In the present paper the results of the experimental research of magnetic-gravity effects are presented. Anomalous magnetic and thermal changes within a radius of 15 meters from the researched device were measured as well. PACS: 41.20.-q; 44.60.+k; 76.50.+q 

　　1. Introduction 

　　There has been a great interest in examining non-linear effects in the system of rotating magnetic fields. Such effects have been observed in the device called Searl's generator or Searl Effect Generator (SEG) [1-4]. A SEG consists of a series of three concentric rings and rollers that circulate around the rings. All parts of SEG are based on the Law of the Squares [5]. The rollers revolve around the concentric rings, but they do not touch them. There's a primary north-pole and primary south pole on the rollers and a primary north-pole and primary south-pole on the concentric rings. Obviously, the north-pole of the roller is attracted to the south-pole of the concentric rings and vice versa. 

　　The rollers have a layered structure similar to the concentric rings. The external layer is titanium, then iron, nylon and the last internal layer was made from neodymium. John R.R. Searl has supposed that electrons are given off from the central element (neodymium) and travel out through other elements. Dr. Searl contends that if nylon had not been used, the SEG would act like a laser and one pulse would go out and it would stop, build up, and another pulse would go out. The nylon acts as a control gate that yields an even flow of electrons throughout the SEG [4]. 

　　In [4] it was shown that in the process of magnetization of the plate and rollers, the combination of constant and variable magnetic fields for creating a special wave (sine wave) pattern on a plate surface and rollers surface was used. The basic effects consist of the rollers self-running around the ring plate with a concurrent reduction of weight and an increasing occurrence of propulsion. These effects come about because of a special geometry of experimental setup. It was shown that the operation of the device in the critical regime is accompanied by biological and real physical phenomena. 

　　Other information where similar effects are be mentioned can be found in the books, Unconventional Flying Objects [6] and the Homopolar Handbook [7] which includes papers on magnetized dielectrics. In this paper we present the experimental device the results we have obtained. 

　　2. Description of the Experimental Installation 

　　The basic difficulty arises in choosing the materials and maintaining the necessary pattern imprinting on the plate and roller surfaces. To simplify the technology we decided to use a one-ring design with one-ring plate (stator) and one set of rollers (rotor). It is obvious, that it was necessary to strengthen the roller rotor near the bearings and balance the rollers well. In the suggested design, air bearings were used which provided the minimum losses due to friction. 

　　From the available description [1-4] it was not clear how to build and magnetize a stator with a one-meter diameter. In order to make the stator, separate magnetized segments of rare earth magnets with a residual induction of 1T were used. The segments were magnetized in a usual way by discharging a capacitor-battery system through a coil. Afterwards, the segments were assembled and glued together in a special iron armature, which reduced magnetic energy. To manufacture the stator, 110 kg of neodymium magnets were used and 115 kg of neodymium were used to manufacture the rotor. High-frequency field magnetization was not applied. It was decided to replace an imprinting technology described in [1-5] with cross-magnetic inserts having a flux vector directed at 90 degrees to the primary magnetization vector of the stator and rollers. 

　　For the cross inserts, modified rare earth magnets with a residual magnetization of 1,2 T and coercive force a little bit greater than in a base material were used. In Fig.1 and Fig.2 the joint arrangement of stator 1 and rotor, made up of rollers 2, and a way of their mutual gearing or sprocketing by means of cross magnetic inserts 19, are shown. Between the stator and roller surfaces the air gap δ of 1-mm is maintained. 

　　No layered structure was used except a continuous copper foil of 0.8 mm thickness, which wrapped up the stator and rollers. This foil has direct electrical contact to magnets of the stator and rollers. Distance between inserts in the rollers is equal to distance between inserts on the stator. In other words, t1 = t2 in Fig.2. 

　　

　　Fig.1. Variant of one-ring converter. / Fig.2. Sprocket effect of magnetic stator and roller inserts. 

　　The ratio of parameters of the stator 1 and the rotor 2 in Fig.2 is chosen so that the relation of stator diameter D to the roller diameter d is an integer equal to or greater than 12. Choosing such ratio allowed us to achieve a "magnetic spin wave resonant mode" between elements of a working body of the device since the circumferences also maintained the same integer ratio. 

　　The elements of magnetic system were assembled in a uniform design on an aluminum platform. In Fig. 3 the general view of the platform with the one-ring converter is displayed. This platform was supplied with springs and shock absorbers with limited ability to move vertically on three supports. The system has a maximum value of displacement of about 10 mm and was measured by the induction displacement meter, 14. Thus, the instantaneous change of the platform weight was defined during the experiment in real time. Gross weight of the platform with magnetic system in the initial condition was 350 kg. 

