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ISBN 978-

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New extended updated Edition 2019

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Table of Contents

Introduction of the extended edition 2019

Foreword to the new extended updated edition 2019

Calculations and Formula Collections with Drawings

Magnetmotor Patents and Plans

Magnetic Motor Design (Extended)

Various magnet motor models presented

Magnet motor models sorted by difficulty level

Build your own magnetic motor

Protection measures before assembly

Overview for the construction of a simple magnetic motor

Further useful information with material costs and construction time

Buying the parts

Shopping list and material list

tool list

Recommended equipment

Drawings and diagrams

Further engine drawings

The electric circuit

The assembly

Fixing the magnets

Coil winding

Build your own Coil Winding Device

Soldering the electric circuit

The battery

Operating and switching on the motor

Building of further magnet motors

Magnetic motor example 1

Magnetic motor example 2

Bonus

Premium magnet motor model for mobile phones

Bonus drawings and images of 3D models

Infinity SAV 1KW 3D Model

Muammer Yildiz 3D Model

Howard Johnson 3D Model

Friedrich Lüling 3D Model

V-Gate 3D Model

Mike Brady 3D model

Bonus Downloads

Closing words

Introduction of the extended edition 2019

Magnetic motors Perpetuum mobile

The solution to the energy problems?

For centuries, man has been fascinated by the idea of building a machine that can once be set in motion, continue to run and supply energy. It is therefore all the more surprising that more and more inventors and inventors seem to be able to build so-called magnetic motors. In any case, many of these inventions have even been patented, which involves a great deal of effort and expense.

No exhaust gases or other emissions, no harmful radiation, no disposal problems - nothing like that! Never again have to fill the oil tank before the winter, never have to feel like the plaything of the energy companies, because the gas, oil, gasoline, diesel or electricity prices increase again at will. No more having to drive to a gas station. Clean air, clean sea, recreation of forests, recreation of soils.

Could you imagine something more beautiful?

Who wouldn't want to examine such a magnetic motor more closely?

How is it constructed? What is the secret?

That information would be priceless, wouldn't it?

The inventor Muammer Yildiz has patented his magnetic motor. In his In his patent specification are incredible information and with it his contained construction drawings, which is connected with a lot of effort and high costs.

This book is also intended to give an insight into free energy to people who have not yet been so familiar with free energy and magnetic motors.

Discover the world of free energy and the technology of magnetic motors yourself with this book.

Just make your own picture of it, even if many people are against magnetic motors. Later in this book, we will go into much more detail on the subject: magnet motors and how to build an attempt at such a motor. With 3D models, bonus downloads, material list, pictures, drawings, tool list, shopping list, patents and much more.

Foreword to the new extended updated edition 2019

This book was written and summarized with much work. Because we care about our readers and we want you to be satisfied as a reader and for a better understanding we ask you to read the following foreword and notes about this book.

If you are really interested in building a magnetic motor, this book of the new Edition 2019 will help you with our 3D models. You can then download them and print them on a 3D printer, for example. If you also look at the 3D models on your PC, you can take a close look at every part of them. So it is much easier for you to build your own magnet motor! Here in this book we provide you with some 3D models!

From Friedrich Lüling to Howard Johnson and much more magnet motors. Simply find the suitable version for yourself to build a magnet motor, in which you simply experiment and on the basis of different magnet motor models a simple motor to reproduce.

In this book you will simply learn the basic tools, materials for the attempt to build a simple magnetic motor. In this 2019 edition, you will also learn more about patent specifications and the knowledge of other magnet motor models.

There are many people who would like to build a magnet motor. And that is why these people want to learn as much information as possible to build a magnet motor. We have researched a lot for this book and have been able to summarize a lot of knowledge about the technology.

And here in this book you will also learn a lot of background knowledge and also about many other magnetic motors. The construction of your own coil winding machine is also explained here. It is also about giving you an insight into the world of magnetic motors.

In this extended updated edition 2019 you will find all information for the attempt to build a simple magnet motor, but with even more magnet motor models, bonus pages, drawings and the 3D models.

If you want to build a magnet motor, simply build your own version with it in your own format and size and take this information from this book with you on your way!

Magnetic Motor Basic Knowledge

Many concepts have been presented in recent years with only one goal in mind: to generate energy as cleanly as possible and at the same time at low cost. No wonder, one might say, when one thinks of the conventional means by which energy has been generated in recent years and to this day.

Examples of this are: Coal-fired power plants, nuclear energy or the well-known combustion engine - all of them machines that have a comparatively low degree of efficiency and above all consume large quantities of non-renewable raw materials (e.g. crude oil). The so-called magnetic motor is quite different.

