Brief Description of the Drawings Fig. 1 presents magnetic core test data showing how the volt-amp reactance power required to set up a constant magnetic flux action in an air gap, as assured by constant a. c. voltage excitation of a magnetizing winding, falls short of the associated power of the potential implicit in the […]

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Page 14 – Dealing with Rotor Induced Counter (Back) EMF – Update/March/2012 Final On the pages 12 and 13, I used Leds in the circuit to give visual indications of current flows. In the following experiments, the Leds are discarded in the CEMF circuit path. Without the 1.8 volt drop across the Leds, more current flows […]

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Page 13 – Dealing with Rotor Induced Counter (Back) EMF – Update/March/2012 Continued The following experiment is intended to give visual confirmation that the BEMF and CEMF current paths take the routes shown on Page 12- Fig1, and are two separate forces that emerge independently, taking different paths in the circuit. In the photos presented below, […]

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Page 12 – Dealing with Rotor Induced Counter (Back) EMF – Update/March/2012 Recently, as I was going through some storage boxes, I came upon an old rotor and some air coil assemblies which had been destined for the junk heap years ago, but which somehow managed to escape their appointed fate. The rotor is bent and […]

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Page 11 : A simple explanation for an apparent accelerative anomoly ! Or "why acceleration occurs when a passive generating output coil in an open magnetic system is short circuited or placed under a higher than nominal load". This explanation is drawn from conventional electronics and focuses on the impedance characteristics of a coil wound on […]

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Page 10 : An Experiment in Bending "Lenz's Law" This is a simple and straighforward experiment, but because of the high torque and speeds involved, YOU will have to build an alternator And for YOUR safety, YOUR rotor, bearings, framework and axle should be made as precisely and well balanced as possible. The materials you choose […]

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Page 9 : Controlling Duty Cycle and the advantage of using Optical Switching versus Hall Switching When Robert Adams first introduced his motor to the world he also introduced a very unique but simple switch in the form of a metal star shape embedded in a disk. It was a mechanical switching system, which he later […]

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Page 8 : Pick-up Coils and Bending Lenz's Law Please don't take a single word I have to say on this page as explicit "truth ". PLEASE reproduce your own motor/generator experiments as outlined on this page. Please Verify Effects For Yourself!!! Hopefully you've already digested some of the complicated stuff, and in keeping with the KISS […]

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Page 7 : Cores and Coils – Continued On page 6 we looked at how using bi-filar coils can minimize current demand and slightly increase torque. On this page we'll look at a few circuits that off-load their regenerative energy to a secondary battery or capacitor. We will discuss using the secondary winding of the bi […]

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To bi or not to bi, that is the question Horatio! Bi-Filar that is. Do you wind single or double (bi-filar) coils for your motor. Its six of one or a half a dozen of the other! Once again, it depends on your requirement. But I'll assume that you want to wind bi-filar, because you've […]

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Page 5 : Cores and Coils – Continued On this page we begin to discuss coil arrangements and magnetic properties. This will eventually lead us to rotor design; since how or what you want your motor to do will dictate the design of your rotor as well. In Fig 13 below we'll look at various coil […]

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Page 4 : Cores and Coils Before continuing with any more circuits, lets examine the coil. After all, without the coil, there is no "motor " in a pulsed coil motor! And "In short", there is also NO "In Short", when it comes to talking about coil design. Especially when we are talking about pulsed motors, […]

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Page 3 : Simple Circuits – Continued On this page, we finally get to collecting CEMF from the drive coil. Fig 7 below introduces a more sophisicated controlling circuit utilizing a Voltage Regulator and Mosfets to do the switching. The circuit also introduces a CEMF output and two different paths in which it can be connected. […]

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Page 2 : Simple Circuits – Continued First I need to explain some things about Back EMP (BEMP) and Back Emf (BEMF). BEMP is Back Electromotive Potential while BEMF is Back Electromotive Force. What's the difference? Force is a measure of mass x acceleration. This implies that a movement of mass is an integral part of […]

simple Adams motor concept 亚当斯电机原理01

Page 1 : Simple Circuits These first simplified circuits are here to show and explain some fundamentals pertaining to Hall IC's, Transistors and the reactive characteristics of Induction coils in pulsed motor systems. In particular, they are designed to show a couple of simple steps that can be taken to prevent components from "blowing" due to […]