　　The stator, 1, was mounted motionlessly, and the rollers, 2, were assembled on a mobile common separator, 3, also regarded as the rotor, connected with the basic shaft, 4, of the device. The rotary moment was transferred through this shaft. The base of the shaft was connected through a friction clutch, 5, to a starting motor, 6, which accelerated the converter up to a mode of self-sustained rotation. The electrodynamics generator, 7, was connected to the basic shaft as a main loading of the converter. Adjacent to the rotor, electromagnetic inductors, 8, with open cores, 9, were located. 

　　

　　Fig.3. The general view of the one-ring converter and platform. 

　　The magnetic rollers, 2, crossed the open cores of inductors and closed the magnetic flux circuit through electromagnetic inductors, 8, inducing an electromotive force emf in them, which acted directly on an active load, 10 (a set of inductive coils and incandescent lamps with a total power load of 1 kW). The electromagnetic inductor coils, 8, were equipped with an electrical drive, 11, on supports, 

　　12. Driven coils for smooth stabilization of the rotor’s rpm were used but the speed of the rotor could be adjusted by changing the main loading, 10. 

　　To study the influence of high voltage on the characteristics of the converter, a system for radial electrical polarization was mounted. On the periphery of the rotor ring, electrodes, 13, were set between the electromagnetic inductors, 8, having an air gap of 10 mm with the rollers, 2. The electrodes are connected to a high-voltage source; the positive potential was connected to the stator, and the negative to the polarization electrodes. The polarizing voltage was adjusted in a range of 0-20 kV. In the experiments, a constant value of 20 kV was used. 

　　In case of emergency braking, a friction disk from the ordinary car braking system was mounted on a basic shaft of the rotor. The electrodynamics generator, 7, was connected to an ordinary passive resistive load through a set of switches ensuring step connection of the load from 1 kW to 10 kW through a set of ten ordinary electric water heaters. 

　　The converter undergoing testing had in its inner core the oil friction generator of thermal energy, 15, intended for tapping a superfluous power (more than 10 kW) into the thermo-exchange contour. But since the real output power of the converter in experiment has not exceeded 7 kW, the oil friction thermal generator was not used. The electromagnetic inductors were connected to an additional load, which was set of incandescent lamps with total power 1 kW and facilitated complete stabilization of the rotor revolutions. 

　　3. Experimental results 

　　The magnetic-gravity converter was built in a laboratory room on three concrete supports at a ground level. The ceiling height the lab room was 3-meters, the common working area of the laboratory was about 100 sq. meters. Besides the presence of the iron-concrete ceiling, in the immediate proximity from the magnetic system there was a generator and electric motor, which contained some tens of kilograms of iron and could potentially deform the field's pattern. 

　　The device was initially started by the electric motor that accelerated the rotation of the rotor. The revolutions were smoothly increased up to the moment the ammeter included in a circuit of the electric motor started to show zero or a negative value of consumed current. The negative value indicated a presence of back current. This back current was detected at approximately 550 rpm. The displacement meter, 14, starts to detect the change in weight of the whole installation at 200 rpm. Afterwards, the electric motor is completely disconnected by the electromagnetic clutch and the ordinary electrodynamics generator is connected to the switchable resistive load. The rotor of the converter continues to self-accelerate and approach the critical mode of 550 rpm where the weight of the device quickly changes. 

　　

　　Fig. 4. -G, +G changes in weight of the platform vs. rpm 

　　In addition to the dependence on the speed of rotation, the weight differential depends on the generated power through the load and on the applied polarizing voltage as well. As seen in Fig.4, at the maximum output power equal to 6-7 kW, the change of weight ∆G of the whole platform (total weight is about 350 kg), reaches 35 % of the weight in an initial condition Gi. Applying a load of more than 7 kW results in a gradual decrease in rotation speed and an exit from the mode of self-generation, with the rotor coming to a complete stop subsequently. 

　　The net weight Gn of the platform can be controlled by applying high voltage to polarization ring electrodes located at a distance of 10 mm from external surfaces of the rollers. Under the high 20 kV voltage (electrodes having negative polarity) the increase of tapped power of the basic generator to more than 6 kW does not influence ∆G if the rotation speed is kept above 400 rpm. "Tightening" of this effect is observed as well as the effect of hysteresis on ∆G (a kind of "residual induction"). The experimental diagrams given on Fig.4 illustrate the +G and –G modes of the converter operations vs. rotor rpm. 

　　

　　Fig.5 Diagrams of a rotor accelerating and loading of the converter. 

