WO2004092009A1 - A Wing ASSEMBLY CAPABLE OF INCREASIGN THE LIFT AND THE ANGLE OF STALL - Google Patents

A Wing ASSEMBLY CAPABLE OF INCREASIGN THE LIFT AND THE ANGLE OF STALL Download PDF

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Publication number
WO2004092009A1
WO2004092009A1 PCT/CN2003/001035 CN0301035W WO2004092009A1 WO 2004092009 A1 WO2004092009 A1 WO 2004092009A1 CN 0301035 W CN0301035 W CN 0301035W WO 2004092009 A1 WO2004092009 A1 WO 2004092009A1
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Prior art keywords
wing
canopy
angle
stall
lift
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PCT/CN2003/001035
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French (fr)
Chinese (zh)
Inventor
Shangxiang Zhu
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Shangxiang Zhu
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Publication date
Application filed by Shangxiang Zhu filed Critical Shangxiang Zhu
Priority to AU2003289606A priority Critical patent/AU2003289606A1/en
Publication of WO2004092009A1 publication Critical patent/WO2004092009A1/en

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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B64AIRCRAFT; AVIATION; COSMONAUTICS
    • B64CAEROPLANES; HELICOPTERS
    • B64C3/00Wings
    • B64C3/38Adjustment of complete wings or parts thereof
    • B64C3/54Varying in area

