Background Art of the Invention The object of this invention is to provide novel method in which unidirectional thrust is generated without any matter that is being propeled and thrown out of the structure, and device to use electric and magnetic fields, with motor to provide rotational motion.

The advantages and uses of the propelentles field thrust generator are many. The most important is use of this method and device in space crafts and rockets whose gas and flame exhausting engines are wasting matter which can not be replenished in space. Also the device is environmently friendly because it does not exhaust any polutants and gases. It can be used not only in space for space crafts, but can replace all gas exhausing enginees for continental, intercontinental and local flights thus saving our atmosphere.

This invention provides very efficient conversion of mechanical force of rotational motion to a unidirectional thrust, strong enough to propel both device and the whole structure to levitate, accelerate and fly near the surface as well far away from it like in deep space, in controled manner.

Summary of the Invention This invention is aimed at providing an rotary device with electromagnetic propeler for efficient conversion of mechanical rotational energy into unidirectional motion of the structure. One prefered embodiment of rotary device is electric motor at the center with legs attached to rotor of electric motor and at the end of those legs are fixed electromagnetic propelers.

Other preferered embodiment is also electric motor at the center and its rotor will rotate ring attached to structure, with electromagnetic propelers being fixed inside that ring

or on its surface. Electric motor might also be located near the rim of the structure close to rotating ring.

This invention also provides electromagnetic propelers, which can be of two types, electric or magnetic propelers, with asymmetrical fields created by using various shapes of electrodes and magnets, and various dielectrics with various shape and/or dielectric constant.

One prefered embodiment of electromagnetic propeler is magnet shaped in tringle form and with variable, nonsymmetrical dimensions. Magnetic field generating means might be permanent magnet. Superconductor plate paralel to the magnet to repeal magnetic field to futher increase asymmetry of the magnetic field might be used.

Other prefered embodiment of electromagnetic propeler are electrodes that use high electric potential. The shape of electrodes is asymmetrical. One embodiment is electrode in form of semicircle plate and other electrode pair in form of straight cable in the center of that semicircle. Other prefered embodiment of electrodes are paralel flat plates of various length for one electrode and flat plate perpendicular to them as other electrode. The space between electrodes might be filled with dielectric.

This invention also provides an system for controling and directing an electromagnetic fields of electromagnetic propeler and also fields inducted by rotating electromagnetic propeler.

In one prefered embodiment a tube that is running through longitidinal axis of structure is directing electromagnetic fields. Other embodiment is in form of skin around the space that will protect passangers of structure from strong inducted electromagnetic fields.

That skin might be metalic. Yet another embodiment for controling propagation of electromagnetic waves is set of canals and those canals might be also made of metal.

This invention also provides an system for efficient use of counter EMF in such way that unidirectional thrust is created.

In one prefered embodiment, counter EMF is created in plate located near the rotating electromagnetic propeler and it opposes electromagnetic fields of propeler thus creating thrust. In yet another prefered embodiment, the counter EMF is created in space located near the passing by electromagnetic propeler.

This invention provides a system to eliminate not needed countra rotation of the structure created by main rotating device for propeler, so the whole structure will stay still and not rotating.

One prefered embodiment is to have attached to the structure dome-shape object which is rotating countrary to the main rotating propeler. The dome-shape object might also cover and protect the whole device from the surrounding medium.

In other prefered embodiment more then one electric motors are used and their prefered position is closer to the edge of the object so contra rotation of the whole structure is eliminated.

This invention also provides space for pasangers and machinery of the structure, its relative position to the main rotating propeler and motor and canals, plates that accompany propeler.

Prefered embodiment for space for the passangers is above rotating propeler. In other prefered embodiment, space for passangers is located between rotating ring with electromagnetic propelers.

This invention is also aimed at providing generator of electrical energy for internal needs of energy consumption in the structure.

Brief description of drawings: Prefered embodiments of this invention will now be described by the way of example with reference to the accompanying drawings in which: Fig. 1A shows a side view of mechanical oscillator with spring and ball in its lowest position.

Fig. 1 B shows a schematical view of LC circuit with capacitor being charged to the maximum.

Fig. 1 C is a plot illustrating relationship of displacement, acceleration and speed when comparing systems in Fig. 1A and Fig. 1B.