　　The effect of a local change of the platform weight is reversible, relative to the direction of rotor turning, and has the same hysteresis. A clockwise rotation causes the critical mode to occur in the area of 550 rpm and the propulsion force against the direction of gravitation vector is created. Correspondingly, a counter-clockwise rotation causes the critical mode to occur the in area of 600 rpm and a force in the direction of gravitation vector is created. The difference in approach to a critical mode of 50 - 60 rpm was observed. It is necessary to mention that the most interesting region are situated above the critical area of 550 rpm, but due to of a number of circumstances the implementation of such research was not possible. It is necessary to note, that probably there are also other resonant modes appropriate to higher rpm of a rotor and to the significant levels of useful loading and weight changing. Proceeding from the theoretical assumptions, the dependence of tapped mechanical energy from the parameters of magnetic system of the converter and rpm of a rotor has a nonlinear character and the received effects are not optimum. From this point of view, the revealing of the maximal output power, of the maximal change of weight and resource of the converter represents the large practical and scientific interest. In tested sample of the converter the using of higher rpm was inadmissible because of unsufficient mechanical durability of the magnetic system, which was built from separate pieces. 

　　In Fig.5 the dependence of weight of a platform and its output power, removed into resistive loading from rpm of a rotor of the converter is explained in detail. The diagrams are constructed for a case of HV polarization ON (top diagram) and HV polarization OFF (bottom diagram). The time from the start moment of the engine up to a mode of self-generation of the converter, at the rotation of a rotor clockwise, approximately is equal 1.5 minutes. (The power of starting engine was about of 2 KW with a reduction on the shaft of the converter is equal 1/10). At achievement of a critical mode (550 rpm.), the change of gross weight of a platform already achieves +/-30% from Gi. In the point of transition to a resonant mode, the revolutions with the large acceleration has increases up to 590 rpm and weight has changes up to + /-35% from Gi. In this time an unpleasant high frequency whistling sound became audible. This place of the diagram begins at once after a critical point (inclination of a curve α1). At achievement of 590 rpm, the first stage of resistive loading in 1 kW is connected to the electrodynamics generator. The whistling sound at once stops, the revolutions are sharply reduced and ∆G also is changing. As soon as the revolutions begin to grow again, the second switchable load is connected and ro-tor's rpm are stabilized at a level of 590-595 rpm. ∆G continues to change. The increasing of switchable loading occurs by steps in 1 kW up to total power of 6 kW. All intervals in time are equal approximately of 10-30 sec. Afterwards, the short-term increasing of revolutions and then the full stabilization of a mode during of 12-15 min were observed. 

　　More than 50 launches of this converter with absolute repeatability within three months were carried out. It is necessary to note, that revolutions will grow with acceleration reflected on the Fig.5 by corners α1…α5, if the generator is not switched to the next step of loading, the rpm will continue increasing. Twice as much loading was required to return to a previous rpm mode. 

　　The above discussion concerns a mode with high voltage polarization of 20 kV "plus" on a "grounded" stator. Without the 20 kV polarization voltage (lower curve) the diagram is approximately the same, but indicates the more hard character of loading and faster change of weight of a platform due to decreasing of rpm. 

　　Other interesting effects include the work of the converter in a dark room when corona discharges are observed around the converter's rotor as a blue-pink glowing luminescence and a characteristic ozone smell. In Fig.6 the cloud of ionization covers the area of a stator and a rotor and has accordingly a toroidal form. 

　　Fig.6. Corona discharges around the converter. On the background of luminescence glowing on rollers' surfaces, we distinguished a «wave picture.» A number of more vigorous strips of discharges around the rollers were observed. These discharges were of a white-yellow color but the characteristic sound for arc discharges was not audible. На поверхностях статора и роликов не имелось никаких видимых эрозионных повреждений as well 

　　

　　as. Erosive damage induced by arc discharges were not present on any surfaces of the stator or the rollers . 

