CN1217767A - vertical axis vortex wind turbine - Google Patents
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- CN1217767A CN1217767A CN96196454A CN96196454A CN1217767A CN 1217767 A CN1217767 A CN 1217767A CN 96196454 A CN96196454 A CN 96196454A CN 96196454 A CN96196454 A CN 96196454A CN 1217767 A CN1217767 A CN 1217767A
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F03—MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03D—WIND MOTORS
- F03D3/00—Wind motors with rotation axis substantially perpendicular to the air flow entering the rotor
- F03D3/04—Wind motors with rotation axis substantially perpendicular to the air flow entering the rotor having stationary wind-guiding means, e.g. with shrouds or channels
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
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- F03D—WIND MOTORS
- F03D3/00—Wind motors with rotation axis substantially perpendicular to the air flow entering the rotor
- F03D3/04—Wind motors with rotation axis substantially perpendicular to the air flow entering the rotor having stationary wind-guiding means, e.g. with shrouds or channels
- F03D3/0436—Wind motors with rotation axis substantially perpendicular to the air flow entering the rotor having stationary wind-guiding means, e.g. with shrouds or channels for shielding one side of the rotor
- F03D3/0445—Wind motors with rotation axis substantially perpendicular to the air flow entering the rotor having stationary wind-guiding means, e.g. with shrouds or channels for shielding one side of the rotor the shield being fixed with respect to the wind motor
- F03D3/0454—Wind motors with rotation axis substantially perpendicular to the air flow entering the rotor having stationary wind-guiding means, e.g. with shrouds or channels for shielding one side of the rotor the shield being fixed with respect to the wind motor and only with concentrating action, i.e. only increasing the airflow speed into the rotor, e.g. divergent outlets
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Abstract
Description
本发明涉及在平行主流中例如独立权利要求前序部分所述的带有切向入流阀和至少一个出流孔的入流流型中的平行旋流和/或螺旋形旋流的高环量或高集中速度和/或高集中质量的涡流的一种产生和利用方法,以及涉及实施该方法的装置。The invention relates to high circulation or high circulation of parallel and/or helical swirls in a parallel main flow, such as an inflow pattern with a tangential inflow valve and at least one outflow hole, as described in the preamble of the independent claim A method for the generation and utilization of eddy currents of high concentrated velocity and/or high concentrated mass, and devices for implementing the method.
本发明的方法和装置可以提高平行流在转换成高环量或高集中速度和/或高集中质量的涡流时的效率,以及形成稳定的涡流和插入主流中。并保证了流经实施该方法的装置的自由入流通过主流。本发明的装置可用于各种流型中,其数量取决于尺寸和提供的空间。所设置的装置的尺寸和数量主要取决于制造的涡流的环量强度。本发明装置也可设置在层流的平行流中。这时产生的涡流在下游利用其能量,例如进一步制成诱导的涡流圈来把较深层的流体运送到表面上。The method and apparatus of the present invention can improve the efficiency of parallel flow conversion into high circulation or high concentrated velocity and/or high concentrated mass eddies, as well as the formation of stable eddies and insertion into the main flow. And a free inflow through the main flow through the device implementing the method is ensured. The device of the present invention can be used in various flow patterns, the number of which depends on the size and space provided. The size and number of devices provided depends primarily on the circulation strength of the eddy currents produced. The device according to the invention can also be arranged in a laminar parallel flow. The vortex generated at this time uses its energy downstream, for example, to further create induced vortex circles to transport deeper fluids to the surface.
在流体力学中,大家熟知的紊流与流体的层流的区别是,紊流具有到底层的涡流。工程上产生涡流,例如为了集中风能而在风流中产生涡流圈,这已在专利文献DE-PS3330899叙述。在这里将翼型构件布置成星形,以使旋涡在一个内圆上撕断,并被风流带走。在下游引起的涡流圈在一个较小的圆内加速流速,已证明可达到两倍。与未加速的流体比较,这种集中速度的流体具有较大的功率。缺点是,集中的装置比相同额定功率的空运转的涡轮机具有大得多的投影入流面。如在所有机翼时一样,升力的特性曲线和涡流形成的特性曲线取决于迎角和入流速度。由此而引起调节和控制费用。不能防止声音传播。In fluid mechanics, the difference between the well-known turbulent flow and the laminar flow of a fluid is that the turbulent flow has eddies to the bottom layer. The generation of vortices in engineering, such as the generation of vortex circles in the wind flow in order to concentrate wind energy, has been described in the patent document DE-PS3330899. Here, the airfoil elements are arranged in a star shape, so that the vortices are torn off on an inner circle and carried away by the wind current. The swirl circle induced downstream accelerates the flow velocity in a smaller circle, and has been shown to double. This concentrated velocity fluid has greater power than an unaccelerated fluid. A disadvantage is that a centralized installation has a much larger projected inflow surface than a dry-running turbine of the same rated power. As with all airfoils, the characteristic curves for lift and vortex formation depend on the angle of attack and the inflow speed. Regulation and control costs arise from this. Does not prevent sound transmission.
在由于螺旋浆引起的功率消耗不断增加时,可看到涡流开裂,涡流开裂可导致功率减小,直至涡流圈破坏为止。在这方面只公开了一种较小的试验设备。When the power consumption due to the propeller is increasing, vortex cracking can be seen, which can lead to a reduction in power until the vortex ring is broken. Only a relatively small experimental device is disclosed in this respect.
专利文献PCT/DE92/00450公开了在各种流型中从平行流产生旋流的一种方法和装置。在内旋流中,涡流发生器设置在同心圆上,其中涡流发生器根据不同的入流产生涡线、制造边缘涡流或管状涡流。这种涡流通过平行旋流在流型中绕成涡流圈,这种涡流圈诱导出一个轴向的附加速度,从而在流型中引起轴流加强和圆周速度增加。其中绕流一个内空心体,在这个空心体中吸入轴流以及吸入诱导出的许多涡流。这样就可在势涡的作用区内设置一台涡轮机或将空心体直接作为涡轮机利用。这种装置的效率主要取决于产生涡流的构件的环量。Patent document PCT/DE92/00450 discloses a method and a device for generating swirl flow from parallel flow in various flow regimes. In the internal swirling flow, the vortex generators are arranged on concentric circles, wherein the vortex generators generate vortex lines, edge vortices or tubular vortices depending on the inflow. This vortex turns into a vortex circle in the flow pattern through the parallel swirl flow, and this vortex circle induces an axial additional velocity, thereby causing the axial flow to strengthen and the peripheral velocity to increase in the flow pattern. The flow flows around an inner hollow body in which the axial flow and many vortices induced by the suction are sucked in. In this way, a turbine can be arranged in the area of action of the potential vortex or the hollow body can be used directly as a turbine. The efficiency of such a device depends essentially on the circulation of the eddy current-generating components.
业已证明的缺点是,产生这种涡流的构件在流体力学上反应缓慢,所以需要较大的自由流程来产生稳定的诱发的涡流。此外,这种涡流的形成过程取决于迎流物体的形状和引入主流的引流处的压力情况。A proven disadvantage is that the hydrodynamically slow response of the components generating such vortices requires a relatively large free flow to generate a stable induced vortex. In addition, the formation process of this vortex depends on the shape of the oncoming object and the pressure situation at the drainage into the main flow.
为了提高涡流的环量,人们提出了设置带有多个入流孔的内部空心体,涡流发生器直接设置在空心体的圆周上,并作为涡轮机利用。这种方案达到的效果是,在由于涡轮机引起能量消耗时增加平行旋流的圆周速度并同时提高这种涡轮机的效率。此外,有人提出将这种涡轮机配制多个叶片以及翼型的隔壁来直接产生较大环量的涡流,而且也可在垂直轴转子中利用绕流机翼或机翼型叶片的升力的流体力学上的诸多优点。In order to increase the circulation of the vortex, it is proposed to arrange an inner hollow body with a plurality of inflow holes, and the vortex generator is directly arranged on the circumference of the hollow body and used as a turbine. This approach has the effect of increasing the peripheral speed of the parallel swirling flows and at the same time increasing the efficiency of such a turbine when energy consumption is caused by the turbine. In addition, it has been proposed to equip this turbine with multiple blades and the partition wall of the airfoil to directly generate a large amount of vortex flow, and it is also possible to use the hydrodynamics of the lift around the airfoil or the airfoil blade in the vertical axis rotor many advantages.
