CN102664511A - Method for generating electromagnetic force with temporal and spatial variation in conducting liquid by adopting fluid driving - Google Patents
Method for generating electromagnetic force with temporal and spatial variation in conducting liquid by adopting fluid driving Download PDFInfo
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Abstract
本发明涉及一种采用流体驱动在导电液体中产生时空变化的电磁力的方法,属于电磁冶金、半导体材料制备、化学工业和玻璃工业技术领域。首先在导电液体中形成一个圆柱形腔体,腔体上设有驱动流体通道口,将涡轮叶片置于圆柱形腔体中,将永磁体与涡轮叶片相对固定;使驱动流体以周期P从腔体的通道口进入或流出,驱动流体驱动涡轮叶片以周期P作正向或反向转动,并带动永磁体转动,产生方向周期变化的的旋转磁场,在腔体外部周围的导电液体内产生涡电流,旋转磁场与涡电流相互作用,产生电磁力,驱动或搅拌导电液体。采用本发明方法构成的电磁驱动器,可用于金属凝固过程中来改善宏观偏析、金属合金化过程以及制备梯度材料、复合材料等领域。
The invention relates to a method for generating a time-space-varying electromagnetic force in a conductive liquid driven by a fluid, and belongs to the technical fields of electromagnetic metallurgy, semiconductor material preparation, chemical industry and glass industry. Firstly, a cylindrical cavity is formed in the conductive liquid, and the cavity is provided with a drive fluid passage port, the turbine blade is placed in the cylindrical cavity, and the permanent magnet and the turbine blade are relatively fixed; the drive fluid flows from the cavity at a period P The passage port of the body enters or flows out, and the driving fluid drives the turbine blades to rotate forward or reverse at a period P, and drives the permanent magnet to rotate, generating a rotating magnetic field with a periodically changing direction, and generating a vortex in the conductive liquid around the outside of the cavity. The electric current, the rotating magnetic field and the eddy current interact to generate an electromagnetic force that drives or stirs the conductive liquid. The electromagnetic driver formed by the method of the invention can be used in the fields of improving macroscopic segregation, metal alloying process, preparing gradient materials, composite materials and the like in the process of metal solidification.
Description
技术领域 technical field
本发明涉及一种采用流体驱动在导电液体中产生时空变化的电磁力的方法,属于电磁冶金、半导体材料制备、化学工业和玻璃工业技术领域。The invention relates to a method for generating a time-space-varying electromagnetic force in a conductive liquid driven by a fluid, and belongs to the technical fields of electromagnetic metallurgy, semiconductor material preparation, chemical industry and glass industry.
背景技术 Background technique
传统的电磁驱动技术由于受到趋肤效应的制约,对于较大尺寸的导电液体驱动效果极为有限。专利(申请号:201210039850.3)提出了一种以流体作为驱动介质在导电液体中产生电磁力的方法,用流体驱动代替已有技术中的电或机械驱动,以简化电磁驱动器的结构,增加设计的灵活性,并扩大电磁驱动器的应用范围。但传统的电磁驱动技术与上述方法存在如下不足:磁场形态单一,产生的电磁力在空间分布较为固定,因而被驱动的导电流体的流场一般不随时间变化,电磁力再导电液体内的空间分布可调性差,具有如下缺点:Due to the restriction of the skin effect, the traditional electromagnetic actuation technology is extremely limited in the actuation effect for larger-sized conductive liquids. The patent (application number: 201210039850.3) proposes a method of using fluid as the driving medium to generate electromagnetic force in a conductive liquid, replacing the electric or mechanical drive in the prior art with fluid drive, so as to simplify the structure of the electromagnetic drive and increase the design flexibility. flexibility, and expand the application range of electromagnetic drives. However, the traditional electromagnetic drive technology and the above method have the following disadvantages: the magnetic field has a single form, and the generated electromagnetic force has a relatively fixed spatial distribution, so the flow field of the driven conductive fluid generally does not change with time, and the spatial distribution of the electromagnetic force in the conductive liquid Poor adjustability has the following disadvantages:
(i)对于合金的凝固问题,由于金属液体的受迫对流模式固定,溶质再分配效果较差,而且研究表明(王晓东等,材料论坛,第508卷,第163-168页):有时不当的电磁场作用不但不能消除浓度偏析,而且还会增大浓度偏析,直接破坏材料的使役性能;(i) For the solidification of alloys, due to the fixed forced convection mode of the metal liquid, the solute redistribution effect is poor, and studies have shown (Wang Xiaodong et al., Materials Forum, Vol. 508, pp. 163-168): sometimes inappropriate The action of electromagnetic field not only cannot eliminate the concentration segregation, but also increases the concentration segregation, directly destroying the service performance of the material;
(ii)在导电流体中形成稳定的热边界层,在需要充分传热的场合下传热效果差;(ii) A stable thermal boundary layer is formed in the conductive fluid, and the heat transfer effect is poor when sufficient heat transfer is required;
(iii)在导电流体中形成稳定的流体流动边界层,导电液体不能被充分地搅拌;(iii) A stable fluid flow boundary layer is formed in the conductive fluid, and the conductive liquid cannot be stirred sufficiently;
(iv)不能根据需要获得可设计的较高的电磁力密度梯度场。(iv) A designable higher electromagnetic force density gradient field cannot be obtained as required.