　　One more effect previously not mentioned was observed i.e. the vertical concentric magnetic "walls" around the installation. We noticed and measured the abnormal permanent magnetic field around the converter within the radius of 15 meters. For the magnetic field measurement the Russian magnetometer F4354/1 was used. Magnetometer used the Hall-effect sensor in the copper shielding. The zones of an increased intensity of a magnetic flux 0.05 T located concentrically from the center of the installation were detected. The direction of the magnetic field vector in these walls coincided with the direction of the rollers' field vector. The structure of these zones reminded us of circles on water from a thrown stone. Between these zones, this portable magnetometer did not register abnormal magnetic fields. The layers of an increased intensity are distributed practically without losses up to a distance of about 15 meters from the center of the converter and quickly decrease at the border of this zone. The thickness of each layer is about 5 - 6 cm. The border of each layer has sharp shape, the distance between layers is about 50 - 80 cm where the upper limit is seen when moving from the center of the converter. A stable picture of this field was observed as well as at a height of 6 m above the installation (on the second floor above the lab). Above the second floor, measurements were not carried out. The similar picture was observed and outside of a room of laboratory, directly in the street, on the ground. The concentric walls are strictly vertical and no had appreciable distortions. In Fig.7 the schematic arrangement of the converter in a room of laboratory and arrangement of concentric magnetic fields are shown. 

　　Fig.7. Schematic placing of the converter and pattern of magnetic fields in the lab's room. 

　　An anomalous decrease temperature in the vicinity of the converter was also found. While the common temperature background in laboratory was + 22°C (±2°C) a fall of temperature equal to 6-8°C was noticed. The same phenomenon was observed in concentric vertical magnetic walls as well as. The measurements of temperature inside the magnetic walls were carried out by an ordinary alcohol thermometer with an inertia of indication about 1.5 min. In the magnetic walls the temperature changes can even be distinctly observed by hand. When placed into this magnetic wall the hand feels very cold at once. A similar picture was observed at the height above installation, i.e. on the second floor of the laboratory as well as despite the ferro-concrete blocking of the ceiling and also on open air outside of the laboratory. 

　　Fig.8. Dependence of intensity of a magnetic field and changes of temperature vs rotor's rpm of the converter. 

　　

　　Concentric magnetic walls and the accompanying thermal effects begin to show themselves by an appreciable image beginning approximately from of 200 rpm., and linearly grow with increasing of revolutions up to a critical mode. The measurements above 600 rpm were not made because of fear of destruction of magnetic system. In Fig.8 the curve of intensity of a magnetic field in мТ and change of temperature in Celsius degrees due to rpm changing is represented. 

　　4. Discussion 

　　All the results we obtained are extremely unusual and require some theoretical explanation. Unfortunately, the interpretation of results within the framework of the conventional physical theory cannot explain all the observed phenomena besides the change of weight. It is possible to interpret the change of weight either as a local change of gravitational force or as an antigravity force repelling its own field. Direct experiment, confirming the presence of a draft force was not performed, but in any case both interpretations of the weight change do not correspond to the modern physics paradigm. A reconsideration of the standard theory of gravitation is possible if we take into consideration space-time curvature. For example, the Kerr metric usually represents the field exterior to an axially symmetric rotating body and distinguishes between positive and negative spin directions as well as forward and backward time directions [8]. An examination of the physical vacuum as a source of these phenomena may also lend itself to better interpretation since the Maxwell stress-energy tensor in the vicinity of the converter undergoes a complex evolution. 

　　From the modern physics position, electrification and luminescence of the converter's magnetic system in the near zone is not completely clear. The phenomenon of the magnetic and thermal "walls" may be connected with Alphen's magnetic-sound waves raised in near zone in magnetized plasma induced by a variable magnetic field of a rotating rotor [9]. The energy exchange between ambient air molecules and the converter may be occurring. At the present time we can not give an exact description of the interactions mechanism and transformation of energy, but without a relativistic we are completely unable to give a physically substantial theory of these phenomena. 

　　In conclusion, we emphasize that issues of the biological influence effects and especially of the variations of real time stream effects, which must be taking place in an operative zone of the converter, were not considered at all. These issues are extremely important and absolutely unexplored; though there are some mentions of J.R.R.Searl about healing action of the SEG's radiation. Our own experience allows us to make only cautious assumption that the short-term stay (dozen minutes) in a working zone of the converter with the fixed output power of 6 kW remains without observed consequences for those exposed. The present paper is only a beginning. 

　　References 

　　Schneider, Koeppl, & Ehlers. «Begegnung mit John R.R. Searl.» Raum und Ziet, #39, 1989, pp. 75-80. 

　　Sandberg, Von S. Gunnar. «Was ist dran am Searl-effect.» Raum und Ziet, #40, 1989, pp. 67-75. 

　　Schneider & Watt. «Dem Searl-effect auf der spur.» Raum und Ziet, # 42, 1989, pp.75-81; #43, pp.73-77. 