这种涡轮机引起能量消耗时产生的平行旋流的圆周速度的增加作为驱动旋场而引起涡轮机效率的进一步提高。与利用纯阻力比较,通过利用升力增加了涡轮机的功率。产生涡流的构件的设置受到了涡轮机的结构空间的限制,因而功率增加受到结构工程方面的限制。Such a turbine causes an increase in the peripheral speed of the parallel swirls generated during energy consumption as a driving swirl field leading to a further increase in the efficiency of the turbine. The power of the turbine is increased by utilizing lift compared to utilizing pure drag. The arrangement of the vortex-generating components is limited by the installation space of the turbine, and thus the power increase is limited by structural engineering.
本发明的任务是提出一种方法和装置来产生高环量或高集中速度和/或高集中质量的能量可利用的涡流,以及保证在引入主流的过程中和引入主流以后以及在诱发的涡流圈中的能量的可利用性。The task of the present invention is to propose a method and a device to generate energy-available eddies of high circulation or high concentrated velocity and/or high concentrated mass, as well as to ensure that during and after the introduction of the main flow and after the induced eddies Availability of energy in the circle.
此外,本发明的任务还在于扩大这个方法的使用范围并提出一些装置,这些装置可设置在多种流型中和/或入流的平行流中来产生涡流及其能量利用,或可增大集中的入流面和提高旋转流体能量的集中程度。Furthermore, the object of the present invention is to extend the scope of use of this method and to propose devices which can be arranged in various flow patterns and/or in the parallel flow of the incoming flow to generate vortices and their energy utilization, or to increase the concentration The inflow surface and improve the concentration of rotating fluid energy.
根据本发明,这些任务是通过独立权利要求中所述的特征来实现的。These tasks are achieved according to the invention by the features stated in the independent claims.
根据本发明,在一种分层的平流中和/或在制造旋流的多种流型中,用一个或多个装置同时产生固定在一个旋转轴上具有流体动能的不同作用的各种涡流,并转换成一个新的涡流形状,其中,在高压作用下在一个带螺旋形入流孔的空心圆柱体的一个内圆上同心地产生一个接近旋转轴的集中速度并可调节的有势中心涡,以及同时在流体压力作用下在相同长度的一条外螺旋线上产生一个较大的包络涡,其中螺旋线的中心大于空心圆柱体的直径,并引起空心圆柱体的外侧绕流,有势中心涡以其速度场在内部和包络涡在外部以速度场的内半径同时在边界层上作用在空心圆柱体的一个例如截锥表面形状的固定或旋转的渗透流体或不渗透流体的覆盖面,在这个覆盖面上涡流的圆周速度增加,直至有势中心涡的中心流出为止,有势中心涡以及包络涡的圆周速度在流出半径上调节成包络涡推动有势中心涡,有势中心涡流入包络涡的低压中心,于是高压便转换成动能。包络涡为制造和保持有势中心涡创造了流体力学的存在条件,并防止集中速度的有势中心涡的开裂,这两种涡流形状汇合成一个在涡心具有明显高的环量和高集中速度的有势管状涡,在包络涡的涡流发生器中有一个出流孔,在流体压力作用下转向流出到待产生的主流中,以涡流稳定的形式插入主流中,并绕成一个诱发的涡流圈或能量可利用的别的形状。According to the invention, in a stratified advection flow and/or in various flow patterns producing swirl flow, one or more devices are used to simultaneously generate various vortices fixed on a rotating shaft with different effects of fluid kinetic energy , and transforms into a new vortex shape, in which, under the action of high pressure, concentrically on an inner circle of a hollow cylinder with a helical inlet orifice, an adjustable potential central vortex with concentrated velocity close to the axis of rotation , and at the same time, under the action of fluid pressure, a larger envelope vortex is generated on an outer helix of the same length, wherein the center of the helix is larger than the diameter of the hollow cylinder, and causes the outer flow around the hollow cylinder, which has the potential A central vortex with its velocity field on the inside and an enveloping vortex on the outside with the inner radius of the velocity field acting simultaneously on the boundary layer on a fixed or rotating permeable or impermeable fluid surface of a hollow cylinder, e.g. a truncated cone surface shape , the peripheral velocity of the vortex increases on this covering surface until the center of the potential central vortex flows out, the peripheral velocities of the potential central vortex and the envelope vortex are adjusted on the outflow radius so that the envelope vortex pushes the potential center vortex, and the potential center The vortex flows into the low pressure center of the enveloping vortex, whereupon the high pressure is converted into kinetic energy. The envelope vortex creates the conditions for the existence of hydrodynamics for the manufacture and maintenance of the potential central vortex, and prevents the cracking of the potential central vortex with concentrated velocity. The potential tubular vortex with concentrated velocity has an outlet hole in the vortex generator of the envelope vortex, which turns to flow out into the main flow to be generated under the action of fluid pressure, inserts into the main flow in the form of vortex stabilization, and winds into a Induced swirl circles or other shapes where energy is available.
根据本发明,实施方法的第一装置由一个设置在旋转轴上方侧向开孔的空心圆柱体构成,该圆柱体位于螺旋线的中心。空心圆柱体的入流孔垂直于迎流设置,其底面是封闭的。在空心圆柱体的另一端面上设置有一个带中心出流孔的覆盖面,该覆盖面例如可构成截锥形。该覆盖面可设置成渗透流体和可旋转的。According to the invention, the first means for carrying out the method consists of a hollow cylinder with a lateral opening above the axis of rotation, which cylinder is located in the center of the helix. The inflow hole of the hollow cylinder is arranged vertically to the incoming flow, and its bottom surface is closed. On the other end of the hollow cylinder there is a cover surface with a central outlet opening, which cover surface can be formed, for example, in the shape of a truncated cone. The cover can be configured to be fluid permeable and rotatable.
这个空心圆柱体被一个具有相等的封闭底面的螺旋线构成的包络涡流发生器构件的圆周面这样包围住,即可进行空心圆柱体的绕流。在空心圆柱体的螺旋形或作成简单圆弧的入流孔范围内,这个圆周面是这样开孔的,即入流孔的自由入流可通过主流并由空心圆柱体绕流合成的体积流量集中在入流孔的较小的半径上。This hollow cylinder is surrounded by the circumferential surface of an enveloping vortex generator component formed by a helix with equal closed bases in such a way that a flow around the hollow cylinder takes place. In the area of the helical or simple arc-shaped inflow hole of the hollow cylinder, this peripheral surface is perforated in such a way that the free inflow of the inflow hole can pass through the main flow and the volume flow resulting from the flow around the hollow cylinder is concentrated in the inflow on the smaller radius of the hole.
在空心圆柱体覆盖面的范围内,包络旋涡发生器的圆周表面构成管状涡流所需的螺旋线,所以在覆盖面上方可产生一个管状涡流,并把由空心圆柱体引起的明显的旋流传递到覆盖面上。为了制造稳定的涡流,包络旋涡发生器具有一个按流体力学确定的比空心圆柱体高的高度,这个高度至少相当于空心圆柱体的两倍高度。Within the coverage of the hollow cylinder, the circumferential surface of the envelope vortex generator constitutes the helix required for the tubular vortex, so a tubular vortex can be generated above the coverage, and the obvious swirl caused by the hollow cylinder is transferred to Coverage. In order to generate a stable vortex, the envelope vortex generator has a hydrodynamically determined height above the hollow cylinder, which corresponds to at least twice the height of the hollow cylinder.