本申请人曾经发表了一种基于传统电磁搅拌技术的模式电磁力办法(王晓东等,冶金与材料通讯B,模式电磁场驱动的周期性反转流I和II,第40卷,2009年,82-90页,104-113页),在凝固前沿模式电磁力场可造成熔体的周期性流动,充分改变溶质的再分配过程,在优化的模式频率作用范围内可达到显著改善凝固过程中浓度偏析的目的。The applicant once published a model electromagnetic force method based on traditional electromagnetic stirring technology (Wang Xiaodong et al., Metallurgy and Materials Communication B, Periodic Countercurrent I and II Driven by Model Electromagnetic Field, Volume 40, 2009, 82- 90 pages, 104-113 pages), the electromagnetic force field in the solidification front mode can cause the periodic flow of the melt, fully change the redistribution process of the solute, and can significantly improve the concentration segregation in the solidification process within the range of the optimized mode frequency the goal of.
发明内容 Contents of the invention
本发明的目的是提出一种采用流体驱动在导电液体中产生时空变化的电磁力的方法,对已有的在导电流体中产生电磁力的方法做出改进,通过驱动流体流量和方向变化来得到周期性变化的电磁力场,以扩展通过流体驱动产生电磁力的用途。The purpose of the present invention is to propose a method of using fluid to drive the electromagnetic force that generates spatiotemporal changes in the conductive liquid, to improve the existing method for generating the electromagnetic force in the conductive fluid, and to obtain by driving the fluid flow and direction changes Periodically varying electromagnetic force fields to expand the use of electromagnetic forces generated by fluid actuation.
本发明提出的采用流体驱动在导电液体中产生时空变化的电磁力的方法,有多种不同的方案,其中第一种方案包括以下步骤:The method of adopting fluid to drive the electromagnetic force that produces spatiotemporal changes in the conductive liquid proposed by the present invention has multiple different schemes, wherein the first scheme includes the following steps:
(1)在导电液体中形成一个圆柱形腔体,腔体上设有驱动流体的第一通道口和第二通道口;(1) A cylindrical cavity is formed in the conductive liquid, and the first channel opening and the second channel opening of the driving fluid are arranged on the cavity;
(2)将涡轮叶片置于圆柱形腔体中,涡轮叶片安装在轴承上,轴承与圆柱形腔体同轴安装;(2) Place the turbine blade in the cylindrical cavity, install the turbine blade on the bearing, and install the bearing coaxially with the cylindrical cavity;
(3)将永磁体与涡轮叶片相对固定;(3) Relatively fix the permanent magnet and the turbine blade;
(4)使驱动流体以周期P从圆柱形腔体上的第一通道口或第二通道口进入或流出,驱动流体驱动涡轮叶片以周期P作正向或反向转动,并带动永磁体以周期P作正向或反向转动,产生方向以周期P变化的旋转磁场,旋转磁场在圆柱形腔体外部周围的导电液体内产生涡电流,旋转磁场与涡电流相互作用,产生方向以周期P变化的电磁力,驱动或搅拌导电液体。(4) Make the driving fluid enter or flow out from the first channel port or the second channel port on the cylindrical cavity at a period P, and the driving fluid drives the turbine blades to rotate forward or reverse at a period P, and drives the permanent magnet to The period P rotates forward or reversely to generate a rotating magnetic field whose direction changes with a period P. The rotating magnetic field generates an eddy current in the conductive liquid around the outside of the cylindrical cavity. The rotating magnetic field interacts with the eddy current to generate a direction with a period P. The changing electromagnetic force drives or stirs the conductive liquid.
上述第一种方案中,所述的永磁体与涡轮叶片相对固定的形式为:设置两个圆盘状连接板,两个连接板分别置于涡轮叶片的两侧,两个连接板的内侧分别与涡轮叶片连接,两个连接板的外侧分别设置第一永磁体和第二永磁体,形成第一磁场和第二磁场。In the above-mentioned first solution, the relative fixed form of the permanent magnet and the turbine blade is as follows: two disc-shaped connecting plates are arranged, and the two connecting plates are respectively placed on both sides of the turbine blade, and the inner sides of the two connecting plates are respectively Connected with the turbine blades, a first permanent magnet and a second permanent magnet are respectively arranged on the outer sides of the two connecting plates to form a first magnetic field and a second magnetic field.
上述第一种方案中,所述的永磁体与涡轮叶片相对固定的形式为:设置一个圆筒形连接板,涡轮叶片与圆筒形连接板连接,圆筒形连接板位于涡轮叶片的外端部,永磁体安装在圆筒形连接板上,第五通道口和第六通道口置于圆柱形腔体的端面。In the above-mentioned first solution, the relative fixed form of the permanent magnet and the turbine blade is as follows: a cylindrical connecting plate is set, the turbine blade is connected with the cylindrical connecting plate, and the cylindrical connecting plate is located at the outer end of the turbine blade In the first part, the permanent magnet is installed on the cylindrical connecting plate, and the fifth channel port and the sixth channel port are placed on the end surface of the cylindrical cavity.