Definitions

  • the present invention relates to aeronautical technology, and more particularly, to a canopy wing that can be used in an aircraft to increase lift and stall angle of attack.
  • the prior art lifting devices are mainly as follows:
  • the most common devices are various types of flaps, including slotted flaps in the early stages of aircraft development, and Fuller flaps and Kruger flaps, which were later invented in succession.
  • Fuller flaps are flaps mounted on the trailing edge of the wing.
  • Kruger flaps are flaps mounted on the leading edge of the wing.
  • the vortex generator device is used to change the laminar flow field to a turbulent flow field at the leading edge or upper airfoil of the wing, so that the airflow on the upper airfoil can obtain greater kinetic energy, realize delayed separation and maximize the lift coefficient.
  • Increased desire But in fact, it did not work as expected, because the result of this increase was to pay a lot of resistance for the price, and this effect
  • the technical problem to be solved by the present invention is that the invention is to find a new way to address the shortcomings in the search for increasing methods, and proposes a new measure that is completely different from the currently used methods in order to obtain a large Good aerodynamic characteristics to improve lift and retard stall.
  • the technical solution adopted by the present invention to solve its technical problems is:
  • the invention adopts a canopy wing, which adopts a sheet structure called a canopy wing, which is installed above the upper wing surface of the wing, and approaches without touching the upper wing. Face, as if a awning covered the upper surface of the wing. Because an airflow channel is formed between the wing and the upper surface of the wing, the airflow from the far front to the upper wing surface is restricted, so that the airflow above the faster wing surface is concentrated under the wing In the channel. Compared with the flow situation where no wing exists, the kinetic energy of the airflow flowing through the upper surface of the wing is greater, so that the airflow divergence point is moved to the rear greatly.
  • the lift coefficient is increased (including the linear segment).
  • the stall angle of attack is greatly increased, so that the maximum lift coefficient is increased, and the purpose of a substantial increase is achieved. It is worth noting that after the use of the wing, the original laminar flow was not converted into a turbulent surface layer, but the laminar flow was maintained. At the same time, the thickness of the canopy wing is small, so the resistance does not increase much, and the lift-drag ratio remains within a reasonable range. Because the canopy is just a thin wing with the same or similar curvature to the upper wing surface, the type resistance is very small, but the frictional resistance is increased. This is the only price, compared with a substantial increase in lift and stall angle of attack.
  • the structure of the canopy wing requires great rigidity, and it is necessary to choose a suitable lightweight and rigid material. From the structural design, it can be considered that the canopy wing is made into an ultra-thin airfoil with a reinforcing rib and a streamlined shape. Fortunately, the force of the wing It is a force type of simply supported beam, which is beneficial to structural design and process manufacturing. In order to further increase the stall angle of attack, another oblique wing structure is proposed. This structure is aerodynamically different from the top-mounted monolithic canopy. However, it can also make the air flow separation point move backward greatly, and the increase of the stall angle of attack greatly exceeds the increase of the stall angle of attack of the combined wing of the top wing. BRIEF DESCRIPTION OF THE DRAWINGS
  • FIG. 1 is a schematic diagram of an upper-mounted canopy wing installed on the wing.
  • Fig. 2 is a schematic diagram of an inclined canopy wing installed on the wing.
  • Figure 3 is a wind tunnel test curve using NACA23012 airfoil as the basic wing and fuselage combination.
  • Fig. 4 is a schematic diagram of another embodiment in which the leading edge of the wing can be deflected downward.
  • Fig. 5 is a schematic diagram of the air flow along the wing section after the canopy wing is installed.
  • Fig. 6 is a first embodiment of the present invention: an upper canopy aircraft.
  • Fig. 7 is another embodiment of the present invention: an inclined canopy aircraft.
  • FIG. 8 is a schematic diagram of the relative positions of the canopy wing and the main wing of the present invention.
  • the canopy wing 1 is located above the upper wing surface 3 of the wing 2.
  • the leading and trailing edges of the wing and the wing are parallel to each other along the wingspan, but along the chord direction, the distance between the lower surface of the wing and the upper surface of the wing is not necessarily equal.
  • 3 ⁇ 4 is the relative height of the leading edge of the wing and the wing.
  • ⁇ 3 ⁇ 4 the wing has a mounting angle ⁇ relative to the wing.
  • the angle ⁇ is the angle between the line connecting the leading and trailing edges of the wing and the wing chord.
  • the change in ⁇ (usually a positive value) is achieved by changing 3 ⁇ 4 (fixed).
  • the size of 3 ⁇ 4 will affect the effect of increasing this device. Calculations, analysis and wind tunnel tests have shown that: The value must be carefully selected. It cannot be too small or too large. Too small, it may hinder the flow of air flow between the wing and the upper airfoil, and the lifting effect is not good. Too big will make the structure difficult. It will also reduce the efficiency fruit. It must be optimized experimentally to determine an optimal value. Preliminary wind tunnel tests have shown that the minimum value is approximately 10% of the wing aerodynamic chord length.
  • the curvature of the upper airfoil 3 must be taken into consideration, and the hinges 9 and 10 should ensure that the inclined wing 5 and 6 can be smoothly opened and retracted.
  • One end of the inclined canopy wings 5 and 6 shown in FIG. 2 is connected to the upper wing surface of the wing 2, and the other end is separated from the upper wing surface by a certain distance. This distance determines the upper anti-angle ⁇ between the inclined wing and the wing.
  • the inclined wing When using the inclined wing, if it is used for low-speed aircraft, it can be fixed and not retracted. That is, the wing is opened during the entire flight. This approach greatly simplifies the structure. When used in supersonic aircraft, it should be designed as a retractable inclined wing. When it is not necessary to use the wing, the wing 5 and 6 should be retracted by using a hydraulic mechanism or other transmission device, and placed in the square grooves 7 and 8 in the wing, which fully fits the upper wing surface of the wing. Maintain a complete single wing profile.