当一个平行流、一个平行的旋流或一个螺旋形的旋流流入本发明的第一装置时,这种流体被分成三种不同作用的体积流量。在底面范围内直至空心圆柱体覆盖面下方通过空心圆柱体的入流孔的垂直入流产生高压,于是在空心圆柱体上产生一个小于入流速度的外圆周速度。同时在包络旋涡发生器中的空心柱体中产生外部螺旋形绕流,从而在下部范围围绕空心圆柱体构成一个同心圆的旋流。这种旋流由于比垂直的入流的圆周速度高而增加了流入空心圆柱体的体积流量。与垂直的入流相比,在空心圆柱体的外半径上产生圆周速度的较大起始值。When a parallel flow, a parallel swirl flow or a helical swirl flow flows into the first device of the invention, this flow is divided into three differently acting volume flows. The vertical inflow through the inflow openings of the hollow cylinder in the region of the base as far as below the hollow cylinder's covering generates a high pressure, so that an outer peripheral velocity on the hollow cylinder is lower than the inflow velocity. At the same time, an outer helical flow is generated in the hollow cylinder in the envelope vortex generator, so that a concentric swirl flow is formed around the hollow cylinder in the lower area. This swirling flow increases the volumetric flow into the hollow cylinder due to the higher peripheral velocity than the vertical inflow. At the outer radius of the hollow cylinder, a greater initial value of the peripheral velocity occurs compared to a vertical inflow.
在空心圆柱体上制造的外部旋流通过包络旋涡的螺旋形流动的流体保持在圆柱体覆盖面上方。圆周速度随半径减小而变大。An external vortex created on a hollow cylinder is maintained above the cylinder cover by the helically flowing fluid of the enveloping vortex. The peripheral speed becomes larger as the radius decreases.
通过离心力的作用,在旋转轴上方产生一个低压中心,这个低压中心通过旋转被固定在空心圆柱体的出流孔上并在这个出流孔中产生作用而在空心圆柱体的入流孔上引起一个抽吸作用。Through the action of centrifugal force, a center of low pressure is generated above the axis of rotation. This center of low pressure is fixed on the outlet hole of the hollow cylinder by rotation and acts in this outlet hole to cause a pressure on the inlet hole of the hollow cylinder. suction action.
同时在空心圆柱体的出流孔方向内在有势涡内产生一个环量而不需要外部入流的引入。环量可按旋转动量定律计算、从结构上进行调节并按亥姆霍兹涡流定理在涡管的横截面变化时保持不变,当这种横截面变化同时预先给出由于出流孔上方作用的低压力而引起的平移形式的方向变化时,出流孔就表示横截面变化。At the same time, a circulation is generated in the potential vortex in the direction of the outlet hole of the hollow cylinder without the introduction of an external inflow. The circulation can be calculated according to the law of rotational momentum, structurally adjusted and remains constant according to the Helmholtz vortex theorem when the cross-section of the vortex tube is changed, when this cross-section change is simultaneously given due to the action above the outlet hole When the direction change in the form of translation caused by low pressure, the outlet hole represents a change in cross section.
尽管向里的圆周速度不断增加和不断增加的离心力作用,还是发现有一个具有自然迁移机理的质量流量流入并通过一个势涡。Despite the increasing inward peripheral velocity and increasing centrifugal force, a mass flow with a natural migration mechanism was found to flow into and through a potential vortex.
速度场的流线的同心圆同时是质点的运动迹线,所以根据旋转动量守恒定律,同心圆表示标准势,标准势可通过圆周速度来区分。The concentric circles of the streamlines of the velocity field are also the motion traces of the particles, so according to the law of conservation of rotational momentum, the concentric circles represent the standard potential, which can be distinguished by the peripheral velocity.
如果质点在势涡的内部进行平移位置交换,则由于能量守恒定律的原因,缺少的质点必须被补充,同时由于相同的原因在速度场的同心圆上必须保持自然标准势。迁移机理可作为许多与势涡旋转方向相反的质点进行的螺旋形位置交换来描述。在这种位置交换中,质点由一个小的圆周速度加速到一个大的圆周速度。这种位置交换至少以动量速度进行,所以根据标准势的惯性矩,标准势保持不变,而且离心力对质量流量不起阻塞作用。实际上没有能量损失就实现了质量流,而且只与包络涡的低压大小有关。If the particles are exchanged in translation in the interior of the potential vortex, the missing particles must be replenished due to the law of conservation of energy, and the natural standard potential must be maintained on the concentric circles of the velocity field for the same reason. The migration mechanism can be described as the helical position exchange of many particles opposite to the rotation direction of the potential vortex. In this position exchange, the particle accelerates from a small peripheral velocity to a large peripheral velocity. This exchange of positions takes place at least with momentum velocity, so the standard potential remains constant according to the moment of inertia of the standard potential, and the centrifugal force does not block the mass flow. Mass flow is achieved virtually without energy loss and is only related to the magnitude of the low pressure of the enveloping vortex.
如所周知,旋涡中心根据它的发生器半径大小为0.65倍半径,这个半径由空心圆柱体的出流孔确定,所以根据本发明产生一个有势中心涡,其最高圆周速度位于出流孔的0.65倍半径上。As is well known, the center of the vortex is 0.65 times the radius according to its generator radius, which is determined by the outlet hole of the hollow cylinder, so according to the present invention a potential central vortex is produced with the highest peripheral velocity at the outlet hole 0.65 times the radius.
出流横截面和包络涡的有效低压中心确定有势中心涡移动到包络涡的低压中心的移动速度。The effective center of low pressure of the outflow cross-section and the envelope vortex determine the movement speed of the potential center vortex to the center of low pressure of the envelope vortex.
旋转和包络涡低压中心之间的分界层同时为有势中心涡制造了一个流体力学的壁,这个有势中心涡在流入时可支持在这个壁上。由于覆盖面上方的自由旋流,这里所谓的旋流可理解为入流压力,所以圆周速度也不会下降到空心圆柱体中建立高压时必须转变的速度值。The boundary layer between the rotating and low-pressure centers of the enveloping vortices simultaneously creates a hydrodynamic wall for the potential central vortex on which the potential central vortex rests upon inflow. Due to the free swirling flow above the covering surface, the so-called swirling flow here can be understood as the inflow pressure, so the peripheral speed will not drop to the speed value that must be converted when the high pressure is established in the hollow cylinder.
从中可得出这样的结论:包络涡的内圆周速度在到低压中心的分界层上比流入的有势中心涡的外圆周速度大。所以在高压作用下朝包络涡涌出的有势中心涡在其外圆周上被包络涡推动。From this it can be concluded that the inner peripheral velocity of the enveloping vortex is greater at the boundary layer to the low-pressure center than the outer peripheral velocity of the inflowing potential central vortex. Therefore, under the action of high pressure, the potential central vortex gushing toward the envelope vortex is pushed by the envelope vortex on its outer circumference.
在高压作用下空心圆柱体产生有势中心涡,该高压的势能不可能径向有效作用和引起有势中心涡的膨胀。The hollow cylinder produces a potential central vortex under high pressure, and the potential energy of the high pressure cannot effectively act radially and cause the expansion of the potential central vortex.
高压在分界层内的被推动的外圆周速度以及较小的内圆周速度之间只有一个自由作用方向。从而压力梯度在圆周速度方向内是一个合力,所以高压只可能转换成动能来加速有势中心涡。The high pressure has only one direction of free action between the driven outer peripheral speed and the lower inner peripheral speed in the boundary layer. Therefore, the pressure gradient is a resultant force in the direction of the peripheral velocity, so the high pressure can only be converted into kinetic energy to accelerate the potential central vortex.
这样就在包络涡发生器内合成一个高环量的、稳定的、结构可调节的和增大的涡流,这个涡流具有一个外螺旋形的入流。This results in a high-volume, stable, structurally adjustable and increasing vortex in the envelope vortex generator, which has an external helical inflow.