其中第二种方案包括以下步骤:The second option includes the following steps:
(1)设置一个内筒和一个外筒,内筒和外筒同轴安装,内筒和外筒之间形成一个套筒形腔体,套筒形腔体的端面上设有驱动流体的第七通道口和第八通道口;(1) Set an inner cylinder and an outer cylinder, the inner cylinder and the outer cylinder are installed coaxially, a sleeve-shaped cavity is formed between the inner cylinder and the outer cylinder, and the end surface of the sleeve-shaped cavity is provided with a first drive fluid. Seventh passageway and eighth passageway;
(2)设置一个圆筒形连接板,涡轮叶片与圆筒形连接板的一侧连接,圆筒形连接板位于涡轮叶片的内端部,永磁体安装在圆筒形连接板的另一侧,将涡轮叶片置于圆柱形腔体中,涡轮叶片安装在轴承上,轴承与圆柱形腔体同轴安装;(2) Set a cylindrical connecting plate, the turbine blade is connected to one side of the cylindrical connecting plate, the cylindrical connecting plate is located at the inner end of the turbine blade, and the permanent magnet is installed on the other side of the cylindrical connecting plate , the turbine blade is placed in the cylindrical cavity, the turbine blade is installed on the bearing, and the bearing is coaxially installed with the cylindrical cavity;
(3)使驱动流体以周期P从圆柱形腔体上的第七通道口或第八通道口进入或流出,驱动流体驱动涡轮叶片以周期P作正向或反向转动,并带动永磁体以周期P作正向或反向转动,产生方向以周期P变化的旋转磁场,旋转磁场在内筒的内侧和外筒的外侧的导电液体内产生涡电流,旋转磁场与涡电流相互作用,产生方向以周期P变化的电磁力,驱动或搅拌导电液体。(3) The driving fluid enters or flows out from the seventh or eighth channel on the cylindrical cavity with a period P, and the driving fluid drives the turbine blades to rotate forward or reverse with a period P, and drives the permanent magnet to The period P rotates forward or reversely to generate a rotating magnetic field whose direction changes with the period P. The rotating magnetic field generates an eddy current in the conductive liquid inside the inner cylinder and outside the outer cylinder. The rotating magnetic field interacts with the eddy current to generate a direction Drive or stir the conductive liquid with the changing electromagnetic force of period P.
其中第三种方案包括以下步骤:The third option includes the following steps:
(1)设置一个内筒和一个外筒,内筒和外筒同轴安装,内筒和外筒之间形成一个套筒形腔体,腔体的端面上设有驱动流体的第七通道口和第八通道口;(1) Set an inner cylinder and an outer cylinder, the inner cylinder and the outer cylinder are installed coaxially, a sleeve-shaped cavity is formed between the inner cylinder and the outer cylinder, and the end surface of the cavity is provided with a seventh channel port for driving fluid and the eighth aisle;
(2)设置一个圆筒形连接板,涡轮叶片与圆筒形连接板的一侧连接,圆筒形连接板位于涡轮叶片的内端部,永磁体安装在圆筒形连接板的另一侧,将涡轮叶片置于圆柱形腔体中,涡轮叶片安装在轴承上,轴承与圆柱形腔体同轴安装;(2) Set a cylindrical connecting plate, the turbine blade is connected to one side of the cylindrical connecting plate, the cylindrical connecting plate is located at the inner end of the turbine blade, and the permanent magnet is installed on the other side of the cylindrical connecting plate , the turbine blade is placed in the cylindrical cavity, the turbine blade is installed on the bearing, and the bearing is coaxially installed with the cylindrical cavity;
(3)使驱动流体以周期P从圆柱形腔体上的第七通道口或第八通道口进入或流出,驱动流体驱动涡轮叶片以周期P作正向或反向转动,并带动永磁体以周期P作正向或反向转动,产生方向以周期P变化的旋转磁场,在内筒的内侧和外筒的外侧的导电液体内产生涡电流,旋转磁场与涡电流相互作用,产生时空上周期性变化的电磁力,驱动或搅拌导电液体。(3) The driving fluid enters or flows out from the seventh or eighth channel on the cylindrical cavity with a period P, and the driving fluid drives the turbine blades to rotate forward or reverse with a period P, and drives the permanent magnet to The period P rotates in the forward or reverse direction to generate a rotating magnetic field whose direction changes with the period P, and eddy currents are generated in the conductive liquid inside the inner cylinder and outside the outer cylinder, and the rotating magnetic field interacts with the eddy current to generate a space-time period The electromagnetic force of sex change drives or stirs the conductive liquid.
