gliding flight mode of operation. This mode of operation is desirable for rapid aerial deployment of one or more than one vehicle to a specific location or locations on the surface, for example, for the purposes of monitoring large scale features in oceanographic applications, or for rapidly assessing large areas in defence and security applications.
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Examples may be realised whereby the hydrofoil portions of the vehicle's hull act as lifting surfaces in underwater powered or gliding flight. In underwater gliding flight, the control surface 1218 may be used to steer the vehicle.
The pressurised hull 1208 forms part of a buoyancy control system, described with reference to
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The upper-most compartment, that is, compartment 1802, may contain water or air. When the vehicle 1206 is at the surface of a body of water, water may be exchanged for air and vice-versa through a simple valve and pump (not shown).
A pair of middle compartments 1804 and 1806 is provided to give buoyancy to the vehicle 1206. The compartments 1804 and 1806 can be filled with a foam such as, for example, a syntactic foam. The foam can have a density that is lower than that of water to provide positive buoyancy.
A pair 1808 and 1810 of further compartments is provided. The compartments 1808 and 1810 are free-flooding compartments. The free-flooding compartments 1808 and 1810 may contain either water or a buoyancy control working fluid. The buoyancy control working fluid can comprise a mineral oil, or other liquid that is substantially incompressible and preferably less dense than water. The buoyancy control working fluid may be pumped into or out of a bladder 1814 to populate or evacuate corresponding bladders (not shown) in the compartments 1808 and 1810. When the buoyancy control working fluid is pumped into the bladder within each of the compartments 1808 and 1810, water within the compartments 1808 and 1810 is displaced into the ambient water surrounding the vehicle 1206.
The lowest compartment 1812 is a pressure hull. The pressure hull 1812 is filled with air but for the bladder 1814, which is arranged to store a volume of buoyancy control working fluid. The buoyancy control working fluid stored in the bladder 1814 can be pumped into the bladders (not shown) within the compartments 1808 and 1810. Conversely, the buoyancy control working fluid may be evacuated from the bladders (not shown) within the compartments 1808 and 1810 into the storage bladder 1814.
When the vehicle is operating at the surface, the upper compartment 1802 is filled with air, and the buoyancy control compartments 1808 and 1810 are filled with water. The vehicle 1206 is arranged to be positively buoyant in this condition.
When the vehicle 1206 is required to dive, the upper compartment 1802 is filled with water, that is, the air is discharged and the vehicle 1206 becomes negatively buoyant. The negative buoyancy allows the vehicle 1206 to dive. The direction of travel during the dive can be controlled by the supplementary thrusters and/or hydrodynamic control surfaces.
When the vehicle is required to ascend, the buoyancy control working fluid stored within the storage bladder 1814 is pumped into the bladders within the buoyancy control compartments 1808 and 1810, which displaces any water within those compartments 1808 and 1810 into the surrounding environment. The resulting effect is that the vehicle 1206 becomes positively buoyant. Once the vehicle broaches the surface, the upper compartment 1802 can be filled with air by expelling the water it contains into the surrounding environment, which further increases the overall buoyancy of the vehicle 1206. The buoyancy control working fluid can then be pumped out of buoyancy control compartments 1808 and 1810 into the storage bladder 1814, which allows the buoyancy control compartments 1808 and 1810 to be filled with water again.
One skilled in the art will appreciate that the operation of a buoyancy control system such as that described may act to alter at least one, or both, of: the centre of gravity position or mass of the vehicle. It will be appreciated that such an alteration may be used when the vehicle is at the surface to dynamically improve, preferably optimise, the vehicle's wave response dynamics to suit ambient waves, especially through the use of an air compartment such as the upper compartment 1802 in the example provided. In particular, it will be appreciated that control of at least one of the following taken jointly and severally in any and all permutations: the vertical position of the centre of gravity of the vehicle relative to the vertical position of the centre of buoyancy of the vehicle, the mass of the vehicle, inertia in the roll direction and inertia in the pitch direction, can be used to effectively tune the response of the vehicle, for example, in at least one, or both, of: pitch and roll. It will be noted that the mass and centre of buoyancy are related such that when the mass is increased, the vehicle becomes more submerged and the centre of buoyancy lowers, and vice versa. It will be appreciated that an alteration of the longitudinal or lateral position of the centre of gravity, as is common for other marine and air vehicles, such as underwater gliders and hang gliders, may be used to effect any combination of at least one or more than one of: lateral, longitudinal, and directional control when on the surface or when below the surface taken jointly and severally in any and all permutations. Finally, one skilled in the art will appreciate that alternatives to a buoyancy control system may be used to effect a centre of gravity alteration, for example, a mass shift system may be used to do so.
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The examples described herein can be deployed and left in theatre or on task for long durations since the movement is wave-powered. Being wave-powered allows the vehicles to autonomously perform a task on site and then drift to a collection point or base under wave-power. Any example vehicle described herein can be arranged to dive and operate beneath the thermocline of a body of fluid.
Example vehicles described and/or claims herein can provide a single form to efficiently perform both the wave-response and thrust-production functions whilst reducing or eliminating the need for moving parts, increasing simplicity and robustness, and generally improving performance relative to the prior art.
Examples can be realised according to any of the following clauses:
Further examples can be realised according to any of the following clauses:
Number | Date | Country | Kind |
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2116187.2 | Nov 2021 | GB | national |
Filing Document | Filing Date | Country | Kind |
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PCT/GB2022/052859 | 11/10/2022 | WO |