  • FIG. 3 is a result of a wind tunnel test performed to compare the raising effect of the wing. It mainly shows the change of lift and stall angle of attack in three cases.
  • the wind tunnel test model used is based on the NACA23012 airfoil, mounted on a cylindrical fuselage, and the fuselage head has an oval shape.
  • the result given is the aerodynamic characteristics of a "wing-in-body" assembly.
  • curve 12 is the change in the lift coefficient of the base structure 15 with the angle of attack
  • the stall angle of attack is about 12 °
  • the maximum lift coefficient is about 0.94.
  • Curve 13 is the lift characteristic curve of the "wing-one" combined body 16 after the upper-type canopy is installed.
  • the stall angle of attack is approximately 20 °.
  • the maximum lift coefficient is approximately 1.6.
  • Curve 14 is the lift characteristic curve of the "wing-in-body" combination 17 after the inclined wing is installed. 4 ⁇ Stall angle of attack of 30 degrees or more (due to conditions, no test greater than 30 ° angle of attack.)
  • the maximum lift coefficient is about 1.4.
  • the interesting phenomenon is that in this form of inclined canopy wing, the lift characteristics are basically unchanged after installing the inclined canopy in a linear range smaller than the stall angle of attack.
  • the above experimental results are limited to 1 / 2-2 Canopy wings on / 3 wingspan. (Note: Resistance and thrust moment characteristics Also unchanged. (Not shown in the figure) Compared with the existing lifting technology, the effect of increasing the maximum lift coefficient and the stall angle of attack of the present invention is greatly ahead.
  • FIG. 4 shows another form of the upper wing: The front edge portion 18 of the wing can be deflected downward. This type of increase effect was tested in a wind tunnel test, and it was found that a downward deflection of 18 would increase the stall angle of attack to 25 °, but the maximum lift coefficient was slightly reduced.
  • Figure 4 also shows that the trailing edge portion 23 of the wing flap can also be deflected downward.
  • FIG. 5 shows a two-dimensional flow picture of the airfoil, with the airfoil 1 placed above the airfoil surface of the airfoil section 11.
  • Zone 1 is located below the lower airfoil of the basic airfoil, and its flow is basically the same as when the wing is not installed. Because the lower airfoil has less curvature and is flat, the air velocity is slower and the pressure is greater.
  • Zone 3 is located between the upper surface of the base airfoil and the lower surface of the wing, forming a duct. Air flows into this area to be further accelerated. The accelerated airflow cannot pass through the wing to the outside, thus maintaining a relatively The large kinetic energy delays the separation of the airflow. Due to the high flow velocity, the pressure in zone 2 is lower than in zone 1.
  • Zone 2 leads to the free flow field above the upper surface of the wing. Because the curvature of the wing is basically the same as the basic airfoil, but larger than the lower wing surface, the airflow is accelerated, and the pressure is relatively low. Because the wing is located between the two low-pressure zones 2 and 3, its force depends on The pressure difference between these two zones. We expect that the faster the flow speed in zone 3, the better and the pressure will become smaller. The airflow is also accelerated when it passes around the wing to Zone 2. It may be faster than Zone 3 and the pressure is very small. It can be inferred that the pressure difference between Zone 3 and Zone 2 is much smaller than Zone 1 and Zone 3. Therefore, the direct force of the wing will not be too great.
  • FIG. 6 is an embodiment of the upper canopy wing.
  • the canopy wings 1 and 13 are placed above the upper wing surfaces of the left and right wings 2 and 14.
  • 19 is the front support rod of the transmission device that pushes and retracts the wing. There can be several. Keep all front poles at the same height when pushing out.
  • the height of the front support rod protruding from the upper airfoil is adjustable.
  • 20 is similar to 19, it is the rear support.
  • the installation angle of the canopy wing with respect to the wing can be achieved by adjusting the protruding height of the front support rod 19.
  • 12 is any kind of aircraft, but also other transportation machinery in the atmosphere or water. Fig.
  • the canopy wings 5, 6, 15 and 16 are placed obliquely on the upper surface of the wing at an upside-down angle.
  • the canopy wing can be stowed and stretched.
  • the tilting canopy can be opened and retracted through a known transmission mechanism to push out or retract the actuator cylinder rod 21. It can also be used in current aircraft.
  • the way of launching the hydraulic actuating mechanism of the spoiler is to realize the retracting of the inclined wing. When retracting, store the wing in the square grooves 7, 8, 17, and 22 on the surface of the wing, so that it fits perfectly with the upper surface of the wing, keeping the original First base airfoil profile.
  • the geometry of the wing and the relative position of the wing and the main wing are not limited to those shown in the implementation forces listed in the above description.
  • the following situations will occur: From the perspective of a certain profile airfoil, the starting point of the leading edge of the canopy wing can be located at a position later than the leading edge of the aerodynamic chord of the main wing; .
  • 23 is a wing on the wing.
  • the wing of the larger aircraft can be divided into several shorter segments adjacent to each other. These fragments of the wing are coordinated and synchronized to be operated and retracted through electrical or mechanical connections between electrical, hydraulic, or mechanical mechanisms to replace the entire wing.
  • This multi-structure form can be applied to parallel wing and inclined wing.
  • the wing is not limited to the application on the main wing, but can also be applied to the normal or duck-type horizontal stabilizer or full-motion control surface.
  • the application of the canopy is not limited to the two embodiments described above.
  • the invention may include many uses, not limited to various aircraft, may be a recovery device for spacecraft returning to the ground, may be a ground effect aircraft, or may be a machine moving in water or any other fluid. Utilizing the good high angle of attack characteristics of the inclined wing to design the anti-rotation device will greatly increase the safety of the aircraft.