其中第四种方案包括以下步骤:The fourth option includes the following steps:
(1)在导电液体中形成第一圆柱形腔体和第二圆柱形腔体,第一圆柱形腔体上分别设有驱动流体的第九通道口和第十通道口,第二圆柱形腔体上分别设有驱动流体的第十一通道口和第十二通道口;(1) A first cylindrical cavity and a second cylindrical cavity are formed in the conductive liquid. The first cylindrical cavity is respectively provided with the ninth channel port and the tenth channel port of the driving fluid, and the second cylindrical cavity The body is respectively provided with an eleventh channel port and a twelfth channel port for driving fluid;
(2)分别将涡轮叶片置于第一圆柱形腔体和第二圆柱形腔体中,涡轮叶片安装在轴承上,轴承与圆柱形腔体同轴安装;(2) The turbine blades are respectively placed in the first cylindrical cavity and the second cylindrical cavity, the turbine blades are installed on the bearings, and the bearings are coaxially installed with the cylindrical cavity;
(3)将第一永磁体和第二永磁体分别与涡轮叶片相对固定;(3) Fixing the first permanent magnet and the second permanent magnet to the turbine blades respectively;
(4)使驱动流体以周期P或P’分别从第一圆柱形腔体的第九通道口或第十通道口以及第二圆柱形腔体上的第十一通道口或第十二通道口进入或流出,驱动流体驱动涡轮叶片以周期P或P’作正向或反向转动,并带动永磁体产生以周期P或P’变化的旋转磁场,在两个圆柱形腔体外部周围的导电液体内产生涡电流,旋转磁场与涡电流相互作用,产生时空变化的电磁力场,驱动或搅拌导电液体。(4) Let the driving fluid flow from the ninth or tenth channel port of the first cylindrical cavity and the eleventh or twelfth channel port on the second cylindrical cavity with a cycle P or P' respectively In or out, the driving fluid drives the turbine blades to rotate forward or reverse with the period P or P', and drives the permanent magnet to generate a rotating magnetic field that changes with the period P or P', and conducts electricity around the outside of the two cylindrical cavities An eddy current is generated in the liquid, and the rotating magnetic field interacts with the eddy current to generate an electromagnetic force field that changes in time and space, driving or stirring the conductive liquid.
本发明提出的采用流体驱动在导电液体中产生时空变化的电磁力的方法,其优点在于:根据本发明提出的采用流体驱动在导电液体中产生电磁力的方法制造的电磁驱动器,实施手段简便、可靠;通过驱动流体流量和方向变化来实现具有周期性变化的电磁力场,电磁力的周期变化频率可根据实际需要作大范围调节,电磁力的大小也可通过驱动流体的流量变化进行调节,因而大大地扩大了应用领域范围。旋转磁场结构的设计灵活多样,例如,采用弧形或条形永磁体单元的盘状磁场结构,螺旋结构的磁场、磁魔环结构的筒形磁场等;电磁力场空间变化的可设计性和可控性很高,如可在导电液体中实现较高的电磁力密度梯度场。The method proposed by the present invention to drive the electromagnetic force generated in the conductive liquid by using the fluid to generate the space-time variation has the advantage that: the electromagnetic driver manufactured by the method used to drive the electromagnetic force generated by the fluid in the conductive liquid proposed by the present invention has simple and convenient means of implementation, Reliable; a periodically changing electromagnetic force field is realized by driving the fluid flow and direction changes. The frequency of the periodic change of the electromagnetic force can be adjusted in a wide range according to actual needs, and the magnitude of the electromagnetic force can also be adjusted by changing the flow rate of the driving fluid. Therefore, the range of application fields is greatly expanded. The design of the rotating magnetic field structure is flexible and diverse, for example, the disk-shaped magnetic field structure using arc or bar-shaped permanent magnet units, the magnetic field of the spiral structure, the cylindrical magnetic field of the magnetic magic ring structure, etc.; the designability and The controllability is very high, such as the high electromagnetic force density gradient field can be realized in the conductive liquid.
根据本发明提出的采用流体驱动在导电液体中产生电磁力的方法制造的电磁驱动器,可用于金属凝固过程中来改善宏观偏析,尤其是当金属熔体体积较大时情形;可用于金属合金化过程:分散添加的合金元素;可用于制备梯度材料、复合材料的工艺过程中:在导电液体内产生较大的电磁力密度场;可用于金属输运、模铸(包括紧密铸造)过程中金属液体温度场的均匀化;可用于加速除气、脱硫等冶金工艺过程。The electromagnetic driver manufactured by the method of generating electromagnetic force in the conductive liquid according to the fluid drive proposed by the present invention can be used in the process of metal solidification to improve macro-segregation, especially when the volume of the metal melt is large; it can be used for metal alloying Process: disperse the added alloy elements; can be used in the process of preparing gradient materials and composite materials: generate a large electromagnetic force density field in the conductive liquid; can be used in the process of metal transportation and die casting (including compact casting) Homogenization of liquid temperature field; can be used to accelerate metallurgical processes such as degassing and desulfurization.
附图说明 Description of drawings
图1是本发明提出的采用流体驱动在导电液体中产生时空变化的电磁力的方法的原理示意图,也是根据本发明方法设计的第一种磁驱动器的结构示意图。Fig. 1 is a schematic diagram of the principle of the method of using fluid drive to generate a time-space-varying electromagnetic force in a conductive liquid proposed by the present invention, and it is also a schematic structural diagram of the first magnetic driver designed according to the method of the present invention.
图2是驱动流体流量及方向在一个周期内随时间变化的波形图。Fig. 2 is a waveform diagram of the change of the flow rate and direction of the driving fluid with time in one cycle.