　　Thomas Jr., John A. «ANTI-GRAVITY: The Dream Made Reality.» Extraordinary Science, vol.VI, Issue 2, 1994. (Also ANTIGRAVITY: The Dream Made Reality, Direct International Science Consortium, 1993, ISBN 1-898827-99-0) 

　　Searl, Prof. John R. R., The Law of the Squares, Books 1-8, Direct International Science Consortium, 1993, ISBN 1-898827-00-1 

　　Hill, Paul R., Unconventional Flying Objects, Hampton Roads, 1995 

　　7. Valone, Thomas, The Homopolar Handbook, A Definitive Guide to N-Machine and Faraday Disk Technologies, Integrity Research Institute, 1994

　　Adler, Bazin, and Schiffer. Introduction to General Relativity, McGraw Hill, New York, 1965 

　　Landau and Lif****z. Electrodynamics of continuous media.- Moscow, Nauka, 1982. (in Russian).

google译文如下:

　　研究所的高温下，俄罗斯科学院， Izhorskaya一十九分之十三，莫斯科127412 ，俄罗斯 

　　摘要 

　　在本文件的结果，实验研究磁引力的影响提出。反常磁，热变化的半径15米的研究，测定装置以及。 PACS系统： 41.20. - Q报表; 44.60 。 +钾; 76.50 。 + q 

　　1 。导言 

　　出现了极大的兴趣研究非线性影响系统的旋转磁场。这种影响已经观察到的装置称为塞尔的发电机或塞尔效果发生器（赛格） [ 1-4 ] 。阿赛格包括一系列的三个同心圆环和辊流通的戒指。所有地区的赛格是根据法方[ 5 ] 。该辊围绕着同心圆环，但他们不碰他们。有一个小学以北极点和南极小学的辊和北部的主要极和初级东南极的同心圆环。显然，北两极的压路机是吸引到东南极的同心圆环，反之亦然。 

　　该轧辊有层状结构类似的同心圆环。外部层是二氧化钛，然后铁，尼龙和内部的最后一层是由钕。约翰率塞尔已经假定给出电子，从核心要素（钕）和旅费通过其他要素。博士塞尔说，如果尼龙尚未使用，赛格将采取行动像一个激光脉冲将一个走出去，将停止，建立，另一个脉冲将出去。尼龙作为一个控制闸门的收益率甚至电子流在整个赛格[ 4 ] 。 

　　在[ 4 ]它表明，在这一进程中的磁化强度的钢板和压路机，结合常数和可变的磁场创造一个特殊的波（正弦波）的模式板轧辊表面和表面使用。基本的影响包括辊自我运行的环板的同时减少重量和增加发生的推进。这些影响是因为特殊形状的实验装置。结果表明，手术设备的关键制度是伴随着生物和真正的物理现象。 

　　其他信息类似的影响提到中可以找到的书籍，非常规飞行物体[ 6 ]和Homopolar手册[ 7 ] ，其中包括文件磁化介质。在本文中，我们目前的实验装置的结果我们已经获得。 

　　2 。说明实验装置 

　　基本的困难在于在选择材料和保持必要的格局印记的钢板和滚轴表面。为了简化技术，我们决定使用一个环设计，一环板（定子）和一组滚筒（转子） 。很显然，这是必要加强滚子附近的转子轴承和轧辊平衡以及。在拟议的设计，空气轴承使用提供了最低限度造成的损失摩擦。 

　　从现有的描述[ 1-4 ] ，目前还不清楚如何建立和定子磁化了一米直径。为了使定子，单独的磁化阶层的稀土磁铁剩余诱导的1T使用。该段磁化在平常的方式履行电容电池系统通过一个线圈。此后，部分组装在一起，并贴在一个特殊的铁电枢，从而减少了磁能量。制造定子， 110公斤的钕磁体被用来和115公斤的钕被用来制造转子。高频领域磁化不适用。这是决定取代印迹技术介绍[ 1-5 ]跨磁插入了磁通矢量针对90度的主要载体的磁化定子和压路机。 

　　对于两岸插入，修改稀土磁铁的剩余磁化强度1,2 T和矫顽力有点大于基础材料的使用。在图1和图2的联合安排一日定子，转子，由轧辊2 ，和一种彼此间的传动装置或sprocketing的方式跨磁插入19列。之间的定子和轧辊表面的空气间隙δ 1毫米不变。 

　　没有层状结构被用来除持续铜箔的0.8毫米的厚度，这结束了定子和压路机。这铝箔直接电接触，以磁体的定子和压路机。插入之间的距离在辊等于之间的距离插入定子。换言之， T1讯号= t2图2 。 

　　1 。变的一环转换器。 / 2 。链轮的影响和定子磁辊插入。 

　　比率参数的定子1和转子2图2选择这样的关系定子直径D的轧辊直径d是整数等于或大于12 。选择这样的比例使我们能够实现“磁自旋波共振模式”要素之间的一个工作机构的设备，因为围也保持相同的整数比。 