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  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Aviation & Aerospace Engineering (AREA)
  • Aerodynamic Tests, Hydrodynamic Tests, Wind Tunnels, And Water Tanks (AREA)
  • Structures Of Non-Positive Displacement Pumps (AREA)

Abstract

A wing assembly has a sheet structure for increasing the lift and the angle of stall. The sheet structure locates above the wing or slopes upwards. The upper sheet can pivot with the trailing edge of the wing. The anhedral of slant sheet also can vary. The sheet is capable of being released or retracted or changed its configuration as required. A duct is formed between the sheet and the upper surface of the wing, and the airflow in the said duct accelerates and has great kinetic energy, which significantly increases the maximum lift coefficient and the angle of stall. Before optimizing, the maximum lift coefficient can increase more than 70% and the angle of stall can increase over 18 degree. The principle of present invention is novel and the structure thereof is simple, so it can be widely used in civil aircraft military aircraft and other machinery which can move in the fluid.

Description

一种增加升力和失速迎角的篷翼 技术领域  Canopy wing for increasing lift and stall angle of attack
本发明涉及航空技术, 更具体地说, 涉及一种可用于航空飞行器上增加升 力和失速迎角的篷翼。 背景技术  The present invention relates to aeronautical technology, and more particularly, to a canopy wing that can be used in an aircraft to increase lift and stall angle of attack. Background technique
为了使飞行器在低速飞行时获得足够的升力, 几乎所有的飞机都安装了增 升装置。 现有技术的增升装置主要有如下几种: 最通常的装置是各种类型的襟 翼,包括飞机发展早期的开缝襟翼以及后来相继发明的富勒襟翼和克鲁格襟翼。 富勒襟翼是安装在机翼后缘的襟翼。 克鲁格襟翼是安装在机翼前缘的襟翼。 按 结构分类有许多类型, 如分裂襟翼, 简单襟翼、 开缝襟翼。 这些襟翼的主要作 用是增加翼型的弯度, 使机翼上面的气流延缓分离, 从而使升力系数增加, 特 别是使失速迎角及最大升力系数增加。 除此以外, 还有喷气襟翼的装置和吸气 襟翼的装置, 用于控制附面层, 进一步延缓气流分离。 上述装置已经获得了良 好的效果, 使飞机的最大升力系数和失速迎角大大增加。 为进一步增大升力, 以便縮短飞机起飞滑跑距离和具有更好的失速特性, 喷气襟翼技术从理论上是 十分有效, 但结构复杂, 还要从引擎中引出喷流到机翼上, 消耗了能量, 高温 气体引到机翼表面, 对材料, 结构要求很高, 所以至今应用不普遍。 在如何进 一步获得更高的升力系数方面, 国内外近年来有许多科学家作了大量努力。 其 中, 有美国专利 563461, 5772155 , 63186771和 6302360和本发明的目的最接 近。 这几份专利公开了一种利用旋涡来改变机翼上翼面的气流流动特性, 试图 达到延缓气流分离, 使失速迎角和最大升力系数增加。 国内专利 94226631, 98201185和 89207887分别提出了利用捕涡机翼, 利用喷气动力和环翼来增升 的方法。 但是, 上述所有努力的效果都很小。 其中, 利用旋涡发生器装置在机 翼前缘或上翼面, 企图将层流流场改变成紊流流场, 使上翼面的气流获得更大 的动能, 实现延缓分离和使最大升力系数增加的愿望。 但实际上, 事与愿违, 因为这种增升的结果是花了使阻力增加很多作为代价换取的, 而且, 这种效果  In order to obtain sufficient lift when the aircraft is flying at low speed, almost all aircraft are equipped with lifting devices. The prior art lifting devices are mainly as follows: The most common devices are various types of flaps, including slotted flaps in the early stages of aircraft development, and Fuller flaps and Kruger flaps, which were later invented in succession. Fuller flaps are flaps mounted on the trailing edge of the wing. Kruger flaps are flaps mounted on the leading edge of the wing. There are many types by structure, such as split flaps, simple flaps, slotted flaps. The main function of these flaps is to increase the camber of the airfoil, to delay the separation of the airflow above the wing, thereby increasing the lift coefficient, especially the stall angle of attack and the maximum lift coefficient. In addition, there are devices for jet flaps and devices for suction flaps, which are used to control the surface layer and further delay the separation of airflow. The above device has achieved good results, which has greatly increased the maximum lift coefficient and stall angle of attack of the aircraft. In order to further increase the lift, in order to shorten the take-off and run-off distance of the aircraft and have better stall characteristics, the jet flap technology is theoretically very effective, but the structure is complex, and it is necessary to draw the jet from the engine to the wing, which consumes With energy, high-temperature gas is introduced to the surface of the wing, which requires high materials and structures, so it has not been widely used so far. In terms of how to obtain a higher lift coefficient, many scientists at home and abroad have made great efforts in recent years. Among them, there are U.S. patents 563461, 5772155, 63186771, and 6302360 which are closest to the object of the present invention. These patents disclose a method of using vortices to change the airflow characteristics of the upper airfoil of the wing in an attempt to delay the separation of the airflow and increase the stall angle of attack and the maximum lift coefficient. Domestic patents 94226631, 98201185, and 89207887 have proposed methods of using vortex trapping wings, jet power, and ring wings to increase the lift. However, the effect of all the above efforts is small. Among them, the vortex generator device is used to change the laminar flow field to a turbulent flow field at the leading edge or upper airfoil of the wing, so that the airflow on the upper airfoil can obtain greater kinetic energy, realize delayed separation and maximize the lift coefficient. Increased desire. But in fact, it did not work as expected, because the result of this increase was to pay a lot of resistance for the price, and this effect
1 1
确 认 本 并不显著。升力的增加不多, 失速迎角的增大也十分有限。可以说, 此路不通。 发表在 1998年 2月号的 "北航学报"上有一篇论文: 《旋涡发生器对机翼最大 升力和失速迎角影响》。 该文曾详细地对利用旋涡发生器增升方法进行了评论, 指出了上面提到的问题。 因此, 需要从其他途径, 找到真正有效的增升方法。 利用旋涡方法增升只有微弱效果这一事实, 可以从最近的一份美国专利 63186771 (2001年 11月)证实。 该文件公开了利用 "老鹰尖嘴式"旋涡发生 器来使 172机翼增升的效果, 给出了数据, 曲线和图表, 并进行了比较。 从公 布的结果可以明显看出: 装与不装鹰嘴旋涡发生器对失速迎角以及升力系数几 乎没有改变, 只看到失速之后的过失速特征略有改善。 发明内容 Confirm this Not significant. There is not much increase in lift, and the increase in stall angle of attack is also very limited. It can be said that this road is not working. A paper published in the February 1998 issue of the Journal of Beihang University: "Effect of Vortex Generators on Maximum Lift and Stall Angle of Attack of Wings" This article has commented in detail on the use of vortex generator lifting methods and points out the problems mentioned above. Therefore, we need to find other effective ways to increase. The fact that the vortex method has only a slight effect on the increase can be confirmed by a recent US patent 63186771 (November 2001). This document discloses the effect of using the "eagle-tip-nosed" vortex generator to raise the 172 wing. The data, curves and charts are given and compared. From the published results, it is obvious that the angle of attack and the lift coefficient of the stalled and unmounted garrule vortex generators have hardly changed. Only the stall characteristics have been slightly improved after the stall. Summary of the invention