图3是根据本发明方法设计的第二种磁驱动器的结构示意图。Fig. 3 is a structural schematic diagram of a second magnetic driver designed according to the method of the present invention.
图4是根据本发明方法设计的第三种磁驱动器的结构示意图。Fig. 4 is a structural schematic diagram of a third magnetic driver designed according to the method of the present invention.
图5是根据本发明方法设计的第四种磁驱动器的结构示意图。Fig. 5 is a structural schematic diagram of a fourth magnetic driver designed according to the method of the present invention.
图6和图7分别是图4和图5中所示的磁驱动器中永磁体的两种不同结构的示意图。6 and 7 are schematic diagrams of two different structures of permanent magnets in the magnetic actuator shown in FIGS. 4 and 5, respectively.
图8是根据本发明方法设计的第五种磁驱动器的一种工作状态图。Fig. 8 is a working state diagram of the fifth magnetic driver designed according to the method of the present invention.
图9是图8所示的磁驱动器的另一种工作状态图。FIG. 9 is another working state diagram of the magnetic driver shown in FIG. 8 .
图1~图9中,1是导电液体;2是圆柱形腔体;3是第一通道口;4是第二通道口;5是涡轮叶片;6是轴承;7是永磁体;8是涡轮叶片的旋转方向;9是导电液体的流动方向;10是第三通道口;11是第四通道口;12是盘状第一连接板;13是盘状第二连接板;14是第一永磁体(由弧形永磁体单元组成);15是第二永磁体(由条形永磁体单元组成);16是圆筒状连接板;17是第五通道口;18是第六通道口;19是套筒形腔体;20是第七通道口;21是第八通道口;22是螺旋形永磁体;23是永磁体磁化方向;24是螺旋形永磁体支撑构架;25是磁场的旋转方向;26是磁魔环结构的永磁体;27是第一圆柱形腔体;28是第二圆柱形腔体;29是第九通道口;30是第十通道口;31是第十一通道口;32是第十二通道口。In Figures 1 to 9, 1 is a conductive liquid; 2 is a cylindrical cavity; 3 is the first channel opening; 4 is the second channel opening; 5 is the turbine blade; 6 is the bearing; 7 is the permanent magnet; 8 is the
具体实施方式 Detailed ways
以下结合附图,对本发明提出的采用流体驱动在导电液体中产生时空变化的电磁力的方法进行详细介绍。In the following, the method of using fluid to drive the electromagnetic force that generates spatiotemporal changes in the conductive liquid proposed by the present invention will be described in detail with reference to the accompanying drawings.
本发明方法有多种不同的方案,其中采用第一种方案设计的磁驱动器的结构如图1所示,包括以下步骤:The inventive method has multiple different schemes, wherein adopts the structure of the magnetic driver of first kind of scheme design as shown in Figure 1, comprises the following steps:
(1)在导电液体1中形成一个圆柱形腔体2,腔体上设有驱动流体的第一通道口3和第二通道口4;(1) A
(2)将涡轮叶片5置于圆柱形腔体1中,涡轮叶片5安装在轴承6上,轴承6与圆柱形腔体2同轴安装;(2) Place the
(3)将永磁体7与涡轮叶片5相对固定;(3) Relatively fixing the
(4)使驱动流体以周期P从圆柱形腔体上的第一通道口3或第二通道口4进入或流出,驱动流体驱动涡轮叶片5以周期P作正向或反向转动,并带动永磁体7以周期P作正向或反向转动,图1中示出了涡轮叶片的旋转方向8和导电流体的流动方向9,永磁体7在涡轮叶片5的带动下产生方向作周期性变化(周期P)的旋转磁场,旋转磁场在圆柱形腔体2外部周围的导电液体1内产生涡电流,旋转磁场与涡电流相互作用,产生方向作周期性变化(周期P)的电磁力,驱动或搅拌导电液体1。(4) Make the driving fluid enter or flow out from the first channel port 3 or the
图1示出了本发明方法的基本原理,通过驱动流体流动方向的周期性变化,实现涡轮叶片5转动方向的周期性变化,从而使与之一同运动的永磁体7也实现旋转方向的周期性变化。如图1(a)和图1(b)所示,变化的周期为P,频率为:f=1/P,在时间段T内(0<T<P)内涡轮叶片作逆时针(或顺时针)旋转,在(P-T)时间段内作顺时针(或逆时针)旋转。这种变化是通过第一通道口3作为流体流入口,第二通道口4作为流体流出口,或者第二通道口4作为流体流入口,第一通道口3作为流体流出口,周期性交替变化来实现的。Fig. 1 has shown the basic principle of the method of the present invention, realize the periodic change of the direction of rotation of the
