| 序号 | 专利名 | 申请号 | 申请日 | 公开（公告）号 | 公开（公告）日 | 发明人 |
|---|---|---|---|---|---|---|
| 1 | 一种超导阵列驱动装置、超低频超导电压源和控制方法 | CN201611138809.6 | 2016-12-12 | CN106533118A | 2017-03-22 | 康焱 |
| 本申请公开了一种超导阵列驱动装置、超低频超导电压源和控制方法，提高超导阵列驱动能力和超低频电压输出准确度。驱动装置包括控制单元、恒流源组；恒流源组产生多路驱动电流；控制单元控制恒流源组输出驱动电流。超低频超导电压源，包含超导阵列和超导阵列驱动装置，超导阵列包含多个超导结阵；超导结阵进一步包含一个或多个超导单元；超导单元相互串联，每一个超导结阵输入一路驱动电流、产生一个量子电压；超导结阵中串联的超导单元数为2的N次幂。超低频超导电压源控制方法，周期性地按照多个离散时间点控制恒流源组输出的驱动电流变化，使超导阵列中的各个超导结阵分别按照所述离散时间点输出预定量值的量子电压，合成超低频正弦波形。 | ||||||
| 2 | 移动磁场产生装置 | CN201110301962.7 | 2011-09-28 | CN102437710B | 2015-05-20 | 杉田聪; 三泽康司; 唐玉琪; 宫入茂德 |
| 本发明提供一种能够使移动磁场的移动速度比以往快的移动磁场产生装置。该移动磁场产生装置具有由以N极和S极成列交替排列的方式且以第一间距配置的多个磁铁(3)构成的磁铁列(5)。该移动磁场产生装置具备第一及第二磁极片列(7及9)，它们与磁铁列(5)之间隔开间隔，将磁铁列(5)夹在之间，并且沿磁铁列(5)延伸且在相互间以规定的相位差配置。第一磁极片列(7)通过多个具有与磁铁列(5)的至少相邻的两个磁铁对置的长度的第一磁极片(8)以第二间距且以成列的方式配置而构成。第二磁极片列(9)也与第一磁极片列(7)同样地构成。使第一及第二磁极片列(7及9)以及磁铁列(5)的一方相对于另一方以规定的相对速度移动。 | ||||||
| 3 | 气体内能发电机 | CN200510011095.8 | 2005-10-31 | CN1866721A | 2006-11-22 | 张永志 |
| 一种将燃料燃烧产生的热能直接转换成电能的发电机。名称为气体内能发电机，它是由处于一旋转运动磁场中的燃烧室连通磁场外的增压通道组成发电机的主要部件。负极板与正极板分别平行设置于燃烧室和增压通道的两端，正极板设计为栅网式利于废气排出，负极导线需经磁屏障管中输出磁场外。 | ||||||
| 4 | 用于控制熔融金属流动的方法 | CN200910164432.5 | 2002-12-10 | CN101628333B | 2010-12-08 | 瓦莱丽·G·卡根 |
| 一种借助于泵送、制动或扼流精确地、迅速地控制熔融金属流动进入金属铸造机的方法。在一个单向磁场内使用了电流的法拉第-安培原理。永久磁铁含有钕或类似的高能稀土材料，以提供“伸出”磁性。这些钕磁铁通常示出为立方体，排列为大功率形状，以驱动强烈的单向磁场B跨越一个非磁性间隙，比商业上供应的其它磁铁强许多倍。此间隙容纳一个管路，用于增压和移动一个熔融金属流动。在制造多数相同的铸件时，一个控制的、间断的、预定的熔融金属流动供给至一系列相同的单独的铸模。本发明排除了对于冶金炉操作冶金活门或昂贵的倾斜机构的需要。现有的炉子作为借助重力流动是太低，但借助本发明的实施例可以改造为可使用的。 | ||||||
| 5 | 电磁泵送、制动和计量熔融金属供给进入金属铸造机用的具有伸出磁场的永久磁铁的使用方法 | CN02827673.6 | 2002-12-10 | CN1918307B | 2010-06-16 | 瓦莱丽·G·卡根 |
| 一种借助于泵送、制动或扼流精确地、迅速地控制熔融金属流动进入金属铸造机的方法。在一个单向磁场内使用了电流的法拉第-安培原理。永久磁铁含有钕或类似的高能稀土材料，以提供“伸出”磁性。这些钕磁铁通常示出为立方体，排列为大功率形状，以驱动强烈的单向磁场B跨越一个非磁性间隙，比商业上供应的其它磁铁强许多倍。此间隙容纳一个管路，用于增压和移动一个熔融金属流动。在制造多数相同的铸件时，一个控制的、间断的、预定的熔融金属流动供给至一系列相同的单独的铸模。本发明排除了对于冶金炉操作冶金活门或昂贵的倾斜机构的需要。现有的炉子作为借助重力流动是太低，但借助本发明的实施例可以改造为可使用的。 | ||||||
| 6 | 流体机械和运行流体机械的方法 | CN200380108740.7 | 2003-12-17 | CN1739229A | 2006-02-22 | 德特莱夫·哈杰; 赫尔穆特·波拉克 |
| 本发明涉及一种流体机械(1)，其包括转子(3)和定子(5)，其中构成一个用于一工作流体(A)的流动通道(7)，所述转子(3)可被该工作流体(A)驱动。此流体机械(1)有一块用于在流动通道(7)内产生可预定的磁场(B)的磁铁(9)。本发明还涉及一种运行一流体机械(1)的方法，该流体机械包括一转子(3)和一定子(5)以及一流动通道(7)，在此方法中，该流动通道(7)被一种含离子的工作流体(A)流过以及在该流动通道(7)内产生一规定的磁场(B)，其中，离子(27)在磁场(B)内偏转。 | ||||||
| 7 | 液态金属发电装置和液态金属发电跑步机 | CN201710107465.0 | 2017-02-27 | CN106877625A | 2017-06-20 | 张旭东; 刘静 |
| 本发明涉及健身器材技术领域，提供了一种液态金属发电装置和液态金属发电跑步机。该装置包括第一永磁铁、第二永磁铁、第一电极、第二电极、转轮以及充有液态金属的环形柔性管道，转轮用于挤压环形柔性管道并驱动液态金属流动，第一永磁铁和第二永磁铁相对设置在环形柔性管道的外侧、且关于环形柔性管道的轴线或轴线的切线方向对称，第一电极和第二电极的第一端分别插设在位于磁场中的环形柔性管道的两侧壁中，液态金属的流动方向、磁场方向以及第一电极和第二电极之间的电流方向两两垂直。该跑步机包括上述液态金属发电装置。本发明噪音小、结构简单、便于安装，通过液态金属切割磁感线产生电流，有效利用了健身运动所产生的能量，节约了电能。 | ||||||
| 8 | 移动磁场产生装置 | CN201110301962.7 | 2011-09-28 | CN102437710A | 2012-05-02 | 杉田聪; 三泽康司; 唐玉琪; 宫入茂德 |
| 本发明提供一种能够使移动磁场的移动速度比以往快的移动磁场产生装置。该移动磁场产生装置具有由以N极和S极成列交替排列的方式且以第一间距配置的多个磁铁(3)构成的磁铁列(5)。该移动磁场产生装置具备第一及第二磁极片列(7及9)，它们与磁铁列(5)之间隔开间隔，将磁铁列(5)夹在之间，并且沿磁铁列(5)延伸且在相互间以规定的相位差配置。第一磁极片列(7)通过多个具有与磁铁列(5)的至少相邻的两个磁铁对置的长度的第一磁极片(8)以第二间距且以成列的方式配置而构成。第二磁极片列(9)也与第一磁极片列(7)同样地构成。使第一及第二磁极片列(7及9)以及磁铁列(5)的一方相对于另一方以规定的相对速度移动。 | ||||||