本发明要解决的技术问题在于, 发明是针对目前在寻求增升方法上存在的 缺点而另辟新途径, 提出了一种新的与目前大量使用的方法完全不同的措施, 以便获得大幅度地提高升力和延缓失速的良好气动特性。  The technical problem to be solved by the present invention is that the invention is to find a new way to address the shortcomings in the search for increasing methods, and proposes a new measure that is completely different from the currently used methods in order to obtain a large Good aerodynamic characteristics to improve lift and retard stall.
本发明解决其技术问题所采用的技术方案是: 发明是采用一种篷翼, 采用 一种安装在机翼的上翼面的上方的称为篷翼的薄片式结构, 靠近而不接触上翼 面, 好像是一个篷子遮住机翼上表面。 由于篷翼和机翼上面之间形成一个气流 通道, 使远前方的来流绕流到上翼面的气流受到了制约, 使得流动较快的上翼 面上方的气流集中在篷翼之下的通道中。 与没有篷翼存在的流动情况相比, 流 经机翼上表面的气流的动能更大了, 于是使气流分流点大大往后方移动, 其结 果是一方面升力系数增大(包括线性段), 另一方面使失速迎角大大增加,从而 使最大升力系数增加, 实现了大幅度增升的目的。值得指出的是:采用篷翼后, 没有将原先的层流流动转化成紊流附面层,而是保持层流。同时篷翼厚度很小, 因此, 阻力增加不多, 升阻比保持在合理的范围内。 由于篷翼只是一片具有与 机翼上翼面相同或相似曲率的薄翼, 型阻很小, 但摩擦阻力有所增加, 这是唯 一的代价, 与大幅度的增加升力和失速迎角相比, 这点代价是值得的, 篷翼的 结构要求具有很大的刚度, 需要选用合适的重量轻, 刚度好的材料。 从结构设 计上, 可考虑将篷翼制造成具有加强肋的超薄翼型, 流线型。 好在篷翼的受力 是简支樑的受力型式,有利于结构设计和工艺制造。为了进一步增大失速迎角, 提出了另一种斜置式的篷翼结构。 该结构从空气动力学上看与上置式的单片篷 翼有所不同。 但它同样可以使气流分离点极大地往后移动, 其失速迎角的增加 量, 大大超过上置式篷翼的组合机翼的失速迎角增加量。 附图说明 The technical solution adopted by the present invention to solve its technical problems is: The invention adopts a canopy wing, which adopts a sheet structure called a canopy wing, which is installed above the upper wing surface of the wing, and approaches without touching the upper wing. Face, as if a awning covered the upper surface of the wing. Because an airflow channel is formed between the wing and the upper surface of the wing, the airflow from the far front to the upper wing surface is restricted, so that the airflow above the faster wing surface is concentrated under the wing In the channel. Compared with the flow situation where no wing exists, the kinetic energy of the airflow flowing through the upper surface of the wing is greater, so that the airflow divergence point is moved to the rear greatly. As a result, the lift coefficient is increased (including the linear segment). On the other hand, the stall angle of attack is greatly increased, so that the maximum lift coefficient is increased, and the purpose of a substantial increase is achieved. It is worth noting that after the use of the wing, the original laminar flow was not converted into a turbulent surface layer, but the laminar flow was maintained. At the same time, the thickness of the canopy wing is small, so the resistance does not increase much, and the lift-drag ratio remains within a reasonable range. Because the canopy is just a thin wing with the same or similar curvature to the upper wing surface, the type resistance is very small, but the frictional resistance is increased. This is the only price, compared with a substantial increase in lift and stall angle of attack. This cost is worthwhile. The structure of the canopy wing requires great rigidity, and it is necessary to choose a suitable lightweight and rigid material. From the structural design, it can be considered that the canopy wing is made into an ultra-thin airfoil with a reinforcing rib and a streamlined shape. Fortunately, the force of the wing It is a force type of simply supported beam, which is beneficial to structural design and process manufacturing. In order to further increase the stall angle of attack, another oblique wing structure is proposed. This structure is aerodynamically different from the top-mounted monolithic canopy. However, it can also make the air flow separation point move backward greatly, and the increase of the stall angle of attack greatly exceeds the increase of the stall angle of attack of the combined wing of the top wing. BRIEF DESCRIPTION OF THE DRAWINGS
下面通过附图进一步描述本发明的工作原理, 构造以及其增升效果。  The working principle, structure and increasing effect of the present invention will be further described below with reference to the drawings.
图 1是机翼上安装有本发明上置式篷翼的示意图。  FIG. 1 is a schematic diagram of an upper-mounted canopy wing installed on the wing.
图 2是机翼上安装有本发明斜置式篷翼的示意图。  Fig. 2 is a schematic diagram of an inclined canopy wing installed on the wing.
图 3是选用 NACA23012翼型为基本机翼和机身组合体的风洞试验曲线。 图 4是篷翼前缘可以向下偏转的另一种实施方案的示意图。  Figure 3 is a wind tunnel test curve using NACA23012 airfoil as the basic wing and fuselage combination. Fig. 4 is a schematic diagram of another embodiment in which the leading edge of the wing can be deflected downward.
图 5是安装篷翼后沿机翼剖面的气流流动状况的示意图。 图 6是本发明的第一种实施方案: 上置篷翼飞机。 图 7是本发明的另一种实施方案: 斜置篷翼飞机。  Fig. 5 is a schematic diagram of the air flow along the wing section after the canopy wing is installed. Fig. 6 is a first embodiment of the present invention: an upper canopy aircraft. Fig. 7 is another embodiment of the present invention: an inclined canopy aircraft.
图 8是本发明的篷翼与主机翼的相对位置的示意图。  FIG. 8 is a schematic diagram of the relative positions of the canopy wing and the main wing of the present invention.
具体实施方式 detailed description
由图 1可见: 篷翼 1位于机翼 2的上翼面 3之上方。 篷翼和机翼的前缘和 后缘沿翼展方面是相互平行的, 但沿翼弦方向上, 篷翼下表面到机翼上表面之 间的距离不一定相等。 是篷翼和机翼后缘的相对高度。 ¾是篷翼和机翼前缘 的相对高度。 当 Hr= 时, 篷翼 1和机翼的上表面 3是相互平行的。 当 ≠¾ 时, 篷翼相对于机翼有个安装角 Φ。 Φ角是篷翼前后缘的连线和机翼翼弦之间 的夹角。 Φ的改变(通常是正值)是通过改变 ¾ (固定 )来实现的。 ¾的大 小会影响这种装置的增升效果。 通过计算、 分析和风洞试验表明: 的值必须 仔细选择。 不能太小, 也不能太大。 太小了, 可能使篷翼与上翼面之前的气 流流动受阻, 增升效果不好。 太大了会使结构发生困难。 同时也会降低增升效 果。 必须通过实验进行优化, 以确定一个 ¾最佳值。 初步的风洞试验表明- 的最小值大约为 10%的机翼空气动力弦的长度。 增大 值, 从 10%弦长增 加到 20%弦长时, 增升效果明显改善。 应当指出的, 即缝隙宽度的最佳值不 是固定的, 从风洞试验获得的结果, 由于尺度效应及附面层厚度与飞行器的真 实尺度有关, 往往要偏大一些, 因此, 真飞机的最佳 要通过实验确定。 图 2 所示, 在机翼 2的上表面 3倾斜地安装了两片篷翼 5和 6。 每片篷翼的一头连 接到机翼的上表面上, 这种联接可以是铰链连接, 也可以是固定连接, 视具体 情况而定。当采用铰链联接时,要考虑到上翼面 3的曲率,铰链 9和 10应保证 斜置篷翼 5和 6能顺利地张开和收起。 图 2中所示的斜置篷翼 5和 6的一端连 接在机翼 2的上翼面上, 另一端离开上翼面有一定的距离。 这个距离决定了斜 置篷翼与机翼之间的上反角 Φ。 Φ的大小也必须优化选择,太大太小都不合适。 本发明的一种实施例曾选取上反角 Φ=10°和 20°两种情况进行了风洞试验, 结 果发现取 20°比取 10°为好。使用斜置式篷翼时,如果用于低速飞机,可以采用 固定不收放的形式。 即在飞行的全过程中都张开篷翼。 这种方式使结构大为简 化。用在超音速飞机上时,应设计成可收放的斜置篷翼。当不须要使用篷翼时, 应利用液压机构或其他传动装置使篷翼 5和 6收起, 置于机翼中的方形凹槽 7 和 8内, 与机翼的上翼面完全贴合, 保持完整的单一的翼剖面。 