在流出到主流之前就对新的涡流形状制造了全部存在条件。这种涡流在流出到主流时已插入待产生的主流中而在涡流和主流之间没有压差。All conditions for the existence of the new vortex shape are created before flowing out into the main flow. Such a vortex, when flowing out into the main flow, is already inserted into the main flow to be generated without a pressure difference between the vortex and the main flow.
这种涡流的环量例如可完全用于要制造的涡流圈的诱导过程。The circulation of such swirl currents can be fully used, for example, for the induction process of the swirl coils to be produced.
根据本发明,可使涡流的环量和空间需要适合结构和能量的要求。According to the invention, the circulation volume and space requirements of the eddy current can be adapted to the structural and energy requirements.
本发明的方法产生的新的效果是,在一个准封闭空间中的高压力作用下与在入流压力作用下和在一个共同旋转轴上方的涡流层的螺旋形卷入下的发展过程统一成一个与时间有关的集中速度过程,从而在产生的新涡流形状稳定地引入要产生的主流的过程中提供能量来使内涡流加速。The novel effect produced by the method according to the invention is that the development processes under the action of high pressure in a quasi-closed space and under the action of the inflow pressure and the helical entrainment of the vortex layer above a common axis of rotation are unified into one The time-dependent concentrated velocity process provides energy to accelerate the inner vortex during the shape-stable introduction of the new vortex generated into the main flow to be generated.
这样就为产生涡流的构件创造了高度标准化的前题,从而有利于这种构件批量生产的经济性。本发明的第一装置可用于要产生能量集中的所有流体中,从而可大大改善经济性。This creates the preconditions for a high degree of standardization for the components generating the eddy currents, which facilitates the economical mass production of such components. The first device according to the invention can be used in all fluids in which energy concentrations are to be produced, thereby greatly improving the economy.
在该方法的一种改进方案中,在一个主流中任意地或在一个圆上、在垂直于主流固定的许多旋转轴上和在相应的一个旋转轴上通过螺旋形的入流在低压作用的出流孔、通流孔和底部边界层之间构成的涡流室产生许多相互沟通的势涡,在这些到出流孔具有最大距离的势涡中制造高集中的中心涡流,而在到出流孔距离不断变小的势涡中则由于涡流中心的形成而制造出涡流管,同时中心涡流和涡流管通过作用的低压力同轴地加速相互推动并产生分层的中心涡流,其中圆周速度通过流体半径调节,在出流孔之前有一个膨胀和稳定阶段,这个阶段可通过一个自然的旋涡尺寸来确定长度,在膨胀和稳定阶段分层中心涡流通过与出流半径和通流半径有关的高压力作用下以及通过中心涡流的内部驱动转变成具有合成圆周速度的涡流,并且集中速度和/或集中质量地稳定地导入主流中。In a refinement of the method, in a main flow at random or on a circle, on a number of axes of rotation fixed perpendicular to the main flow and on a corresponding one of the axes of rotation by means of a helical inflow at the outlet of the low-pressure effect The vortex chamber formed between the flow hole, the flow hole and the bottom boundary layer produces many potential vortices communicating with each other, and a highly concentrated central vortex is created in these potential vortices with the largest distance to the flow hole, while in the flow hole to the flow hole In the potential vortex whose distance is getting smaller, the vortex tube is created due to the formation of the vortex center. At the same time, the central vortex and the vortex tube accelerate each other coaxially through the acting low pressure and generate a stratified central vortex, in which the peripheral velocity passes through the fluid. Radius regulation, there is an expansion and stabilization phase before the outlet orifice, this phase can be determined by a natural vortex size to determine the length, in the expansion and stabilization phase, the stratified central vortex passes the high pressure related to the outlet radius and the flow radius Under the action and by the internal drive of the central vortex, it is converted into a vortex with a resultant peripheral velocity, and the concentrated velocity and/or the concentrated mass are stably introduced into the main flow.
根据本发明,在一个圆上,在一个或多个与主流保持垂直的旋转轴上方,由于溢出的主流而在一定的面和/或装置上产生低压力,通过这种低压力使轴流导入主流中,同时从主流的螺旋形流入涡流室中的入流在过压力作用下制造有势涡,该有势涡的旋转轴与垂直于主流的旋转轴一致。在有势涡中通过半径变小来实现圆周速度的增加,并朝与旋涡有关的例如喷嘴形的设置在垂直旋转轴上方的一系列涡流室的出孔方向制造集中速度和/或集中质量,在其上作用主流的低压力,而且集中质量同轴地在旋转轴上方平移。沿垂直旋转轴在各个势涡中产生在其旋转轴上的不同的集中速度,可达到的最大集中速度和集中质量在离主流的低压面最远的势涡中。根据在垂直的旋转轴上设置的势涡的数量这样减少制造在主流的低压作用方向内的集中速度,即由各个势涡的出流口流出的中心流的外圆周速度与在主流低压面方面内随后流过的势涡在垂直轴上方的涡流中心速度接近一致。然后朝主流方向这样合成的分层涡流中心流体在主流的低压力的面积下方范围内经过一个与时间有关的膨胀阶段,在这个阶段中由于高压力使集中质量在这个分层的中心流体中保持稳定,这样就把直径与长度的比例大致小于和等于1∶6的自然涡转变成高集中速度和高集中质量以及高环量的形状稳定的涡流。According to the invention, on a circle, above one or more axes of rotation kept perpendicular to the main flow, a low pressure is generated on certain faces and/or devices due to the overflowing main flow, by means of which low pressure the axial flow is introduced into the In the main flow, the inflow from the main flow spirally into the vortex chamber at the same time creates a potential vortex under the action of overpressure, and the rotation axis of the potential vortex is consistent with the rotation axis perpendicular to the main flow. In the potential vortex, the peripheral velocity is increased by decreasing the radius and producing a concentrated velocity and/or a concentrated mass towards the outlet of the vortex-related, e.g. nozzle-shaped, series of vortex chambers arranged above the vertical axis of rotation, The low pressure of the main flow acts on it, and the concentrated mass translates coaxially over the axis of rotation. Different concentrated velocities on its axis of rotation are produced in each potential vortex along the vertical axis of rotation, the maximum achievable concentrated velocity and concentrated mass being in the potential vortex farthest from the low pressure side of the main flow. According to the number of potential vortices arranged on the vertical axis of rotation, the concentrated velocity produced in the low-pressure action direction of the main flow is reduced in this way, that is, the outer peripheral velocity of the central flow flowing out from the outlet of each potential vortex is the same as that in the low-pressure surface of the main flow The velocity of the vortex center above the vertical axis of the potential vortex flowing through in the inner space is close to the same. The stratified vortex center fluid thus synthesized in the direction of the main flow then undergoes a time-dependent expansion phase in the region below the low-pressure area of the main flow, during which the concentrated mass remains in this stratified center fluid due to the high pressure. Stable, so that the natural vortex with a ratio of diameter to length approximately less than or equal to 1:6 is transformed into a shape-stable vortex with high concentrated velocity, high concentrated mass and high circulation volume.
根据本发明,可显著扩大产生涡流的装置的可集中的入流面,其中通过制造的分层的和稳定的涡流中心流体创造新的流动形状并集中能量加以利用。这样就导致集中过程的效率增加和部分大的质量流量通过主流的较小旋转模截面。根据本发明,借助于平行流中的涡流通过自身诱导构成诱导的涡流圈,从而相对于主流产生部分的高的诱导的附加速度,这种附加的速度可用于集中的质量传输来产生可利用的能量。在旋流中插入的涡流可绕成涡流圈,从而产生轴向诱导的附加速度,这种附加的速度通过本发明作用的一个垂直轴转子加速被驱动的旋流。According to the invention, the concentrable inflow area of the vortex-generating device can be considerably enlarged, wherein new flow shapes are created by the produced stratified and stable vortex center fluid and energy is concentrated for utilization. This results in an increased efficiency of the concentrating process and a smaller rotating die cross-section for part of the larger mass flow through the main flow. According to the invention, by virtue of the eddy currents in the parallel flow forming induced swirl circles by their own induction, a high induced additional velocity of the part is generated relative to the main flow, which can be used for concentrated mass transport to generate available energy. The vortices inserted in the swirl flow can be wound into vortex coils, thereby producing axially induced additional velocity which accelerates the driven swirl flow through a vertical axis rotor with which the present invention operates.