　　要素的磁系统组装在一个统一的设计对铝的平台。在图。 3 ，一般认为该平台的一环转换器的显示方式。这个平台是提供了弹簧和减震器的能力有限垂直移动的三个支持。该系统具有最高的价值位移约10毫米，是衡量感应位移计， 14 。因此，瞬时变化的平台重量被界定在实验期间实时。总重量的平台，磁系统的初始条件为350公斤。 

　　定子， 1 ，展开motionlessly ，以及压路机， 2 ，组装移动共同分离器， 3 ，也被视为转子，连接的基本骨干， 4日，该装置。旋转的时刻被移送通过这一骨干。该基地的连接轴是通过摩擦离合器， 5日，一个起动电机， 6 ，加快转换到模式的可自我维持的轮换。发电机的电， 7日，是连接到基本骨干作为一项主要装载器。邻近转子，电磁感应， 8日，与开放的内核， 9日，位于。 

　　图3 。人们普遍认为的一环转换器和平台。 

　　磁辊， 2 ，越过开放的核心封闭电感和磁电路通过电磁感应， 8 ，诱导了电动势电动势他们，这直接采取了积极的负荷， 10 （一组感应线圈和白炽灯总用电负荷的1千瓦） 。电磁感应线圈， 8日，配备了一个电子驱动器， 11日，对支持， 

　　12 。驱动线圈顺利稳定的转子转用的速度，但转子可以调整改变的主要装货， 10 。 

　　研究影响高电压的特点转换器，系统的径向极化的电气安装。周边转子环，电极， 13日，被确定之间的电磁感应器， 8日，有一个空气间隙10毫米的压路机， 2 。电极连接到一个高电压源;的积极潜力是连接到定子，和消极的两极化电极。极化电压的调整是在一系列的0-20千伏。在实验中，不断地价值20千伏使用。 

　　在紧急情况下刹车，摩擦盘从普通汽车制动系统是安装在一个基本轴转子。发电机的电， 7日，是连接到一个普通的被动式电阻负荷通过一系列步骤确保交换机连接的负载从1千瓦到10千瓦通过一套10个普通电热水器。 

　　该转换器进行测试已在其内部核心的石油摩擦产生热能， 15日，旨在窃听多余的功率（超过10千瓦）的热交换轮廓。但是，因为真正的输出功率转换器的实验还没有超过7万千瓦，石油摩擦热发电机没有使用。电磁感应器被连接到一个额外的负载，这是一套与白炽灯总功率1千瓦，并促进全面稳定的转子革命。 

　　3 。实验结果 

　　磁重力转换器是内置在实验室室三个具体支持在地面水平。在楼底高度实验室房间3米，在共同的工作领域的实验室，约100平方米。除了在场的情况下铁的具体上限，在紧靠从磁系统有一台发电机和电动马达，其中载有几公斤的铁和可能变形领域的格局。 

　　该装置最初是由电动机，加速转动转子。在革命顺利上升到目前的电表列入电路的电动马达开始出现零增长或负价值的消耗电流。消极价值的存在表明，当前的背部。目前这回发现在大约550转。该位移计， 14日，开始检测体重变化的整个安装在200转。此后，电动马达是完全断开的电磁离合器和普通电发电机连接到开关的电阻负荷。转子的转换继续自我加速和方法的关键模式，在550转的重量装置迅速的变化。 

　　图。 4 。荷， + G体重变化的平台与转速 

　　除了依赖的速度旋转，重量差别取决于发电的负荷和应用偏光以及电压。正如图4 ，在最大输出功率相当于6-7千瓦，改变重ΔG整个平台（总重量约350公斤） ，达到35 ％的体重在游戏初始条件。应用负载超过700千瓦的结果逐渐减少转速和退出模式，自我一代，与转子来一个完整的一站式其后。 

　　净重量促性腺激素的平台可以控制采用高电压的电极极化环位于距离从10毫米外表面的滚轮。根据最高的20千伏电压（电极产生负面极性）的增加，利用权力的基本发电机超过6千瓦不会影响ΔG如果转速保持在400以上转。 “紧缩”这种效应是观察，以及滞后效应的ΔG （一种“剩余上岗” ）。实验图图给出说明+ G和荷模式的转换业务与转子转速。 