As can be seen from FIG. 1: The canopy wing 1 is located above the upper wing surface 3 of the wing 2. The leading and trailing edges of the wing and the wing are parallel to each other along the wingspan, but along the chord direction, the distance between the lower surface of the wing and the upper surface of the wing is not necessarily equal. Is the relative height of the trailing edge of the wing and wing. ¾ is the relative height of the leading edge of the wing and the wing. When H r =, the wing 1 and the upper surface 3 of the wing are parallel to each other. When ≠ ¾, the wing has a mounting angle Φ relative to the wing. The angle Φ is the angle between the line connecting the leading and trailing edges of the wing and the wing chord. The change in Φ (usually a positive value) is achieved by changing ¾ (fixed). The size of ¾ will affect the effect of increasing this device. Calculations, analysis and wind tunnel tests have shown that: The value must be carefully selected. It cannot be too small or too large. Too small, it may hinder the flow of air flow between the wing and the upper airfoil, and the lifting effect is not good. Too big will make the structure difficult. It will also reduce the efficiency fruit. It must be optimized experimentally to determine an optimal value. Preliminary wind tunnel tests have shown that the minimum value is approximately 10% of the wing aerodynamic chord length. Increasing the value, when the chord length is increased from 10% to 20%, the increase effect is obviously improved. It should be noted that the optimal value of the gap width is not fixed. The results obtained from wind tunnel tests are often larger because the scale effect and the thickness of the surface layer are related to the true dimensions of the aircraft. Better to be determined experimentally. As shown in FIG. 2, two pieces of canopy wings 5 and 6 are installed obliquely on the upper surface 3 of the wing 2. One end of each wing is connected to the upper surface of the wing. This connection can be a hinged connection or a fixed connection, depending on the situation. When the hinge connection is adopted, the curvature of the upper airfoil 3 must be taken into consideration, and the hinges 9 and 10 should ensure that the inclined wing 5 and 6 can be smoothly opened and retracted. One end of the inclined canopy wings 5 and 6 shown in FIG. 2 is connected to the upper wing surface of the wing 2, and the other end is separated from the upper wing surface by a certain distance. This distance determines the upper anti-angle Φ between the inclined wing and the wing. The size of Φ must also be optimized, too large and too small are not suitable. According to an embodiment of the present invention, wind tunnel tests have been performed in two cases: the upper inclination angle Φ = 10 ° and 20 °, and it is found that 20 ° is better than 10 °. When using the inclined wing, if it is used for low-speed aircraft, it can be fixed and not retracted. That is, the wing is opened during the entire flight. This approach greatly simplifies the structure. When used in supersonic aircraft, it should be designed as a retractable inclined wing. When it is not necessary to use the wing, the wing 5 and 6 should be retracted by using a hydraulic mechanism or other transmission device, and placed in the square grooves 7 and 8 in the wing, which fully fits the upper wing surface of the wing. Maintain a complete single wing profile.
图 3是为了对比篷翼的增升效果而进行的风洞试验的结果。 主要显示了三 种情况的升力和失速迎角的变化情况。 采用的风洞试验模型是以 NACA23012翼 型为基础翼型, 安装在圆柱形的机身上, 机身头部为一椭圆形。 给出的结果是 "翼一身"组合体的气动特性。 由图 3可见, 曲线 12是基础结构 15的升力系 数随迎角变化情况, 失速迎角约为 12°,最大升力系数约为 0. 94。 曲线 13是安 装上置式篷翼后的 "翼一身"组合体 16的升力特性曲线。 失速迎角约为 20°。 最大升力系数约为 1. 6。 曲线 14是安装斜置式篷翼后的 "翼一身"组合体 17 的升力特性曲线。 失速迎角达 30度以上(因条件限制, 未进行大于 30°迎角的 试验。)最大升力系数约为 1. 4左右。有趣的现象是在这种斜置篷翼形式下,在 小于失速迎角的线性段范围内, 加装斜置篷翼后升力特性基本上不变, 上述实 验结果是限于在 1/2-2/3的翼展长度上装设篷翼的。(注:阻力和俯迎力矩特性 也不变。 图上未画出) 与现有的增升技术比较, 本发明的增加最大升力系数和 失速迎角的效果大大领先。 图 4给出了上置篷翼的另一种形式: 篷翼的前缘部 分 18可以向下偏折。 曾在风洞试验中测试了该种形式的增升效果, 发现 18向 下偏折会使失速迎角增大到 25°, 但最大升力系数略有降低。 图 4还表示了篷 翼薄片的后缘部分 23也可向下偏折。 图 5表示了篷翼的二维气流的流动图画, 篷翼 1置于翼剖面 11上翼面的上方。来流 V 巟过篷翼和基础篷翼的组合体时, 划分开三个流场: 1 区是位于基础翼型下翼面的下方, 其流动情况跟未装篷翼 时基本相同。 由于下翼面曲率较小, 平坦, 空气流动速度较慢, 压力较大。 3 区介于基础翼型的上表面和篷翼的下表面之间, 形成一个涵道, 空气流入这个 区域得到进一步的加速, 被加速后的气流不能穿越篷翼流到外面, 因此保持了 较大的动能, 使气流分离延缓许多。 由于流速大, 2区压力比 1区小。 2区处在 篷翼上表面的上方通往自由流场。由于篷翼的曲率变化基本上与基本翼型一致, 但比下翼面大, 气流得到加速, 压力比较低, 由于篷翼处在两个低压区 2和 3 之间, 其受力情况取决于这两个区的压力差。 我们期望 3区的流动速度越快越 好, 压力变小。 在气流经过篷翼绕到 2区时也被加速, 可能比 3区流速更快, 压力也很小, 可以推测, 3区和 2区的压力差相对于 1区和 3 区是要小得多, 因此, 篷翼的直接受力不会太大。 这有利于结构设计, 所增加的升力, 实际上 大部分是作用在基础机翼上的。 图 6是上置篷翼的一种实施方案。篷翼 1和 13 置于左右机翼 2和 14的上翼面的上方。 19是将篷翼推出和收起的传动装置的 前支杆, 可以有几个。 推出时应保持所有前支杆的伸出高度相同。 前支杆伸出 上翼面的高度是可调整的。 20与 19类似, 是后支杆。 篷翼相对于机翼的安装 角度可通过调整前支杆 19的伸出高度来实现。可通过液压机构或其他方式。 12 是任何一种飞机, 也可以是其他在大气中或水中的运输机械。 图 7是斜置式篷 翼的一种实施方案。篷翼 5, 6, 15和 16斜置于机翼上表面, 呈某个上反角度。 篷翼可以收起和张幵, 斜置篷翼的张开与收起是通过一种公知的传动机构, 将 作动筒支杆 21推出或缩回来实现的,还可以利用目前飞机上普遍采用的推出扰 流片的液压作动机构的方式来实现斜置式篷翼的收放。 收放时将篷翼收藏到机 翼表面的方形凹槽 7, 8, 17和 22之内, 使之和机翼上表面完全贴合, 保持原 先的基础翼型外形。 FIG. 3 is a result of a wind tunnel test performed to compare the raising effect of the wing. It mainly shows the change of lift and stall angle of attack in three cases. The wind tunnel test model used is based on the NACA23012 airfoil, mounted on a cylindrical fuselage, and the fuselage head has an oval shape. The result given is the aerodynamic characteristics of a "wing-in-body" assembly. As can be seen from Figure 3, curve 12 is the change in the lift coefficient of the base structure 15 with the angle of attack, the stall angle of attack is about 12 °, and the maximum lift coefficient is about 0.94. Curve 13 is the lift characteristic curve of the "wing-one" combined body 16 after the upper-type canopy is installed. The stall angle of attack is approximately 20 °. The maximum lift coefficient is approximately 1.6. Curve 14 is the lift characteristic curve of the "wing-in-body" combination 17 after the inclined wing is installed. 4。 