       POD包含一个环形磁铁组,大约2-3英寸长,基于1英寸直径的磁铁。双线圈层在磁铁组外边,彼此绝缘。线圈的方向不重要。第三个线圈在POD中心磁芯上,连接后当脉冲时,磁芯消磁。这是重点。一个END磁铁和磁铁组磁性相反,气隙1mm。系统被脉冲,以至于POD磁芯反复消磁,近似于亚当斯电机机械地消磁循环。        POD磁芯后面的基本观点是,磁铁组上的双线圈提供额外的势能到消磁循环,能量因此从磁铁组持续提取出来。磁铁组试图抵消这个不平衡,反过来消耗来自END磁铁的能量。因此END磁铁结束显现出来的同一异常“寄存器”性质,就像亚当斯电机显现的。


        当在寄存器,我推测转子磁铁提供“free precharge”到电机电路。永磁场减少了需要的消磁的电能输入。因此需要较少的电能消磁,比我们从接近时得到的动能总和。   很明显基础物理获得很好的判断。磁铁被机械的强迫进入自相矛盾的饱和,在定子区衰退时,需要较小的电能输入,比接近时获得动能。在那样的情况下,假设一些东西异常不是没有理由的,没有登记在主流科学文献,但可能确实发生。       我提前解释这个异常的前提是,开关闭合的瞬间,势能从永磁中释放,一个主要的异常通量效应呈现出来,结合永磁的中央磁极面。磁铁异常显然耦合定子输入电流,赐予它传奇的性质,输入电流减少,输入电压上升,一个反向电流直接返回到原电源在开关打开后。   这些是我推测的一般特性,与相耦合相关。那是与输入电子流反向的时间极性。电流消耗的一半,可能两个时间极性同时呈现的一个结果,磁通和场密度变化率双倍效应,一个是物理电子,另外一个异常的耦合通量矢量。吸收环境能代替传统的向外辐射能量。能量反向流动到电源。虽然不是一个真正的相位共轭波,这个推测混合了共轭波理论是我最好的尝试使这个现象言之有理。   后来的固态实验用POD消磁,建议当在寄存器,电磁脉冲几何看起来像下面。这个主要的电磁“闪耀”是机械的偏向寄存器和定子消磁循环的结果,是亚当斯奇异性能的重要体现,电流消耗减少,电压上升,BEMF猛增。   当在寄存器,我推测转子磁铁提供“free precharge”到电机电路。永磁场减少了需要的消磁的电能输入。因此需要较少的电能消磁,比我们从接近时得到的动能总和。 很明显基础物理获得很好的判断。磁铁被机械的强迫进入自相矛盾的饱和,在定子区衰退时,需要较小的电能输入,比接近时获得动能。在那样的情况下,假设一些东西异常不是没有理由的,没有登记在主流科学文献,但可能确实发生。  


亚当斯电机基础原理 亚当斯电机的理论相对复杂,这份文档的目的是建立一个框架让一个人可以开始分析,没别的。最好的变量组合实在太多了,对临时实验者获得最好结果,机械转子呈现了很多控制问题。因为进一步的变量超过了下面讨论的,这份文档仅能作为研究亚当斯电机的入门指导。焦点是解释怎么呈现寄存器中通量异常,而不是优化这个异常本身。 背景 第一个尝试亚当斯电机理论的人是哈罗德阿斯普登。他的观点保存在他的专利中,在这份文档的最后完整呈现。基本观点是亚当斯电机属于开关磁阻电机。也就是说磁铁偏离寄存器,定子被脉冲,磁芯实际上消磁,以便转子能自由旋转过定子区。有争论的OU效应是基于磁芯的一个效应,与超过材料本身磁饱和点的操作有关。 虽然聪明绝顶,必须说的是这些观点仅是理论上的,哈罗德阿斯普登开发的电机遭受低速。这符合磁芯饱和。我不关心任何磁芯饱和在实际工程中的优势。所以我提出了解释电机的代替理论,当转子磁铁被吸向定子磁芯时,声称寄存器异常的根据,不是运行在超出磁芯正常饱和,而是在定子上有一个发电线圈,亚当斯每次都说的神秘4:1(但是从没有在任何图纸中显示)

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