　　图图的转子加速和负载的转换器。 

　　影响了当地的变化平台重量是可逆的，相对的方向转子转动，并具有相同的滞后。顺时针方向旋转的关键原因模式将发生在该地区的550转速和推进武力的方向引力矢量创建。相应地，一个逆时针旋转的关键原因模式发生了面积为600转的力量和方向的引力矢量创建。在不同的办法，一个重要模式， 50 -6 0转观察。有必要提及的是，最有趣的区域都位于上述关键领域的550转，但由于一些情况下，实施这种研究是不可能的。必须指出，这可能也有其他适当的谐振模式，以更高的转速的转子和大量的有益的装载和体重变化。从理论假设，依赖挖掘机械能的参数磁系统的转换器和转速的转子非线性特性和所收到的效果不是最佳。从这个角度来看，暴露的最大输出功率，最大的体重变化和资源的转换代表的大型实用和科学的兴趣。在测试的样品转换器的使用较高的转速是不能接受的，因为unsufficient机械耐久性的磁系统，这是由单独的内置件。 

　　在图的依赖重量的平台和其输出功率，删除到电阻加载的转速转子的转换器是详细解释。该图是建造一个高压情况多极化的（顶部图）和高压开关两极化（下图） 。时间从开始的时刻引擎多达模式的自我一代的转换，在旋转的转子顺时针方向，大约等于1.5分钟。（电源启动发动机约2万千瓦，以减少对轴的转换，等于1 / 10 ） 。在实现的关键模式（ 550转。 ）变化的总重量的平台已经达到+ / -30 ％来自游戏。在这一点过渡到谐振模式下，革命与大加速度已上升至590转速和体重的变化高达+ / -35 ％来自游戏。在这一次不愉快的高频口哨声成了声。这个地方的图一旦开始后的一个关键点（倾斜的曲线α1 ）。在实现590转，第一阶段的电阻负荷1千瓦连接到电发电机。在呼啸的声音再次停止，革命的急剧减少和ΔG也正在发生变化。当革命开始再度增长，第二个开关的负荷和滚装连接器的转速是稳定在一个水平的590-595转。 ΔG继续发生变化。越来越多的负荷开关的步骤发生在1千瓦到总功率6千瓦。所有的时间间隔大约是平等的10-30秒。此后，短期增加的革命和随后的全面稳定的一种方式在12-15分钟的观察。 

　　50多个发射的这个转换器与绝对重复性三个月内进行。必须指出，即革命将加速增长，反映在图的角落α1 ... α5 ，如果不是发电机切换到下一步的装载，在转速将继续增加。两倍负荷需要返回前面的转速模式。 

　　上文的讨论涉及一个模式，高电压极化的20千伏“附加”了“停飞”状态。如果没有20千伏电压极化（下曲线）图大致相同，但表明了更为强硬的性质和更快的加载改变重量的一个平台，由于降低转速。 

　　其他有趣的效果包括工作的转换在黑屋子里电晕放电时，观察各地的转换器的转子作为一个蓝色发光粉红色的发光特性及臭氧的气味。在图云电离覆盖面积的定子和转子，并为此一环的形式。 

　　6 。电晕放电的转换器。论的背景下发光的发光滚轮，表面的，我们尊敬的一«波图片。 »一些更有力的狭长放电辊周围观察。这些排放物是一个白色的，黄色的特点，但声音电弧放电是没有听见。 На поверхностях статора и роликов не имелось никаких видимых эрозионных повреждений以及 

　　同样地。糜烂性损伤的电弧放电不在场的任何表面的定子或滚筒。 

　　还有以前的影响没有提到有人即垂直磁场同心“墙”周围安装。我们注意到和测量异常常任理事国周围磁场转换器内的半径15米。为测量磁场的磁力计，俄罗斯F4354 / 1使用。磁力仪使用霍尔效应传感器中的铜屏蔽。该地区增加强度的磁通0.05 Ť concentrically从位于中心的检测安装。的方向矢量磁场在这些墙壁正好与方向的滚子'字段病媒。结构的这些区提醒我们，界水从扔石头。这些地区之间，这种便携式磁力仪没有登记磁场异常。该层增加强度的分布几乎没有损失高达距离约15米的中心转换，并迅速减少在边境的区。厚度每一层约5 -6厘米。边界的每一层有大幅形状，层间距离约为50 -八零厘米在上限是当看到正在从中心的转换器。一个稳定的图片这一领域的观察以及在高度6米以上的安装（二楼以上的实验室）。上述二楼，测量，没有进行。类似图片的观察和境外的一个房间的实验室，直接在大街上，在地面上。同心墙是严格垂直，没有了可观的扭曲。在原理图安排的转换在一个房间里的实验室和安排同心磁场显示。 