| 9 | 用于控制熔融金属流动的方法 | CN200910164432.5 | 2002-12-10 | CN101628333A | 2010-01-20 | 瓦莱丽·G·卡根 |
| 一种借助于泵送、制动或扼流精确地、迅速地控制熔融金属流动进入金属铸造机的方法。在一个单向磁场内使用了电流的法拉第—安培原理。永久磁铁含有钕或类似的高能稀土材料，以提供“伸出”磁性。这些钕磁铁通常示出为立方体，排列为大功率形状，以驱动强烈的单向磁场B跨越一个非磁性间隙，比商业上供应的其它磁铁强许多倍。此间隙容纳一个管路，用于增压和移动一个熔融金属流动。在制造多数相同的铸件时，一个控制的、间断的、预定的熔融金属流动供给至一系列相同的单独的铸模。本发明排除了对于冶金炉操作冶金活门或昂贵的倾斜机构的需要。现有的炉子作为借助重力流动是太低，但借助本发明的实施例可以改造为可使用的。 | ||||||
| 10 | 电磁泵送、制动和计量熔融金属供给进入金属铸造机用的具有伸出磁场的永久磁铁的使用方法 | CN02827673.6 | 2002-12-10 | CN1918307A | 2007-02-21 | 瓦莱丽·G·卡根 |
| 一种借助于泵送、制动或扼流精确地、迅速地控制熔融金属流动进入金属铸造机的方法。在一个单向磁场内使用了电流的法拉第—安培原理。永久磁铁含有钕或类似的高能稀土材料，以提供“伸出”磁性。这些钕磁铁通常示出为立方体，排列为大功率形状，以驱动强烈的单向磁场B跨越一个非磁性间隙，比商业上供应的其它磁铁强许多倍。此间隙容纳一个管路，用于增压和移动一个熔融金属流动。在制造多数相同的铸件时，一个控制的、间断的、预定的熔融金属流动供给至一系列相同的单独的铸模。本发明排除了对于冶金炉操作冶金活门或昂贵的倾斜机构的需要。现有的炉子作为借助重力流动是太低，但借助本发明的实施例可以改造为可使用的。 | ||||||
| 11 | Feed mechanism for rosar transponder including transmitting-receiving antenna for rosar device | JP2001399482 | 2001-12-28 | JP2003149334A | 2003-05-21 | KLAUSING HELMUT; KALTSCHMIDT HORST |
| PROBLEM TO BE SOLVED: To solve the problem of maintenance cost, weight and unbalance due to electric power supply for a transponder being based on aerodynamic energy. SOLUTION: In this ROSAR feed mechanism for a transmitting-receiving antenna built in a tip part of a rotor blade of a helicopter, piezoelectric or electrodynamic conversion from wind energy to electric energy is performed by a pair of miniature turbine generators built in one or two or more flat passages passing in a transponder card, or a ribbon making vibrating motion in these passages. COPYRIGHT: (C)2003,JPO | ||||||
| 12 | Pump assembly | JP18649087 | 1987-07-24 | JPH0797148B2 | 1995-10-18 | ロバート・マイケル・セレピアン |
| A pump assembly (18) is disclosed for transferring the internal energy from a second or intermediate liquid metal to a first or primary liquid metal. The pump assembly comprises a pump duct (72) for receiving the first liquid metal and a primary generator duct (70) for receiving a first flow of the pumped, intermediate liquid metal. A first or main (76) means in the illustrative form of a plurality of field coils generates and applies a main magnetic field through the pump and the primary generator ducts, whereby a first current flow is established through the pump and primary generator ducts and the primary liquid metal is pumped. An auxiliary generator duct (102) receives a second flow of the pumped, intermediate liquid metal. An auxiliary means (96), illustratively in the form of permanent magnets, generates an auxiliary magnetic field through the auxiliary generator duct, whereby the interaction of the auxiliary magnetic field and the second flow of the pumped, intermediate liquid metal generates a second current flow to excite the field coils. | ||||||
| 13 | Magnetic fluid turbo device | JP25206190 | 1990-09-25 | JPH03128659A | 1991-05-31 | UIRIAMU FURANSHISU HANAN ZA SA |