图2所示为驱动流体流量及方向在一个周期内随时间变化的波形图,设驱动流体流量为Q,将驱动流体从第一通道口3流入的方向记为正,从第一通道口3流出的方向记为负,驱动流体流量随时间的周期性变化则可用图2(c)中的方波(i)来表示,也可以是方波,也可以是正(余)弦波,或类似正(余)弦波的其它波形,如图2(c)中的曲线(ii)所示。另外,由于驱动流体的惯性作用与考虑机械安全的原因,驱动流体换向需要一定时间,换向所需时间为2Tp,一般要求P>>Tp,如图2(c)中曲线(iii)所示,以保证导电液体1不但被充分驱动(驱动强度的幅值趋于饱和),而且实现周期性特征明显的模式流动。这种驱动流体的周期性变化也可以有另外一种间歇式的形式,如图2(d)所示,驱动流体在一个周期内作用一定长的时间(0<T<P),其余时间内驱动流体流量为零。Fig. 2 shows the waveform diagram of the flow rate and direction of the driving fluid changing with time in one cycle, assuming that the flow rate of the driving fluid is Q, the direction in which the driving fluid flows from the first channel port 3 is marked as positive, and the direction from the first channel port 3 is marked as positive. The outflow direction is recorded as negative, and the periodic change of the driving fluid flow rate with time can be represented by the square wave (i) in Figure 2(c), which can also be a square wave, or a positive (cos) sine wave, or similar Other waveforms of sine (cosine) waves are shown in curve (ii) in Fig. 2(c). In addition, due to the inertia of the driving fluid and the consideration of mechanical safety, it takes a certain amount of time for the driving fluid to change direction, and the time required for the change is 2T p , generally requiring P>>T p , as shown in the curve (iii) in Figure 2(c) ) to ensure that the
被驱动的导电液体1流动的周期性具有如下特征:驱动流体流动的周期性与被驱动的导电液体受到的电磁力的周期性相同;导电液体1所受电磁力的幅值变化与驱动流体的流量具有一定关系,导电流体1要获得具有明显周期特征的流动,驱动流体的流量需大于一定的阀值;驱动流体方向变化的周期与其流量(即流体的动能)要有一定的配合关系,要实现导电液体1的周期性流动,周期P也需大于一定的阀值。考虑到磁驱动器的尺寸特征与应用领域,导电液体1受到的电磁力场的频率f一般要小于0.2赫兹(周期P大于5秒)。The periodicity of the flow of the driven
根据本发明方法第二种方案设计的磁驱动器的结构如图3(e)所示,在圆柱形腔体2的侧壁上设置驱动流体的两个通道口,分别记为驱动流体的第三通道口10和驱动流体的第四通道口11,其中的永磁体7与涡轮叶片8相对固定的形式为:设置两个连接板12和13,两个连接板12、13分别置于涡轮叶片8的两侧,两个连接板12、13的内侧分别与涡轮叶片8连接,两个连接板12、13的外侧分别设置第一永磁体14和第二永磁体15,形成第一磁场和第二磁场。The structure of the magnetic driver designed according to the second scheme of the method of the present invention is shown in FIG. The
从图3(e)和图3(f)可以看出在这种结构中,连接板12和13为盘状且平行于圆柱形腔体2的端面,并采用双永磁体磁场结构,即第一永磁体14和第二永磁体15来实现空间变化的电磁力场。轴承6位于圆柱形腔体腔体2的中心,轴承6的内圈与圆柱形腔体2连接,轴承6的外圈与涡轮叶片5连接,保证涡轮叶片5在驱动流体作用下可自由转动,轴承6的外圈同时还与分列涡轮叶片5两侧的两个盘状连接板12、13连接,两个连接板12、13的内侧分别与涡轮叶片5连接,两个连接板12、13的外侧分别设置第一永磁体14和第二永磁体15,通过设计使两个永磁体14、15具有不同的结构,如图3(g)和图3(h)所示,第一永磁体14和第二永磁体15的磁体单元形状分别为圆弧形和长条形的永磁体。永磁体单元也可以根据需要设计成其它形状。永磁体旋转产生空间分布不同的涡电流,在导电液体内形成空间分布不同的电磁力场。根据需要在导电液体1内可获得较大的电磁力密度梯度的区域,这样的空间变化的大梯度电磁力场可用于某些材料的特殊制备工艺中。It can be seen from Fig. 3(e) and Fig. 3(f) that in this structure, the connecting
根据本发明方法第三种方案设计的磁驱动器的结构如图4所示,其中图4(i)是圆柱形腔体的内部结构示意图,图4(j)是其侧视图。永磁体7与涡轮叶片5相对固定的形式为:设置一个圆筒形连接板16,圆筒状连接板16与圆柱形腔体2同轴。涡轮叶片5与圆筒形连接板16连接(相连或镶嵌其中),圆筒形连接板16位于涡轮叶片5的外端部,永磁体14、15安装在圆筒形连接板16上。如图4(j)所示,驱动流体的两个通道口位于圆柱形腔体2的两个端面上,记为驱动流体的第五通道口17和第六通道口18,此时涡轮叶片8可设计成三维的异型结构,保证涡轮叶片8在驱动流体驱动下自由、平稳旋转。The structure of the magnetic actuator designed according to the third solution of the method of the present invention is shown in FIG. 4, wherein FIG. 4(i) is a schematic diagram of the internal structure of a cylindrical cavity, and FIG. 4(j) is a side view thereof. The