　　图7 。示意图放置的模式转换和磁场实验室的房间。 

　　减少的反常高温在附近的转换还发现。虽然共同温度在实验室的背景是+ 22 ℃ （ ± 2 ℃ ）下降了温度等于6-8 ° C被发现。同样的现象，有人在同心垂直磁墙壁以及。测量温度的磁场内墙壁进行了一个普通的酒精温度计的惯性，说明约1.5分钟。在磁墙的温度变化，甚至可以观察到明显的手。当放入这个磁墙的手感到非常冷一次。类似的图片有人在上面安装高度，即在二楼的实验室，以及尽管钢筋混凝土封闭的上限，也露天以外的实验室。 

　　图。依赖强度的磁场和温度变化与转子转速的转换器。 

　　同心磁墙壁和随之而来的热效应开始显示自己可观的形象开始从大约200转。 ，并呈线性增长，越来越多的革命行动的重要模式。测量转速600以上还没有，因为害怕破坏磁系统。在图的曲线强度的磁场中мТ和改变温度摄氏度由于转速变化的是代表出席了会议。 

　　4 。讨论 

　　所有的结果，我们得到的极不寻常的，需要一定的理论解释。不幸的是，结果解释的框架内进行的常规物理理论无法解释所有的观测现象除了体重的变化。这是有可能的解释的体重变化作为一个地方的变化引力或作为反引力力击退自己的领域。直接实验，证实了存在草案武力是不能完成的，但在任何情况下都解释的体重变化并不符合现代物理学的范例。复议的标准引力理论是可能的，如果我们考虑到时空曲率。例如，通常吨克尔代表实地外部的轴对称旋转机构和区分积极和消极的自旋方向，以及前进，后退的时间方向[ 8 ] 。考试的物理真空作为一个来源的这些现象也可能有助于更好地解释，因为麦克斯韦应力能量张量附近的转换经历了一个复杂的演变。 

　　从现代物理学的立场，电气化和发光的转换器的磁系统在不久的区并不完全清楚。这种现象的磁性和热“墙”可能与尔芬的磁声波中提出的近区的磁化等离子体诱导可变的磁场旋转转子[ 9 ] 。在之间的能量交换空气分子和转换可能会发生。目前，我们不能给出一个确切的描述了互动机制和转变的能源，但没有相对论，我们是完全不能给身体大量的理论，这些现象。 

　　总之，我们强调指出，问题的生物效应的影响，特别是在变化的实时流的影响，必须发生在一个执行区的转换，并不被视为在所有。这些问题是极其重要的和绝对探索，尽管有一些提到JRRSearl约愈合行动赛格的辐射。我们自己的经验使我们只能谨慎的假设，即短期逗留（ 12分钟）在工作区的转换器与固定输出功率6千瓦仍然没有观察到这些后果暴露无遗。本文件只是一个开始。 

　　参考文献 

　　1 。施耐德， Koeppl ， ＆埃勒斯。 «相遇麻省理工学院的约翰率塞尔。 »空间与Ziet ， ＃ 39 ， 1989 ，页。 75-80 。 

　　2 。桑德伯格，冯南贡纳尔。 «什么是dran 10:00塞尔效应。 »空间与Ziet ， ＃ 40 ， 1989 ，页。 67-75 。 

　　3 。施耐德＆瓦。 «老挝塞尔效应奥夫之刺激。 »空间与Ziet ， ＃ 42 ， 1989 ， pp.75 - 81 ; ＃ 43 ， pp.73 - 77 。 

　　4 。托马斯小约翰A «反引力：国产的梦现实。 »超常的科学， vol.VI ，第2期， 1994年。 （又反引力：国产的梦现实，直接国际科学联合会， 1993年的ISBN 1-898827-99-0 ） 

　　5 。塞尔教授约翰率，该法的平方，图书1-8 ，直接国际科学联合会， 1993年的ISBN 1-898827-00-1 

　　6 。希尔，保罗R ，非常规飞行物体，汉普顿路， 1995年 

　　7 。 

　　7 。瓦隆，托马斯，在Homopolar手册，明确的指南氮机和法拉第磁盘技术，完整性研究所， 1994年 

　　8 。 

　　阿德勒，巴赞，并希弗。介绍广义相对论，希尔， 1965年，纽约 

　　9 。兰和里夫施茨。电动力学连续媒体.-莫斯科，科学， 1982 。 （俄文） 。

IGV的超过机场 　　 　　三IGV的机场 　　 　　四IGV的一个机场 　　 　　Square 4, Level 2 Diagram 　　 　　广场4 ，第2级片图 　　 　　在卡特IGV