Stall angle of attack of 30 degrees or more (due to conditions, no test greater than 30 ° angle of attack.) The maximum lift coefficient is about 1.4. The interesting phenomenon is that in this form of inclined canopy wing, the lift characteristics are basically unchanged after installing the inclined canopy in a linear range smaller than the stall angle of attack. The above experimental results are limited to 1 / 2-2 Canopy wings on / 3 wingspan. (Note: Resistance and thrust moment characteristics Also unchanged. (Not shown in the figure) Compared with the existing lifting technology, the effect of increasing the maximum lift coefficient and the stall angle of attack of the present invention is greatly ahead. FIG. 4 shows another form of the upper wing: The front edge portion 18 of the wing can be deflected downward. This type of increase effect was tested in a wind tunnel test, and it was found that a downward deflection of 18 would increase the stall angle of attack to 25 °, but the maximum lift coefficient was slightly reduced. Figure 4 also shows that the trailing edge portion 23 of the wing flap can also be deflected downward. FIG. 5 shows a two-dimensional flow picture of the airfoil, with the airfoil 1 placed above the airfoil surface of the airfoil section 11. When the incoming flow V passes through the combination of the wing and the base wing, three flow fields are divided: Zone 1 is located below the lower airfoil of the basic airfoil, and its flow is basically the same as when the wing is not installed. Because the lower airfoil has less curvature and is flat, the air velocity is slower and the pressure is greater. Zone 3 is located between the upper surface of the base airfoil and the lower surface of the wing, forming a duct. Air flows into this area to be further accelerated. The accelerated airflow cannot pass through the wing to the outside, thus maintaining a relatively The large kinetic energy delays the separation of the airflow. Due to the high flow velocity, the pressure in zone 2 is lower than in zone 1. Zone 2 leads to the free flow field above the upper surface of the wing. Because the curvature of the wing is basically the same as the basic airfoil, but larger than the lower wing surface, the airflow is accelerated, and the pressure is relatively low. Because the wing is located between the two low-pressure zones 2 and 3, its force depends on The pressure difference between these two zones. We expect that the faster the flow speed in zone 3, the better and the pressure will become smaller. The airflow is also accelerated when it passes around the wing to Zone 2. It may be faster than Zone 3 and the pressure is very small. It can be inferred that the pressure difference between Zone 3 and Zone 2 is much smaller than Zone 1 and Zone 3. Therefore, the direct force of the wing will not be too great. This is good for structural design, and most of the increased lift actually acts on the base wing. Figure 6 is an embodiment of the upper canopy wing. The canopy wings 1 and 13 are placed above the upper wing surfaces of the left and right wings 2 and 14. 19 is the front support rod of the transmission device that pushes and retracts the wing. There can be several. Keep all front poles at the same height when pushing out. The height of the front support rod protruding from the upper airfoil is adjustable. 20 is similar to 19, it is the rear support. The installation angle of the canopy wing with respect to the wing can be achieved by adjusting the protruding height of the front support rod 19. Can be through the hydraulic mechanism or other means. 12 is any kind of aircraft, but also other transportation machinery in the atmosphere or water. Fig. 7 is an embodiment of the inclined wing. The canopy wings 5, 6, 15 and 16 are placed obliquely on the upper surface of the wing at an upside-down angle. The canopy wing can be stowed and stretched. The tilting canopy can be opened and retracted through a known transmission mechanism to push out or retract the actuator cylinder rod 21. It can also be used in current aircraft. The way of launching the hydraulic actuating mechanism of the spoiler is to realize the retracting of the inclined wing. When retracting, store the wing in the square grooves 7, 8, 17, and 22 on the surface of the wing, so that it fits perfectly with the upper surface of the wing, keeping the original First base airfoil profile.
关于篷翼的几何形状和篷翼与主机翼的相对位置, 不限于上述说明所列举 的实施力中表示的情况。 为了取得最佳的气动效果, 或为了保证篷翼有必要的 强度和刚度, 或为了减轻重量, 或由于受到主机翼面上操纵面上下偏转产生的 限制, 在实际应用中, 会出现如下情况:. 从某个剖面翼型上看, 篷翼的前缘起 点可以位于主机翼气动弦前缘稍后某个位置; 篷翼的后缘(终止点)位于主机 翼气动弦后缘前面某个位置。 如图 8所示。 其中, 23为机翼上的付翼。 此外, 沿主机翼翼展方向,较大型飞机的篷翼可分成相互接邻的几个较短的片段组成。 这些片段篷翼, 通过电气、 液压或机械机构之间的电气或机械连接, 协调同步 操纵收放, 以代替整片篷翼的作用。 这种多元结构形式可应用于平行篷翼和斜 置式篷翼。 篷翼不限于主机翼上应用, 也可应用于正常式或鸭式水平安定面或 全动操纵面。  The geometry of the wing and the relative position of the wing and the main wing are not limited to those shown in the implementation forces listed in the above description. In order to obtain the best aerodynamic effect, or to ensure the necessary strength and rigidity of the wing, or to reduce the weight, or due to the limitation caused by the deflection on the control surface of the main wing surface, in actual applications, the following situations will occur: From the perspective of a certain profile airfoil, the starting point of the leading edge of the canopy wing can be located at a position later than the leading edge of the aerodynamic chord of the main wing; . As shown in Figure 8. Among them, 23 is a wing on the wing. In addition, along the wingspan of the main engine, the wing of the larger aircraft can be divided into several shorter segments adjacent to each other. These fragments of the wing are coordinated and synchronized to be operated and retracted through electrical or mechanical connections between electrical, hydraulic, or mechanical mechanisms to replace the entire wing. This multi-structure form can be applied to parallel wing and inclined wing. The wing is not limited to the application on the main wing, but can also be applied to the normal or duck-type horizontal stabilizer or full-motion control surface.
篷翼的应用不限于上述两种实施方案。 本发明可以包括许多种用途, 不限 于各种飞机, 可以是宇宙飞船重返地面的回收装置, 可以是地效飞行器, 也可 以是在水中或任何其他流体中运动的机械。 利用斜置式篷翼良好的大迎角特性 来设计抗尾旋装置, 将极大地增加飞机的安全性。  The application of the canopy is not limited to the two embodiments described above. The invention may include many uses, not limited to various aircraft, may be a recovery device for spacecraft returning to the ground, may be a ground effect aircraft, or may be a machine moving in water or any other fluid. Utilizing the good high angle of attack characteristics of the inclined wing to design the anti-rotation device will greatly increase the safety of the aircraft.