This special electric motor is similar to a conventional electric motor, but it has some characteristics and innovations that make it unique and could make it the future of power generation. Let's delve into this fascinating topic and take a closer look at how the magnet motor works and what makes it so special.

It is called either a magnetic motor or a magnetic generator.

As already mentioned: In principle, the magnet motor is similar to the conventional electric motor, but here not only one magnet is used, but several. Depending on the motor type and power, these differ in terms of both the number of magnets and their arrangement. The difficulty here is to find the appropriate arrangement of the magnets on the stator. In recent years and decades, a great deal has been tested here and new solutions presented time and again.

Magnet Motor - Electric Motor: The Differences

Let us now come to the really important differences between a conventional electric motor and a magnetic motor. While a conventional electric motor uses electricity to generate mechanical energy or work, a magnetic motor does not use electricity, it generates it! Only a certain amount of initial energy is required to start the magnet motor. Once in operation, it runs completely self-sufficient and produces electricity sustainably. A dream, isn't it? Thats where the idea of the famous Perpetuum Mobile comes to mind, i.e. a machine that runs practically infinitely without any input of energy from outside and produces energy by itself.

In order to understand how the magnet motor works, let's take another close look at the principle. Perhaps we can manage to outwit the assumptions of school physics. As already mentioned, the magnet motor is started once by hand and should then continue to run almost infinitely without the supply of external energy. This is due to the special arrangement and the quantity of magnets inside, which are supposed to keep the coil and the armature inside constantly moving. If it is doubted that there is a magnetic force that constantly attracts and repels poles, it would have to question our entire planet Earth.

For the earth with its magnetic poles has been rotating for millions of years and thus functions according to the same principle. According to physics, the planet Earth should not rotate at all, because no energy is added to it from the outside. Scientists, you are more closely concerned with the magnet motor, make these neutrinos responsible for the fact that the magnet motor functions. The neutrinos they contain are converted into magnetic force, which is then ejected by the magnetic motor in the form of electricity.

The advantages of the magnetic motor are obvious: It produces its own energy without having to be supplied with energy. It does not produce any harmful radiation, exhaust gases or other environmentally harmful substances. Thus the magnetic motor would be the ultimate solution for all energy problems in the world.

Why nobody has produced it yet can only be speculated about. Experts repeatedly mention the influential energy and oil lobby as the reason for this. To refresh the memory of some: A permanent magnet (or also a simple magnet) has a north and a south pole. While the north and south poles attract each other, the north and north or south and south poles repel each other. If you now place magnets, which are differently aligned, on a disk and put this disk into a circular container which also has exactly aligned magnets, you get a permanent magnet generator which once driven, no longer stops working. This is because the magnets permanently attract and repel each other. Since they are exactly aligned according to the building plan, they are in an imbalance so that they constantly attract and repel each other and thus produce a never-ending movement. This movement (also called kinetic energy) can be converted into electric current.

Magnet generators are based at this motion, which are based at attracting resp. repelling poles. In this way, a magnet generator produces energy. The energy is generated by the magnetic forces in the magnet generator. The higher these magnetic forces are, the higher is the energy which can be generated in it. In a magnet generator, the magnets used can move both to the fixed electrical conductor. The reverse case is also possible; the electrical conductor moves to the fixed magnet. In both cases, energy is generated.

For a magnet generator one needs only very simple means. For this reason even a hobby hobbyist can build such a magnet generator himself. Basically only a few magnets are needed. You can use ceramic magnets as well as rod magnets. Furthermore one needs a smaller as well as a larger wheel to which the magnets are attached. First you attach the magnets to the smaller wheel. It should be noted that these are attached in the same polarity to the wheel. The smaller inner wheel must remain movable. Around the inner wheel the bigger wheel is fixed. This wheel should be made of a non-conductive material. Magnets are now attached to this larger wheel. These must be opposite in their polarity to the inner ring. Now the magnets of the outer ring and the magnets of the inner ring work on each other. The inner ring begins to rotate. After some time it turns faster and faster and energy is generated. In this way you can create a permanent magnet generator.

The circular accelerator

Most magnetic motors and approaches are circular accelerators. The advantage is obvious, as a compact motor can be built by the circular motion.

With a linear accelerator, the distance would have to be endless, or the part to be moved would somehow have to be led back to the beginning.

The challenge with a circular accelerator is the so-called sticky point. This can be described quite simply using the example of the V-gate.