实施本发明方法的第二装置由一个设置在旋转轴上方的侧向呈螺旋形开口的空心圆柱体构成。该空心圆柱体的入流孔垂直于入流设置,其底面是封闭的。在空心圆柱体另一端面上设置了一个具有一个与基圆同心的出流孔的遮盖面,该遮盖面例如在基圆内可作成截锥。在与入流垂直的空心圆柱体竖立的旋转轴整个长度上设置了在空心圆柱体的基圆上带中心通流孔的其他圆锥形隔壁,从而构成涡流室。这些涡流室的中心通流孔是这样确定的,即空心圆柱体的遮盖面的截锥的出流孔具有最大的半径,而设置在空心圆柱体内部的全部通流孔的半径则分别小一定的值,此值由在涡流室中产生涡流的流体力学条件得出。半径减小大约可为0.65r,其中r表示出流孔方向内的较大半径。The second device for carrying out the method according to the invention consists of a hollow cylinder with lateral helical openings arranged above the axis of rotation. The inflow hole of the hollow cylinder is arranged perpendicular to the inflow, and its bottom surface is closed. On the other end face of the hollow cylinder there is provided a cover surface with an outlet opening concentric to the base circle, which cover surface can be formed, for example, as a truncated cone in the base circle. A further conical partition wall with a central flow hole on the base circle of the hollow cylinder is provided over the entire length of the axis of rotation of the hollow cylinder perpendicular to the inflow, thereby forming a vortex chamber. The central flow openings of these vortex chambers are defined in such a way that the outlet holes of the truncated cone of the cover surface of the hollow cylinder have the largest radius, while the radii of all the flow holes arranged inside the hollow cylinder are each smaller by a certain amount. The value of , which is derived from the hydrodynamic conditions that create the vortex in the vortex chamber. The radius reduction may be approximately 0.65r, where r indicates the larger radius in the direction of the orifice.
当一个平行流、一个平行旋流或一个螺旋形旋流流经本发明第二装置时,个作为整体流入的体积流量被分成不同作用的体积流量。在底面范围内直至空心圆柱体覆盖面下方,在空心圆柱体入流横截面上方的垂直入流产生高压力。在最小通流半径的涡流室中高压力作用最大。涡流室中的高压力随通流面的增大而下降。在垂直旋转轴上方产生一个过压差,随着高压力减小,在涡流室和膨胀室的外半径上产生圆周速度的较大起始值。When a parallel flow, a parallel swirl flow or a helical swirl flow flows through the second device according to the invention, the volume flow flowing in as a whole is divided into different acting volume flows. The vertical inflow above the inflow cross-section of the hollow cylinder generates a high pressure in the region of the base as far as below the hollow cylinder coverage. The effect of high pressure is greatest in the vortex chamber with the smallest flow radius. The high pressure in the vortex chamber decreases as the flow area increases. An overpressure difference is created above the vertical axis of rotation, with a decrease in high pressure, resulting in a larger initial value of the peripheral speed on the outer radius of the vortex chamber and expansion chamber.
同时在空心圆柱体的涡流室中,沿出流孔方向产生势涡的环量。这个环量可按旋转动量定律计算并在涡管的横截面变化时保持不变。当这种横截面变化同时预先给出由于出流孔上方作用的低压力而引起的平移形式的方向变化时,则出流孔和通流孔就表示横截面变化。出流孔和通流孔的直径具有对确定集中速度的特征,下方设置的涡流室直径的喷嘴形的减小则对集中质量过程至关重要。喷嘴锥体的开角是可以选择的,这样有势的高压力转换成动能便可对要流出的中心涡流的外圆周速度加速。质量流量可通过一个带有自然迁移机理的势涡。从理论上讲,速度场的流线同心圆按势涡理论同时就是无质量流通过的质点的迹线。在实际的势涡中,流线和迹线的同心圆按旋转动量守恒定律形成管形的标准势,这种标准势可通过圆周速度来区分。这种标准势必须保持不变。与电工学中描述的半导体模型相似,这种势在流体中也可作为空间电荷状态来表示。带有能量的质量可在正的无质量的空间中排列成负的空间电荷状态。这样就可在涡流中看出质量迁移的实际机理。在势涡内部进行质点位置交换时,由于能量守恒定律的原因,缺少的质点必须予以补充,同时由于相同的原因,在速度场同心圆上的自然标准势必须保持不变。迁移机理可作为许多与势涡旋转方向相反的质点进行的螺旋形位置交换来描述。在这种位置交换中,质点由一个较小的圆周速度在利用重力的情况下加速到一个较大圆周速度的势能作用。位置交换至少以动量速度进行,所以根据标准势的惯性矩,标准势保持不变,而且离心力对质量流量没有阻塞作用。实际上没有能量损失实现了质量流,而且只由出流孔上方的低压力来确定。At the same time, in the vortex chamber of the hollow cylinder, the circulation of the potential vortex is generated along the direction of the outlet hole. This circulation can be calculated according to the law of rotational momentum and remains constant when the cross-section of the scroll tube is changed. The outlet openings and throughflow openings represent a cross-sectional change if this cross-sectional change simultaneously prescribes a change in direction in translation due to the low pressure acting above the outlet opening. The diameters of the outflow openings and through-flow openings are characteristic for determining the concentration velocity, while the nozzle-shaped reduction in the diameter of the vortex chamber arranged below is crucial for the concentration mass process. The opening angle of the nozzle cone is selectable so that the potentially high pressure converted into kinetic energy accelerates the outer peripheral velocity of the outgoing central vortex. Mass flow can be through a potential vortex with a natural transport mechanism. Theoretically speaking, according to the potential vortex theory, the streamline concentric circles of the velocity field are also the traces of the mass point through which the massless flow passes. In the actual potential vortex, the concentric circles of streamlines and tracklines form a tube-shaped standard potential according to the law of conservation of rotational momentum, and this standard potential can be distinguished by the peripheral velocity. This standard potential must remain constant. Similar to the semiconductor model described in electrotechnology, this potential can also be represented as a space charge state in fluids. Energetic masses can be arranged in negative space charge states in positive massless space. This allows the actual mechanism of mass transfer to be seen in the eddy currents. When exchanging particle positions inside the potential vortex, due to the law of energy conservation, the missing particles must be replenished, and for the same reason, the natural standard potential on the concentric circles of the velocity field must remain unchanged. The migration mechanism can be described as the helical position exchange of many particles opposite to the rotation direction of the potential vortex. In this exchange of positions, the particle is accelerated from a smaller peripheral velocity to a higher peripheral velocity under the action of potential energy by gravity. The exchange of positions takes place at least with momentum velocity, so the standard potential remains constant according to the moment of inertia of the standard potential, and the centrifugal force has no blocking effect on the mass flow. Mass flow is achieved with practically no energy loss and is only determined by the low pressure above the orifice.