Claims

权 利 要 求 Rights request
1、 一种增加升力和失速迎角的篷翼, 包括机翼、 薄片式结构, 收放传动 机构, 其特征在于, 所述称为篷翼的薄片结构位于所述机翼上表面的上方, 所 述篷翼的曲率和所述机翼的上表面曲率相同或相似。 1. A canopy wing for increasing lift and stall angle of attack, comprising a wing, a laminar structure, and a retractable transmission mechanism, characterized in that the laminar structure called a canopy wing is located above the upper surface of the wing, The curvature of the wing and the curvature of the upper surface of the wing are the same or similar.
2、 根据权利要求 1所述的一种增加升力和失速迎角的篷翼, 其特征在于- 所述薄片结构置于机翼上表面的上方构成上置篷翼, 通过液压机构或任何其他 传动机械连接到所述机翼上。  2. A canopy wing that increases lift and stall angle of attack according to claim 1, characterized in that-the sheet structure is placed above the upper surface of the wing to form an upper awning wing, which is driven by a hydraulic mechanism or any other transmission Mechanically connected to the wing.
3、 根据权利要求 2所述的一种增加升力和失速迎角的篷翼, 其特征在于: 所述上置篷翼可绕后缘旋转。  3. The canopy wing for increasing lift and stall angle of attack according to claim 2, wherein the upper canopy wing can rotate around a trailing edge.
4、 根据权利要求 2或 3所述的一种增加升力和失速迎角的篷翼, 其特征 在于: 所述上置篷翼的后缘到机翼上表面的距离是固定不变的。  4. The canopy wing for increasing lift and stall angle of attack according to claim 2 or 3, characterized in that the distance from the rear edge of the upper canopy wing to the upper surface of the wing is fixed.
5、 根据权利要求 2或 3所述的一种增加升力和失速迎角的篷翼, 其特征 在于: 所述上置篷翼可以收回, 置于机翼上表面的方型凹槽中。  5. The canopy wing for increasing lift and stall angle of attack according to claim 2 or 3, characterized in that: the upper canopy wing can be retracted and placed in a square groove on the upper surface of the wing.
6、 根据权利要求 1或 2所述的一种增加升力和失速迎角的篷翼, 其特征 在于: 所述篷翼的前缘和后缘与机翼的前缘和后缘的位置相一致, 或者篷翼的 前缘和后缘顺序设置在机翼的前缘和后缘之间。  6. The canopy wing for increasing lift and stall angle of attack according to claim 1 or 2, characterized in that: the leading edge and the trailing edge of the wing are consistent with the positions of the leading edge and the trailing edge of the wing Or, the leading and trailing edges of the wing are sequentially arranged between the leading and trailing edges of the wing.
7、 根据权利要求 1或 2所述的一种增加升力和失速迎角的篷翼, 其特征 在于: 斜置式篷翼和机翼上表面之间有一个上反角, 并且斜置式篷翼可收回, 置于机翼上表面的方型凹槽中。  7. A canopy wing for increasing lift and stall angle of attack according to claim 1 or 2, characterized in that: an inclined angle between the inclined wing and the upper surface of the wing, and the inclined wing can Retract and place in a square groove on the upper surface of the wing.
8、 根据权利要求 1所述的一种增加升力和失速迎角的篷翼, 其特征在于 : 所述薄片结构呈一个安装角连结在所述机翼的上翼面上, 构成斜置式篷翼, 安 装角在飞行中固定不变或可以调节大小。 8, according to claim one of the claims 1 to increase the lift and stall angle of attack of the wing canopy, wherein: the upper wing surface of the sheet structure were connected to a mounting angle of the wing, the wing constituting the canted canopy The mounting angle is fixed during flight or can be adjusted.
9、 根据权利要求 1或 2或 8所述的一种增加升力和失速迎角的篷翼, 其 特征在于: 篷翼的前缘部分和后缘部分往下偏转。 9. A canopy wing for increasing lift and stall angle of attack according to claim 1 or 2 or 8, characterized in that: the leading edge portion and the trailing edge portion of the wing are deflected downward.
10、 根据权利要求 1或 2或 8所述的一种增加升力和失速迎角的篷翼, 其 特征在于:所述篷翼由几个片段组成,通过液压机构或其他传动机构相互连接, 协同动作。  10. The canopy wing for increasing lift and stall angle of attack according to claim 1 or 2 or 8, characterized in that the canopy wing is composed of several segments, which are connected to each other through a hydraulic mechanism or other transmission mechanism to cooperate action.
PCT/CN2003/001035 2003-01-17 2003-12-04 A Wing ASSEMBLY CAPABLE OF INCREASIGN THE LIFT AND THE ANGLE OF STALL WO2004092009A1 (en)

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CNB021338620A CN100513256C (en) 2003-01-17 2003-01-17 Sail wing for increasing lift force and stalling attack angle

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DE102009006212A1 (en) * 2009-01-27 2010-09-23 Fritz Unger Method for increasing lifting of e.g. aerofoil, for use in aerodynamically-flying aircraft, involves arranging body above another body in aerodynamic-flow, and moving aerofoil upwardly by parts during application of air flow
US8882470B2 (en) 2011-01-07 2014-11-11 Fritz Unger Rotor for a wind power generator

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* Cited by examiner, † Cited by third party
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US9016637B2 (en) * 2012-02-10 2015-04-28 The Boeing Company High-positioned 3-position variable camber krueger
CN113968341B (en) * 2021-12-08 2024-01-26 北京航空航天大学 Miniature unmanned aerial vehicle using bionic winglet
CN114506442A (en) * 2022-01-28 2022-05-17 中国商用飞机有限责任公司 Wing with turbulence auxiliary device and flight device comprising same

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GB2237254A (en) * 1989-10-25 1991-05-01 Richard Harry Barnard Secondary lifting surfaces using separated flow
CN2095830U (en) * 1991-04-22 1992-02-12 林永克 Air propeller
DE4140139A1 (en) * 1991-12-05 1993-06-09 Klaus Dipl.-Werkmeister 6600 Saarbruecken De Lellig Aircraft which can be converted from biplane to monoplane - has short take-off and landing capability but high cruising speed
CN2186706Y (en) * 1994-01-24 1995-01-04 南京理工大学 High lift eddy catching wing
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Publication number Priority date Publication date Assignee Title
GB2237254A (en) * 1989-10-25 1991-05-01 Richard Harry Barnard Secondary lifting surfaces using separated flow
CN2095830U (en) * 1991-04-22 1992-02-12 林永克 Air propeller
DE4140139A1 (en) * 1991-12-05 1993-06-09 Klaus Dipl.-Werkmeister 6600 Saarbruecken De Lellig Aircraft which can be converted from biplane to monoplane - has short take-off and landing capability but high cruising speed
CN2186706Y (en) * 1994-01-24 1995-01-04 南京理工大学 High lift eddy catching wing
US5772155A (en) * 1996-06-01 1998-06-30 Nowak; Dieter K. Aircraft wing flaps

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102009006212A1 (en) * 2009-01-27 2010-09-23 Fritz Unger Method for increasing lifting of e.g. aerofoil, for use in aerodynamically-flying aircraft, involves arranging body above another body in aerodynamic-flow, and moving aerofoil upwardly by parts during application of air flow
US8882470B2 (en) 2011-01-07 2014-11-11 Fritz Unger Rotor for a wind power generator

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AU2003289606A1 (en) 2004-11-04
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