| PURPOSE: To increase an output voltage by forming a proper electrode surface at the outer-periphery and inner-periphery parts of a device and performing liquid contact. CONSTITUTION: A current J in a radial direction, flowing in a fluid 48, generates acceleration in a peripheral direction at the flow of the fluid 48 in a left annular channel 34, in the presence of a magnetic field B in a side direction. When the fluid 48 flows from a point A to a point B, a large amount of pressure is generated in the flow of the fluid 48. After that, the fluid 48 passes through an outside turbine blade 46 and moves from the point B to a point C, thus causing a change in liquid momentum to generate a torque in a disk 32. Although the fluid 48 at the point C moves relatively slowly, pressure is large. By guiding the flow of the fluid 48 to a right annular channel 36, the fluid 48 generates a controlled turn and hence a high-voltage energy is speedily and effectively converted at a point D. COPYRIGHT: (C)1991,JPO | ||||||
| 14 | Ring-shaped flow coupler | JP19979087 | 1987-08-12 | JPS6447264A | 1989-02-21 | AOYAMA GORO; KAWABE RYUHEI; IKEDA TAKASHI; GOTO TADASHI |
| PURPOSE:To relieve the stress and to improve efficiency by dividing an insulating material into a plurality of pieces. CONSTITUTION:A ring-shaped clearance formed between a coaxial cylindrical inner pipe 1 and an outer pipe 2 is divided into a generator side flow path 5 and a pump side flow path 6 by means of a conductive flow path pipe 3. And, the insulating materials 4 are placed to the outside of the inner pipe 1 and the inside of the outer pipe 2. In addition, they are fixed to the conductive flow path pipe 3 and slight clearances 13 are kept without coming into contact with the inner pipe 1 and the outer pipe 2. And, both the generator side flow path 5 and the pump side flow path 6 divided the insulating materials 4 at the center part of a flow path in the circumferential direction. Accordingly, a ring-shaped electromagnetic flow coupler reduces its electric potential to zero at the center part of the flow path in case the dimensions of the flow path are uniformalized circumferentially, and even if the insulating materials are divided circumferenctially by putting a slit 7 axially, the current is not leaked to a side-wall. | ||||||
| 15 | Pump aggregate | JP18649087 | 1987-07-24 | JPS63101795A | 1988-05-06 | ROBAATO MAIKERU SEREPIAN |
| A pump assembly (18) is disclosed for transferring the internal energy from a second or intermediate liquid metal to a first or primary liquid metal. The pump assembly comprises a pump duct (72) for receiving the first liquid metal and a primary generator duct (70) for receiving a first flow of the pumped, intermediate liquid metal. A first or main (76) means in the illustrative form of a plurality of field coils generates and applies a main magnetic field through the pump and the primary generator ducts, whereby a first current flow is established through the pump and primary generator ducts and the primary liquid metal is pumped. An auxiliary generator duct (102) receives a second flow of the pumped, intermediate liquid metal. An auxiliary means (96), illustratively in the form of permanent magnets, generates an auxiliary magnetic field through the auxiliary generator duct, whereby the interaction of the auxiliary magnetic field and the second flow of the pumped, intermediate liquid metal generates a second current flow to excite the field coils. | ||||||