具有最高圆周速度的涡流中心根据它的发生器半径大小构成0.65倍半径,这个半径由空心圆柱体的出流孔来确定。根据本发明产生一个中心涡流,它的最小的外圆周速度位于空心圆柱体出流孔的半径上,而它的最大圆周速度则位于涡流室的出流孔的0.65r上,这个最大的圆周速度离空心圆柱体的出流孔最远。通过在空心圆柱体出流孔下方的涡流室内的膨胀阶段,分层的涡流中心流体被稳定成一个具有合成圆周速度场的涡流,这个出流孔通过出流孔的直径与涡流室的高度的比例例如大约小于和等于1∶6来表征。出流横截面、空心圆柱体的高压力和作用的低压力确定着中心涡流的转移速度。因此,在空心圆柱体中产生分层中心涡流的高压力的势能不可能是径向作用的,而是通过空心圆柱体的出流孔下方的喷嘴形状转换成动能,这种动能引起稳定的涡流的外圆周速度的加速。The vortex center with the highest peripheral velocity forms a radius of 0.65 times its generator radius, which is determined by the outlet opening of the hollow cylinder. Produce a central vortex according to the present invention, its minimum outer peripheral velocity is positioned on the radius of hollow cylinder outlet hole, and its maximum peripheral velocity then is positioned on the 0.65r of the outlet hole of swirl chamber, and this maximum peripheral velocity furthest from the outlet hole of the hollow cylinder. Through the expansion stage in the vortex chamber below the outlet hole of the hollow cylinder, the stratified vortex center fluid is stabilized into a vortex with a synthetic peripheral velocity field, which is achieved by the diameter of the outlet hole and the height of the vortex chamber A ratio of approximately less than and equal to 1:6 is characterized, for example. The outflow cross-section, the high pressure of the hollow cylinder and the acting low pressure determine the transfer velocity of the central vortex. Therefore, the potential energy of the high pressure that creates the stratified central vortex in the hollow cylinder cannot act radially, but is converted into kinetic energy by the nozzle shape below the outlet hole of the hollow cylinder, and this kinetic energy causes a stable vortex The acceleration of the outer peripheral speed.
其结果是,产生稳定的、结构可以调节的和增强的高集中速度和/或高集中质量以及高环量的中心涡流。在流入主流之前制造了新的涡流形状的全部存在条件。这种中心涡流的环量和集中质量例如完全可用于制造涡流圈的诱导过程。与没有集中质量的简单的环量比较起来,通过可压缩流体的集中速度和集中质量提高了功率。The result is a stable, structurally adjustable and enhanced central vortex with high concentrated velocity and/or high concentrated mass and high circulation volume. Creates all the conditions for the new vortex shape to exist before flowing into the main flow. The circulation and concentrated mass of such a central vortex can be fully used, for example, in the induction process for producing the vortex circle. The concentrated velocity and concentrated mass of the compressible fluid increases power compared to a simple circulation without a concentrated mass.
这可从计算涡流圈的诱导中心速度的关系式中得出,即环量与旋涡数的乘积除以涡流圈长度。根据本发明,势涡的数量通过在一个空间内制造的环量来集中,这样,在该圆上便可设置大得多的总环量。This can be derived from the relationship for calculating the induced center velocity of the swirl circle, which is the product of the circulation and the number of swirls divided by the length of the swirl ring. According to the invention, the number of potential vortices is concentrated by the circulation produced in a space, so that a much larger total circulation can be arranged on this circle.
根据本发明,可使涡流的环量和空间需要适合换能器的结构和能的需求。According to the invention, the circulation volume and space requirements of the eddy current can be adapted to the structure and energy requirements of the transducer.
用本发明方法产生的新的效果是,将一个与时间有关的集中速度过程在高压力作用下与准封闭空间中的轴向的集中速度和集中质量的中心涡流的形成过程结合起来。The new effect produced by the method according to the invention is the combination of a time-dependent concentrated velocity process under the action of high pressure with an axially concentrated velocity in a quasi-enclosed space and the formation of a central vortex of the concentrated mass.
本发明的第二装置同样可用于要制造能量集中的全部流体中。The second device of the invention can likewise be used in all fluids in which energy concentrations are to be produced.
本发明的几个实施例表示在附图中,并在下面进行详细说明。附图表示:Several embodiments of the invention are shown in the drawings and described in detail below. The accompanying drawings indicate:
图1表示第一装置实施例的一个纵截面示意图;Fig. 1 represents a schematic longitudinal section of the first device embodiment;
图2表示图1实施例的一个横截面;Fig. 2 represents a cross-section of Fig. 1 embodiment;
图3表示第二装置实施例的一个纵截面示意图;Fig. 3 shows a schematic longitudinal section of the second device embodiment;
图4表示图3实施例截面A-A的横截面示意图;Fig. 4 represents the schematic cross-sectional view of Fig. 3 embodiment section A-A;
图5表示在一个有势涡中的质点运动机理的三维示意图。Fig. 5 shows a three-dimensional schematic diagram of the particle motion mechanism in a potential vortex.
图1表示第一装置第一实施例,在一个底面1上设置了一个空心圆柱体2和一个螺旋形的包络涡发生器3。空心圆柱体2在其外圆周表面上有一个入流孔4,且其端面用一个遮盖面5盖住,遮盖面5的中心设置一个出流孔6,用出流孔6的半径以及空心圆柱体2的外半径可调节一个要制造的有势中心涡的集中速度。而环量则只由空心圆柱体2的外半径和外圆周速度来确定。FIG. 1 shows a first embodiment of a first device, on a base 1 a
一次制造成的环量在横截面变化和涡流平移时由于能量守恒的原因必定保持相等。Due to the reason of energy conservation, the amount of circulation produced at one time must remain equal when the cross-section changes and the vortex translates.
在底面1上设置了一个具有一个包络涡的相同旋转轴的包络涡发生器3。该发生器由一个一侧敞口的圆柱体7组成,它的横截面8为螺旋形。在圆柱体7中设置了一个具有相同中心的空心圆柱体2。空心圆柱体2的外圆周表面和圆柱体7的螺旋形敞口的内圆周表面在空心圆柱体2的入流孔4上方具有一个按流体力学确定的距离。这样构成的流动空间9用来制造空心圆柱体2外部的绕流。An enveloping
在空心圆柱体2入流孔4的范围内,圆柱体7的圆周表面10上开有孔,孔11终止于遮盖面5下方的入流孔4。遮盖面5最好由一个截锥表面组成,其最小的直径由出流孔6构成。一侧敞口的螺旋形圆柱体7的圆周表面伸出空心圆柱体2,伸出的长度按流体力学确定,但至少是空心圆柱体2的大约两倍的长度。这样,在出流的涡流稳定插入流入要产生的主流中时就可得出一个理想的总高度。这里对不同的尺寸需要经验的试验。In the area of the
圆周表面10形成一个垂直于主流设置的入流横截面12。入流横截面12通过孔11扩大,所以主流同样可垂直流经入流孔4。The
当流体流经本发明第一装置时,在起动阶段有三个体积流量在相同的旋转轴起作用。When the fluid flows through the first device of the invention, three volume flows act on the same axis of rotation during the start-up phase.