V-Gate principle structure and V-Gate forces for a better understanding of the structure of the V-Gate engine. (The view is from the front to the round rotor).

V-gate forces

Here are the different forces acting on the rotor. Before the rotor rotates to the sticky point, the stator repels the two obliquely arranged rows of magnets on the rotor and the rotor rotates. At some point the rotor has rotated until the sticky point is reached. Here now 2 forces work.

There is also the repulsion of the external rows of magnets, which have set the rotor in rotation. In addition there are the counteracting forces of the inner rows of magnets. You can see by the blue arrows at the top of the stator.

These act against the direction of rotation and stop the rotation of the rotor. In order to overcome the sticky point more easily, the "first" inner two magnets with the polarity are inserted the other way round.

With other magnet motors there is the same problem of the sticky point, and different approaches to overcome it. If the "Sticky Point" did not exist, magnet motors in series production would probably already be the norm.

The V-Gate magnet motor is a circular accelerator. In contrast to the linear accelerator, here the 2 rows of magnets are guided around a tube or wheel. Due to the circular arrangement of the magnets, the rotor is accelerated.

A longitudinal magnet serves as a standing part (stator). Once the rows of magnets are guided around the rotor, the magnets of the outer line meet those of the inner line.

Calculations and Formula Collections with Drawings

Now you get more calculations and formula collections from Howard Johnson.

His work revolved around simple mathematical observations and calculations. Starting with Coulomb's law..:

The action of the f-line with the distance of the straight line between the poles, the superposition properties related to several poles and the limitation to systems fixed in space are all known conditions. They use the overlay properties to increase the application of a spatial domain with many more poles. However, this is first divided into numbers to better develop the analytical expressions.

Our analysis will be two-dimensional and on the same plane, bounded by the vertical x-y plane. It should be noted that the horizontal column "track" of Howard Johnson's linear model has many flat magnets with a rectangular cross section, each with an aspect ratio (length x thickness) of 16.

This high value is the reason for this two-dimensionality of the model and helps to minimize and effect the z direction. This is the reason for the two-dimensional analysis, at least in the case of the linear model we are looking at here.

Even though Coulomb's law repeatedly arouses suspicion, it offers a simple yet useful form. It describes the interactions between two magnetic mono- poles.

where M and M' describe the pole strength (positive if north, negative if south), u is the permeability of the medium in which the poles are located, r is the distance between the two poles in a straight line, and f is the force vector acting on each pole individually, positive for repulsion and negative for attraction.

The Coulomb Law

Coulomb's law is a very important law from the basics of electrostatics. In words, it means that the force between two point charges is directly proportional to the product of the two charges and inversely proportional to the square of their distance. The direction of the force coincides with the line connecting the two charges. If you have not understood this, simply enter the appropriate values into the following equation:

And there is:

"F" the force in Newton

Q1" and "Q2" are the charges in Coulomb - but in our example M and M.

r" the distance in meters

ε0" the electrical field constant

"π" the circle number, π = 3,14159...

The numerical value for the electric field constant cannot be determined theoretically, but must be measured during a test. The force between the charges is repulsive if the charges have the same sign. This results in F > 0. If the sign of the two charges is different, the two charges attract each other and the force F is less than zero ( F < 0 ).

Coulomb's law uses the idea of a point charge. Below, one imagines a charge that is only present at a single point. However, this is a theoretical model. In reality, a charge can never sit in one point, but only on a body with finite extension. Nevertheless, Coulomb's law can be applied practically: If the charges are evenly distributed on a sphere surface, the distance between the centers of the sphere can be interpreted as the distance between corresponding point charges.

To illustrate some of the prerequisites and extensions of Coulomb's law, let us first give a simple example of a magnetic disk located along the x-axis. The plate, with a limited length L, is a permanent magnet magnetized over its y-direction thickness and with a high aspect ratio (to eliminate z-direction corner effects).

The south pole side is directed upwards, with the north side downwards on the underside of the plate. Underside effects are ignored as if the plate shows a continuous distribution of only southern monopoles along the x-axis. To integrate this distribution, we swap M' with the differential dM' and use the function B(x) so that it looks like this at the end: dM' = B(x) dx

The size of the total strength transmission, F, based on an isolated northern monopoly with strength M, placed somewhere in the upper half of the x-y plane.

where x is the ratio x/L. Assuming the magnetic strength along the plate can be represented by the southern constant -B and neglects end effects at x = 0 and x = L, reduced to

where the strength parameter M' was determined by the integration - over the plate length L and p is the ratio r/L.