| 16 | Actuator using magnetic fluid | JP5443184 | 1984-03-23 | JPS60200758A | 1985-10-11 | KADOTA OTOMATSU |
| PURPOSE:To obtain a ready, accurate and compact actuator by filling magnetic fluid through two cylinders which respectively contain pistons, and moving the pistons by electromagnetic forces. CONSTITUTION:An acutuator has cylinders 1, 2, pistons 3, 4 slidably contained respectively in the cylinders, a piston rod 5, magnetic fluid 6 filled between the pistons 3 and 4, and control coils 7, 8 for controlling the flow of the fluid 6. A current is flowed from a power source 9 by a current controller 10 in the coils 7, 8. Thus, the fluid 6 is attracted by one energized coils 7, 8 to move in the cylinders 1, 2, thereby moving the pistons 3, 4. | ||||||
| 17 | Magnetic fluid pump | JP20100183 | 1983-10-28 | JPS6096172A | 1985-05-29 | IKEGUCHI TAKASHI; KAWAIKE KAZUHIKO; NODA MASAMI; ITOU MOTOYA |
| PURPOSE:To obtain a pump which may not damage due to wear and tear and has excellent durability and reliability by circulating magnetic fluid by energizing an electromagnet and transporting the liquid by the pumping action of the magnetic fluid. CONSTITUTION:Magnetic fluids 3', 3'' in a tube 1 move in a direction of a branch port B of downstream side and liquid 10 is pumped and transported by the movement of the fluids, but when the fluids 3'' arrives at the port B, the energization of an electromagnet 4 is stopped, and an electromagnet 7 is, on the contrary, energized. Then, the fluid 3'' which is arrived at the port B is pushed into a bypass tube 2, and fluid 3 is, on the contrary, pushed out into the tube 1 newly from a branch port A of upstream side. Since the solvent of the fluid 3 is nonsoluble in the liquid 10, the fluid 3 is not dissolved in the liquid 10 nor mixed. Thus, mechanical slidable part can be eliminated to eliminate the possibility of damage due to wear and tear. | ||||||
| 18 | Pumping device | JP4302382 | 1982-03-19 | JPS57166876A | 1982-10-14 | UORUTAA GAI ROMAN |
| 19 | HIGH VOLUME AIR/GAS/FLUID FLOW POWERED TORUS SHAPED ELECTRIC GENERATOR | EP16020274.3 | 2016-07-18 | EP3273582A1 | 2018-01-24 | Parlatos, Stelios |
A high volume air, gas or fluid flow powered torus electric generator includes a hollow torus shaped housing 10, an insulated copper coil winding 13, an entrance point 11 and an exit point 12 for the flow, a sphere shaped permanent magnet 14 and the terminals of the copper coil windings 16, 17. Thus, flow can be used to produce electricity just by forcing the magnetic sphere to revolve inside the hollow torus shaped housing and thus through the coil. This generator can convert kinetic energy from the flow into electric energy and vice versa in a simple and not much demanding way. |
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| 20 | Systems and methods for plasma propulsion | EP06250099.6 | 2006-01-10 | EP1681465B1 | 2012-08-08 | Allen, Edward H. |
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