流入入流孔4的部分体积流量产生高压并在空心圆柱体2中产生一个相应减小的外圆周速度,由该圆周速度在空心圆柱体2中产生一个环量。The partial volume flow into the
在入流孔4的范围内流入入流横截面12的部分体积流量通过圆柱体7的螺旋形入流绕空心圆柱体2产生一个旋流,该旋流具有一个平移分量并超过遮盖面5保持不变。同时流经入流孔4的垂直入流通过这个旋流叠加,所以增加了空心圆柱体2的外圆周速度和环量。The helical inflow of the partial volume flow into the
在孔11上方的入流横截面12范围内流入的部分体积流量制造一个旋涡形的管状涡。这个管状涡在出流孔6上方产生一个快速的旋转,从而形成一个低压中心,并在出流孔6上方产生作用。如果在起动阶段后形成全部流体状态,则通过出流孔6在空心圆柱体2的入流孔4中开始产生一个抽吸过程,这个过程由出流孔6上方的旋涡形包络涡的低压中心的低压大小来确定。The partial volume flow flowing in in the region of the
在圆柱体2中制造的势涡按入流孔半径的0.65构成一个旋涡中心,在这个旋涡中心保持最高的圆周速度。The potential vortex produced in the
这样可平移的有势中心涡根据旋转动量守恒定律具有在空心圆柱体2内可进行调节的环量。Such a translatable potential central vortex has an adjustable circulation within the
这个有势中心涡被拉入包络涡的低压中心,从而在空心圆柱体2内产生一个圆周速度的加速。同时由于包络涡在边界层旋转到低压中心时的较高的圆周速度,这个包络涡便向外推动流入的有势中心涡,这样,有势中心涡内的高压降压成动能,并产生一个稳定的加速度。This potential central vortex is drawn into the low-pressure center of the envelope vortex, thereby producing an acceleration of peripheral velocity within the
根据本发明,包络涡的低压中心通过截锥形的遮盖面5和在出流孔6适合出流口6范围内要流出的有势中心涡的直径,所以设置的边界层变得有效。这样,有势中心涡便可无扰动地流入低压中心。因此,两股涡流汇合成一个新的涡流形状而不需外部的扰动流入。According to the invention, the low-pressure center of the envelope vortex passes through the frusto-
图3表示第二装置的一个实施例,在这个装置中,在底面21上设置了一个空心圆柱体22以及朝入流横截面31设置了一个空心圆柱体的螺旋形开孔。空心圆柱体22用一个遮盖面26盖住。在空心圆柱体22基圆的上面设置了一个带有一个出流孔30的喷嘴锥体32。在喷嘴锥体32下方构成一个膨胀室33,它由涡流室35的喷嘴锥体25的一个通流孔28限定。在涡流室35下方设置了一个涡流室36,涡流室36由带有中心通流孔29的喷嘴锥体24以及带有出流孔30的喷嘴锥体23构成。涡流室27由底面21限定。膨胀室33以及涡流室35;36;37通过图中未示出的螺旋形入口与入流横截面31连通。FIG. 3 shows an exemplary embodiment of the second device, in which a hollow cylinder 22 is provided on the bottom surface 21 and a helical opening of the hollow cylinder is provided towards the inflow cross section 31 . The hollow cylinder 22 is covered by a cover surface 26 . A nozzle cone 32 with an outlet opening 30 is arranged on the base circle of the hollow cylinder 22 . An expansion chamber 33 is formed below the nozzle cone 32 , which is delimited by a throughflow opening 28 of the nozzle cone 25 of the swirl chamber 35 . Arranged below the swirl chamber 35 is a swirl chamber 36 which is formed by the nozzle cone 24 with the central throughflow opening 29 and the nozzle cone 23 with the outlet opening 30 . A swirl chamber 27 is defined by the bottom surface 21 . The expansion chamber 33 and the vortex chamber 35 ; 36 ; 37 communicate with the inflow cross section 31 via a spiral inlet, not shown in the figures.
环量Γ在螺旋形入口时由平均的入口半径re和在该半径上保持的流速来确定。环量按下式计算:Γ=Ve·2π·reThe circulation Γ in the case of a spiral inlet is determined by the mean inlet radius re and the flow velocity maintained at this radius. The circulation is calculated according to the following formula: Γ=Ve·2π·re
从中可得出这样的结论:在膨胀室33和涡流室35;36;37中根据较小的出流孔和通流孔建立的高压降低平均入流速度并相应降低环量。这个速度的降低与一个在出流孔27上方面积形作用的低压起相反作用。在图中未详细示出的用来产生低压的装置可任意选择,只是旋涡中心流体的未扰动的运送应当是有条件的。借助于低压作用一次制造的较高环量必需在横截面变化和涡流中心流体转移时在涡流室35;36;37的内部和膨胀室33中由于能量守恒的原因必需保持不变。From this it can be concluded that the high pressure that builds up in the expansion chamber 33 and the swirl chamber 35 ; 36 ; 37 due to the smaller outflow and throughflow openings reduces the mean inflow velocity and correspondingly reduces the circulation volume. This reduction in velocity counteracts an area-shaped low pressure acting above the outlet opening 27 . The means for generating the low pressure, which are not shown in detail in the figures, can be chosen arbitrarily, but an undisturbed delivery of the fluid in the center of the vortex should be a condition. The higher circulation produced once by means of the effect of low pressure must remain constant in the interior of the vortex chambers 35 ; 36 ; 37 and in the expansion chamber 33 for reasons of energy conservation during cross-sectional changes and fluid transfers in the vortex centers.
当流体流经第二装置时,体积流量分成四个不等的分流量,并呈螺旋形流入膨胀室33和涡流室35;36;37中。根据产生的高压,内腔33;35;36;37中的螺旋形入流转变成一种势涡形状,这样圆周速度朝旋转轴34的方向增加。在涡流中心产生最大的圆周速度。由出流孔27和通流孔28;29;30引起的涡流中心可用0.65半径进行调节。亦即由于能量守恒定律的原因,随着出流孔逐渐变小而产生较大的圆周速度。这是通过试验证明了的,而且是可重复的。在涡流室37中在通流孔30上方制造的环量Z1在起动阶段结束后构成的涡流中心为0.65r10。涡流室36的涡流中心通过直径选择相当于环量Z1的外圆周速度的通流孔29。环量Z2包络环量Z1。环量Z3包络环量Z2,环量Z4包络环量Z3。全部涡流中心Z1至Z4都是根据出流孔或通流孔的半径制造的,并且只要分界层中出现圆周速度差,这些涡流中心就会在这种分层的涡流中心流体中独立存在。由于朝出流孔27去的高压不断变小,在旋转轴上方的环量Z1的横截面中保持最大的高压势。由于在出流面27上方每单位面积上作用的高压是相等的,所以在环量Z1中由于高压比低压的压差而产生最大的迁移速度。这样,Z2至Z4移动和旋转到旋转轴34所需的势位是稳定的。在膨胀室33中可通过所有圆周速度均化为一个合成的速度场来实现涡流的稳定性。由于环量、集中速度和集中质量作为面积积分必须保持不变,所以构成一个符合这些存在条件的实际涡流。When the fluid flows through the second device, the volume flow is divided into four unequal fractions and flows helically into the expansion chamber 33 and the vortex chamber 35; 36; 37. Depending on the high pressure generated, the helical inflow in the inner chamber 33 ; 35 ; 36 ; 37 is transformed into a potential vortex shape, so that the peripheral speed increases in the direction of the axis of rotation 34 . The maximum peripheral velocity is generated at the center of the vortex. The vortex center caused by the outlet hole 27 and the through hole 28; 29; 30 can be adjusted with a radius of 0.65. That is to say, due to the law of energy conservation, a larger peripheral velocity is generated as the outlet hole gradually becomes smaller. This has been demonstrated experimentally and is reproducible. The circulation Z1 produced in the vortex chamber 37 above the throughflow opening 30 forms a vortex center of 0.65r 10 after the end of the start-up phase. The vortex center of the vortex chamber 36 passes through the flow opening 29 whose diameter is chosen to correspond to the outer circumferential speed of the circulation Z1. The circulation Z2 envelops the circulation Z1. The circulation Z3 envelops the circulation Z2, and the circulation Z4 envelops the circulation Z3. All swirl centers Z1 to Z4 are produced according to the radii of the outlet or through-holes and are present independently in such a stratified swirl center fluid as long as there is a peripheral velocity difference in the boundary layer. Due to the ever-decreasing high pressure towards the outlet opening 27, a maximum high pressure potential remains in the cross-section of the circulation Z1 above the axis of rotation. Since the high pressure per unit area above the outflow surface 27 is equal, the maximum migration velocity is generated in the circulation Z1 due to the pressure difference between the high pressure and the low pressure. In this way, the potentials required for Z2 to Z4 to move and rotate to the rotation axis 34 are stabilized. The stabilization of the vortex can be achieved in the expansion chamber 33 by averaging all peripheral velocities into a resultant velocity field. Since the circulation volume, concentrated velocity and concentrated mass must remain constant as area integrals, a real vortex conforming to these conditions of existence is constituted.