根据本发明方法第四种方案设计的磁驱动器的结构如图5所示,设置一个内筒和一个外筒,内筒和外筒同轴安装,并且具有两个端面,组成一个套筒形腔体19,其中图5(k)是套筒形腔体19的内部结构示意图,图5(l)是其侧视图,套筒形腔体19的端面上设有驱动流体的第七通道口20和第八通道口21;轴承6的外圈同轴安装在套筒形腔体19的外筒的内壁上,轴承6的内圈与涡轮叶片5连接,设置一个圆筒形连接板16,圆筒形连接板16的外侧与涡轮叶片5的内端部连接,永磁体14或15安装在圆筒形连接板的内侧(相连或镶嵌其中)。工作时使驱动流体以周期P从圆柱形腔体上的第七通道口20或第八通道口21进入或流出,驱动流体驱动涡轮叶片5以周期P作正向或反向转动,并带动永磁体以周期P作正向或反向转动,产生以周期P作正向或反向转动的旋转磁场,在套筒形腔体19的中心部分的导电液体1内产生涡电流,旋转磁场与涡电流相互作用产生以周期P作变化的电磁力,驱动或搅拌导电液体1。The structure of the magnetic driver designed according to the fourth scheme of the method of the present invention is shown in Figure 5, an inner cylinder and an outer cylinder are arranged, the inner cylinder and the outer cylinder are coaxially installed, and have two end faces to form a sleeve-shaped
图6是上述图4和图5中所示的磁驱动器中永磁体的一种结构示意图。其中图6(m)是螺旋磁场的结构示意图,螺旋形磁场由螺旋形永磁体22产生,磁体上的每一点磁化方向23均沿径向,螺旋形永磁体22与支撑构架24组成一个套筒形结构与套筒形连接板16连接。图6(m)所示的螺旋形永磁体22可以作为图4和图5所示的磁驱动器中的永磁体。图6(m)也示出了磁场的旋转方向25。其工作原理如图6(n)和图6(o)所示,这里可有两种工作方式:一种是单独采用图6(n)或图6(o)所示的工作状态,流速场周向和轴向的速度分量可分别表示为(Vφ,Vz),(-Vφ,-Vz),流场不随时间变化;第二种为在时间T内螺旋形磁场作逆时针旋转(图6(n))或顺时针旋转(图6(o)),相应地,在时间(P-T)内螺旋磁场作顺时针旋转(图6(o))或逆时针旋转(图6(n)),螺旋形永磁体22在驱动流体的驱动下旋转,在导电液体1中产生相应的三维螺旋结构的流动,流动方向9分别在图6(n)和图6(o)中示出,可见这种结构的磁驱动器将在导电液体1中产生时间和空间上周期性变化的电磁力场。FIG. 6 is a schematic structural view of the permanent magnet in the magnetic driver shown in FIG. 4 and FIG. 5 above. Figure 6(m) is a schematic diagram of the structure of the spiral magnetic field. The spiral magnetic field is generated by the spiral
图7是上述图4和图5中所示的磁驱动器中永磁体的另一种结构示意图。其中图7(p)是一种传统的八单元组成的磁魔环结构的磁场26的示意图,永磁体上的箭头表示该磁体单元的磁化方向23,在垂直轴线的中心截面上磁场分布均匀,在轴线上磁场呈高斯分布,即在轴向上随着离开磁体的距离增加,磁场迅速衰减。轴向上电磁场强度的分布可通过磁魔环的高度来调节,这样的设计对在导电液体中产生较高的电磁力密度梯度场是很有利的。图7(p)所示的磁魔环结构的永磁体25可以作为图4和图5所示的磁驱动器中的永磁体。图7(q)和图7(r)是磁魔环结构的永磁体在本发明中的工作原理图。图7(p)也示出了磁场的旋转方向25。其工作原理如图7(q)和图7(r)所示,也有两种工作方式:一种是单独采用图7(q)或图7(r);第二种是在时间T内螺旋形磁场作逆时针旋转(图7(q))或顺时针旋转(图7(r)),相应地,在时间(P-T)内螺旋磁场作顺时针旋转(图7(r))或逆时针旋转(图7(q)),磁魔环结构的永磁体25在驱动流体的驱动下旋转,在导电液体1中产生相应的三维纺锤形结构的流动,流动方向9分别在图7(q)和图7(r)中示出。FIG. 7 is another schematic structural view of the permanent magnet in the magnetic actuator shown in FIGS. 4 and 5 above. Wherein Fig. 7 (p) is the schematic diagram of the
需要指出的是,以上是通过举例来说明通过特定的磁场设计在本发明的磁驱动器作用下在导电液体1中产生空间变化的电磁力场,因此不限于采用其它可产生空间变化电磁力场的磁场结构。It should be pointed out that the above is an example to illustrate that a spatially varying electromagnetic force field is generated in the
根据本发明方法第五种方案设计的磁驱动器的结构如图8所示,该方法包括以下步骤:The structure of the magnetic driver designed according to the fifth scheme of the method of the present invention is as shown in Figure 8, and the method comprises the following steps:
(1)在导电液体1中形成第一圆柱形腔体27和第二圆柱形腔体28,第一圆柱形腔体27上分别设有驱动流体的第九通道口29和第十通道口30,第二圆柱形腔体28上分别设有驱动流体的第十一通道口31和第十二通道口32;(1) The first
(2)分别将涡轮叶片5置于第一圆柱形腔体27和第二圆柱形腔体28中,涡轮叶片5安装在轴承6上,轴承6与圆柱形腔体27,28同轴安装;(2) Place the
(3)将永磁体7分别与涡轮叶片5相对固定;(3) Fixing the
(4)使驱动流体以周期P或P’分别从第一圆柱形腔体27的第九通道口29或第十通道口30以及第二圆柱形腔体28上的第十一通道口31或第十二通道口32进入或流出,驱动流体驱动涡轮叶片5以周期P或P’作正向或反向转动,并带动永磁体产生方向作周期性变化(周期为P或P’)的旋转磁场,在两个圆柱形腔体27,28外部周围的导电液体1内产生涡电流,旋转磁场与涡电流相互作用产生时空变化(周期为P或P’)的电磁力场,驱动或搅拌导电液体1。(4) Let the driving fluid flow from the
图8(s)和图8(t)示出了两个磁驱动器作并列布置的情形,通过第九通道口29、第十通道口30、第十一通道口31、第十二通道口32驱动流体流动方向的设置,可实现两个磁驱动器的旋转方向相反,即其中一个为逆(顺)时针方向旋转,另一个则为顺(逆)时针方向旋转,且按照一定的周期P作周期性变化。在这种结构中,根据磁极同性相斥,异性相吸的原理,在并列布置的两个磁驱动器之间建立起关联的磁场,在此关联磁场的作用下,导电液体的流动方向9如图中所示,在导电液体1中形成周期性流动。Fig. 8 (s) and Fig. 8 (t) have shown the situation that two magnetic drivers are arranged side by side, through the