Now comes the symmetrically positioned northern monopoly over the center of a magnetized attracting plate. (Center picture 1)

Then comes the effect of force imbalance on a north monopoly over a magnetized plate and tends to restore the pole to the leaf.

(Center Fig. 2)

If the northern monopole is placed directly above the center of the plate, at the coordinates (E,n), with E=L/2 and the vertical air gap separation distance of the increasing force vectors acting on (E,n), the result is as shown above in center Figure 1

Note that a shift of the north monopoly to the left creates a force imbalance that pulls the pole back to the right, as shown in the center of Figure 2. If we now only consider the x-component of F, we write

Here the calculation for image (8)

where X and Y are the dimensionless relations. 9 and 10 can be integrated for each fixed position (XY) of the North monopoly in the upper half of the plane this can be integrated to yield 11.

(11)

Then comes the X-directional distribution of the X-components of attracting strengths, exerted at a north monopoly by a thin, magnetized plate. This ratio is shown as a continuous function that parametrically considers X position with Y. The Y=1 curve represents the field influence of the north monopoly positioned at a constant air gap separation (n=L) at a fairly vertical distance above the plate. Whereby at Y=0.1 the monopoly is positioned much closer to the X-axis. The reversal of the starch components by its zero value in the middle of the plate (X=1/2) is clearly visible. To record some trajectories through this field we now assume that the y-component will be F.

In dimensionless form of equality of motion for trajectories of monopoles upside of plate in flat X-Y space..:

And the following formula:

Here t is present and T is only a randomly chosen time. As previously mentioned, L is the length of the plate; whereas g is the gravitational force of attraction constant and W is the force of the downward weight of the moving monopoly over the plate. For the magnetic force determinations (rx)mag and (ry)mag we exchange directly from the formula (Figure 11) and the formula (Figure 12). Some of the trajectories resulting from the integration of formula (Figures 13 and 14).

The repulsive plate

If one replaces +B with -B for B in, the plate length L, which lies along the X-axis, becomes repulsive with the northern side upwards, opposite the north monopoly above on position (E, n). Of course the sign becomes positive and the functions (rx)mag and (ry)mag change their behaviour accordingly. Again, (rx)mag gets a balance point at X = ½, but now it's destabilizing. As a consequence, the trajectories for the North monopolies in this case are much more interesting than they were with the attracting plate. Figure 11 below shows different trajectories with different values for the W/J trajectories.

Parameter G was included and in each example the trajectories started at (0.9, 0.2) with an initial velocity of zero. We continue with the trajectories of a north monopoly in a repelling field, produced by a thin, magnetized plate which lies in the X-interval 0-1..:

The attractive and repellent plates can be easily demonstrated since rubberized, flexible plate magnets are available on the market, e.g. at Permag Corp. of Jamaica, NY. It might also be interesting to know that with minor modifications, this first simple analytical plate can be used to gain insight into the function of the so-called "magnetic wankel".

The oscillatory path of a northern monopoly behaved by x-directional motion over a three elementary linear torque arrangement..:

In this picture you can see that the North Monopoly was allowed to start moving itself in the origin with Vx, starting with zero.

Now we come to our last adaptation which, as it turned out in the first test a few months earlier, is an exciting revelation. Johnson found that the horizontal air gap between the magnet elements, which includes the torque track, should vary slightly from the norm to compensate for the movement of the fittings.

Introducing this variation into a two-dimensional model, assuming the load is uneven, would certainly convert the field from conservative to non-conservative.

In the meantime, it should be clear that only an unconservative model has the chance to explain the phenomenon of the permanent magnet motor.

With these thoughts in mind, an attempt was made to vary the armature monopoly of image 14 in the second torque magnet and above, the horizontal distance parameter, xp during the integration process (including during motion).

The result is shown in Figure 15 below.

It was found that through small variations in the xp, as the monopoly developed along the trajectory track from one X position to another, enough control was possible to move the pole over the full length of the torque and beyond.

With this expression the integration becomes uncomplicated and provides the typical oscillatory type of trajectory as shown here.

Howard Johnson found that the focusing magnet armatures of his linear model start at both ends of the torque path, simply by ensuring that the northern end of this bipolar crescent leads south. (See Figure 1):

This image shows how the X direction moves from right to left instead of left to right as in our previous example. It is also made easy by simply turning the figure 90° clockwise, the behavior of the dimensionless speed, since Vx is defined as:

Figure 15: Continuing path of a north monopoly restrained and recording x-directional motion, like a linear torque.

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The Magnet Motor

Introduction of the extended edition 2019

Foreword to the new extended updated edition 2019

Calculations and Formula Collections with Drawings

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