图4以横截面表示环量Z1至Z4,通过入流横截面31流入的体积流量通过喷嘴锥体25下方和上方的空心圆柱体22的螺旋形孔口导向并通过该锥体隔开,喷嘴锥体25的出流孔位于环量Z4下方,并相当于环量Z4的内边界层线。4 shows the circulations Z1 to Z4 in cross-section, the volume flow flowing in through the inflow cross-section 31 is guided and separated by the helical orifice of the hollow cylinder 22 below and above the nozzle cone 25, the nozzle cone The outflow hole of the body 25 is located below the circulation Z4 and corresponds to the inner boundary layer line of the circulation Z4.
由于高压以及由于出流孔27上方作用的低压使平行于旋转轴34的涡流中心流体产生平移。在膨胀室33和涡流室35;36;37中根据相应流体横截面减去的质量部分在保持旋转时必须补充。由于在势涡理论中没有产生质量流量,所以能量传输必须是无损失地进行。如图5原理图所示,在相应分界层的排出的空间中支承的势涡内的质点的位置交换是与热涡旋转方向相反向内并通过重力向下方的平面进行的。图5示意描述了这样一种位置交换过程。从图中可看出,圆周速度较慢的质点在外半径上形成一个管形的标准势N1,该标准势在整个高度上都是相等的。标准势N2表示由于半径减小而引起的一个较高的圆周速度,标准势N3和N4也是如此。当一个用黑球表示的质点被拉入轴流中时,则会短时间地产生一个空的空间,这个空间在同心的流线上用白球即所谓空隙球来表示。由于重力作用和一个较快的圆周速度的势作用,一个质点从一个外部标准势N3加速返回到空位上的标准势N4中。标准势N3上的空位被标准势N2的一个质点占据,于是空隙球转移到标准势N1。质点向里移入旋涡中,空隙球方向相反离开该旋涡。圆周速度的势和重力作用都可以看出,所以通过一个势涡的质量流量只与涡流中心流体的平移速度有关。这些过程是可以重复的。The fluid in the center of the vortex parallel to the axis of rotation 34 is translated in translation by the high pressure and by the low pressure acting above the outlet orifice 27 . The mass fraction subtracted from the respective fluid cross sections in the expansion chamber 33 and the vortex chamber 35 ; 36 ; 37 must be replenished while the rotation is maintained. Since no mass flow occurs in potential vortex theory, energy transfer must be lossless. As shown in the schematic diagram of Fig. 5, the position exchange of the particles in the potential vortex supported in the discharged space of the corresponding boundary layer is carried out on the plane opposite to the rotation direction of the thermal vortex, inward and downward by gravity. Figure 5 schematically describes such a location exchange process. It can be seen from the figure that the mass point with a slower peripheral velocity forms a tube-shaped standard potential N1 on the outer radius, and the standard potential is equal on the entire height. The standard potential N2 represents a higher peripheral velocity due to the reduced radius, as do the standard potentials N3 and N4. When a particle represented by a black sphere is pulled into the axial flow, an empty space is briefly created, which is represented by a white sphere, the so-called interstitial sphere, on the concentric streamlines. Due to the gravitational effect and the potential effect of a faster peripheral velocity, a particle accelerates from an external standard potential N3 back to the standard potential N4 on the vacancy. The vacancy on the standard potential N3 is occupied by a particle of the standard potential N2, so the interstitial sphere is transferred to the standard potential N1. The particles move inward into the vortex, and the interstitial balls leave the vortex in the opposite direction. Both the potential and gravitational effects of peripheral velocity can be seen, so the mass flow through a potential vortex is only related to the translational velocity of the fluid in the center of the vortex. These processes are repeatable.
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ES454192A1 (en) * | 1976-12-13 | 1977-12-01 | Zapata Martinez Valentin | System for the obtainment and the regulation of energy starting from air, sea and river currents |
US4309146A (en) * | 1980-03-12 | 1982-01-05 | The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration | Amplified wind turbine apparatus |
ES8301330A1 (en) * | 1980-07-24 | 1982-12-01 | Central Energetic Ciclonic | System for the obtaining of energy by fluid flows resembling a natural cyclone or anti-cyclone |
US4452562A (en) * | 1983-05-06 | 1984-06-05 | Iowa State University Research Foundation, Inc. | Tornado type wind turbines |
DE4107208A1 (en) * | 1991-03-04 | 1992-09-10 | Juergen Schatz | System for generating system energy from atmospheric winds - uses wind power generator tower with collection and equipment storey |
DE4117838A1 (en) * | 1991-05-29 | 1992-12-03 | Juergen Schatz | METHOD AND DEVICE FOR THE ENERGY USE OF GASEOUS FABRIC FLOWS, ESPECIALLY SLOWLY FLOWING FABRIC FLOWS |
DE4302823A1 (en) * | 1993-01-28 | 1995-02-09 | Juergen Schatz | Method and device for generating a vortex coil in a vortex |
DE4309588A1 (en) * | 1993-03-22 | 1994-09-29 | Juergen Schatz | Method and device for generating energetically useful vorticity from parallel flows |
DE4429376A1 (en) * | 1994-08-12 | 1996-02-15 | Juergen Schatz | Wind rotor for use in all weathers |
-
1996
- 1996-07-05 CN CN96196454A patent/CN1217767A/en active Pending
- 1996-07-05 PL PL96324623A patent/PL324623A1/en unknown
- 1996-07-05 JP JP9504724A patent/JPH11508661A/en active Pending
- 1996-07-05 CA CA002226122A patent/CA2226122A1/en not_active Abandoned
- 1996-07-05 WO PCT/DE1996/001251 patent/WO1997002431A1/en not_active Application Discontinuation
- 1996-07-05 TR TR1998/00005T patent/TR199800005T1/en unknown
- 1996-07-05 EP EP96923827A patent/EP0836677A1/en not_active Withdrawn
- 1996-07-05 BR BR9609593-8A patent/BR9609593A/en not_active Application Discontinuation
- 1996-07-05 AU AU64124/96A patent/AU6412496A/en not_active Abandoned
-
1998
- 1998-01-05 NO NO980031A patent/NO980031L/en unknown
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109607658A (en) * | 2018-12-30 | 2019-04-12 | 中海油能源发展股份有限公司安全环保分公司 | A kind of adjustable cyclone air-flotation device of swirl strength and operating method |
CN109607658B (en) * | 2018-12-30 | 2023-12-15 | 中海油能源发展股份有限公司安全环保分公司 | Cyclone air floatation device with adjustable cyclone strength and operation method |
CN111852771A (en) * | 2020-07-29 | 2020-10-30 | 西南石油大学 | A small wind energy generating device and method for self-adapting wind direction and wind speed |
CN111852771B (en) * | 2020-07-29 | 2022-03-08 | 西南石油大学 | Small wind power generation device and method adaptive to wind direction and wind speed |
CN113931807A (en) * | 2021-08-25 | 2022-01-14 | 华北电力大学 | A method for measuring the operating angle of attack of wind turbine blades |
CN113931807B (en) * | 2021-08-25 | 2023-04-21 | 华北电力大学 | A method for measuring the angle of attack of wind turbine blade operation |
Also Published As
Publication number | Publication date |
---|---|
BR9609593A (en) | 1999-12-21 |
EP0836677A1 (en) | 1998-04-22 |
WO1997002431A1 (en) | 1997-01-23 |
AU6412496A (en) | 1997-02-05 |
JPH11508661A (en) | 1999-07-27 |
NO980031L (en) | 1998-03-05 |
TR199800005T1 (en) | 1998-04-21 |
CA2226122A1 (en) | 1997-01-23 |
PL324623A1 (en) | 1998-06-08 |
NO980031D0 (en) | 1998-01-05 |
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