图9(u)和图9(v)所示,通过第九通道口29、第十通道口30、第十一通道口31、第十二通道口32驱动流体流动方向的设置,可实现两个磁驱动器的旋转方向相同,即其中一个为逆(顺)时针方向旋转,相应地,另一个则为逆(顺)时针方向旋转,且按照一定的周期P作周期性变化。为了在导电液体中产生较高的电磁力密度梯度场,两个磁驱动器的旋转方向设为相同,在两个磁驱动器之间的导电液体中形成具有周期性且具有较高的电磁力密度梯度场,进而在导电液体内产生具有较大梯度的流速场。As shown in Figure 9(u) and Figure 9(v), through the setting of the
此外,本发明方法中,由于驱动流体的流量与所驱动的导电液体受到的电磁力有一定的函数关系,一般地,驱动流体的流量越大,所获得的电磁力也越大(电磁力未达到饱和状态)。因此,还可以通过调节驱动流体的流量,在导电液体中获得实际应用需要的电磁力场。In addition, in the method of the present invention, since the flow rate of the driving fluid has a certain functional relationship with the electromagnetic force received by the driven conductive liquid, generally, the greater the flow rate of the driving fluid, the greater the electromagnetic force obtained (the electromagnetic force has not reached saturation state). Therefore, the electromagnetic force field required for practical applications can also be obtained in the conductive liquid by adjusting the flow rate of the driving fluid.
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CN101578448A (en) * | 2007-01-04 | 2009-11-11 | 新展电业有限公司 | Tidal electricity generating apparatus |
US20100320771A1 (en) * | 2007-11-16 | 2010-12-23 | Michael John Urch | Power Generator |
US20110115231A1 (en) * | 2009-11-12 | 2011-05-19 | Nostrum Energy Pte. Ltd. | Hydrokinetic energy conversion system |
CN102146883A (en) * | 2010-02-09 | 2011-08-10 | 李希南 | High-power magnetic fluid power generator system for wind power generation |
CN102261300A (en) * | 2011-03-30 | 2011-11-30 | 张青 | Device for acquiring liquid vortex power |
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2012
- 2012-04-28 CN CN2012101350499A patent/CN102664511B/en not_active Expired - Fee Related
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
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CN101578448A (en) * | 2007-01-04 | 2009-11-11 | 新展电业有限公司 | Tidal electricity generating apparatus |
US20100320771A1 (en) * | 2007-11-16 | 2010-12-23 | Michael John Urch | Power Generator |
US20110115231A1 (en) * | 2009-11-12 | 2011-05-19 | Nostrum Energy Pte. Ltd. | Hydrokinetic energy conversion system |
CN102146883A (en) * | 2010-02-09 | 2011-08-10 | 李希南 | High-power magnetic fluid power generator system for wind power generation |
CN102261300A (en) * | 2011-03-30 | 2011-11-30 | 张青 | Device for acquiring liquid vortex power |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
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CN102980415A (en) * | 2012-11-20 | 2013-03-20 | 中国科学院研究生院 | Method for driving periodic flow of metal melt on basis of spiral magnetic field of electrified coil |
CN104467357A (en) * | 2013-09-15 | 2015-03-25 | 波音公司 | Ferrofluid motor |
EP2849322A3 (en) * | 2013-09-15 | 2015-11-25 | The Boeing Company | Ferrofluid motor |
US9543818B2 (en) | 2013-09-15 | 2017-01-10 | The Boeing Company | Ferrofluid motor |
CN107024118A (en) * | 2015-11-05 | 2017-08-08 | 高桥谦三 | Liquation delivery pump and liquation induction system |
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