Fig. 2A shows a side view of the same mechanical oscillator as presented in Fig. 1A, but with the ball in its middle position.

Fig. 2B shows a schematical view of the same LC circuit as presented in Fig. 1 B, but with capacitor not charged.

Fig. 2C is a plot illustrating relationship of displacement, acceleration and speed when comparing systems in Fig. 2A and Fig. 2B.

Fig. 3A shows a side view of the same mechanical oscillator as presented in Fig. 1A and Fig. 2A, but with the ball in its upper position.

Fig. 3B shows a schematical view of the same LC circuit as presented in Fig. 1 B and Fig. 2B, but with capacitor charged opposite to that in Fig. 1 B.

Fig. 3C is a plot illustrating relationship of displacement, acceleration and speed when comparing systems in Fig. 3A and Fig. 3B.

Fig. 4 is a side view of half-wave dipole transmiting antenna and its electric and magnetic fields.

Fig. 5A shows expansion of electromagnetic field shown in Fig. 4.

Fig. 5B shows colapse of electromagnetic field shown in Fig. 4.

Fig. 6 shows side view of ball rotating in circle.

Fig. 7 shows a plot with acceleration of the ball in Fig. 6 versus time.

Fig. 8 shows partial side view of right half of antenna shown in Fig. 4, but only with its electric fields.

Fig. 9A shows a antenna derived from a Fig. 8.

Fig. 9B shows a profile of the antenna in Fig. 9A.

Fig. 10A shows a cut of another antenna form derived from Fig. 8.

Fig. 10B shows a front view of the antenna in Fig. 10A.

Fig. 10C shows a profile view of the antenna in Fig. 1 OA.

Fig. 11A shows profile of yet another another antenna form derived from Fig. 8.

Fig. 11 B shows a front view of the antenna in Fig. 11A.

Fig. 11 C shows a front view of another form of the that as shown in Fig. 11 B.

Fig. 11 D shows a front view of simplified form of antenna shown in Fig. 11A.

Fig. 11 E shows a profile of the antenna shown in Fig. 11 D.

Fig. 11 F shown a top view of the antenna shown in Fig. 11 D.

Fig. 12 shows profile view of yet another antenna derived from Fig. 8.

Fig. 13A shows partial side view of antenna based on Fig. 12.

Fig. 13B shows side view of antenna shown in Fig. 13A..

Fig. 14 shows another form of antenna derived from that shown in Fig. 13A.

Fig. 15 shows partial side view of right half of antenna shown in Fig. 4, but only with its magnetic fields.

Fig. 16 shows partial side view of upper half of magnetic fields shown in Fig. 15.

Fig. 17A shows partial upper side view of the magnet whose form is based on magnetic fields as shown in Fig. 16.

Fig. 17B shows back view of the magnet shown in Fig. 17A.

Fig. 18A shows back view of yet another magnet whose form is based on magnetic fields as shown in Fig. 16.

Fig. 18B is top view of the magnet shown in Fig. 18A.

Fig. 18C is a side view of the magnet shown in Fig. 18A.

Fig. 19A shows front view of yet another combination of two magnets whose form is based on magnetic fields as shown in Fig. 16.

Fig. 19B is top view of the magnet shown in Fig. 19A.

Fig. 19C is a side view of the magnet shown in Fig. 19A.

Fig. 20A shows front view of another form of combination of two magnets whose form is based on magnets as shown in Fig. 19A.

Fig. 20B is a side view of the magnet shown in Fig. 20A.

Fig. 21 is top view of magnet from Fig. 17A rotating in a circle as shown in Fig. 6, having magnet instead of the ball.

Fig. 22 is partial side view of rotary device with magnets from Fig. 17A.

Fig. 23 is partial side view of rotary device with antenna from Fig. 11A.

Fig. 24 is partial side of rotary device shown in Fig. 23 wrapped in special case.

Fig. 25 shows profile of rotary device similar to that shown in Fig. 22 and with surrounding oblique shape plate, which is also shown in Fig. 26.

Fig. 26 is bottom view of the Fig. 27 and partially is bottom view of the device in Fig. 25.

Fig. 27 is profile view of one embodiment of the craft which illustrates usage of the rotary device described in Fig. 22 and Fig. 25.

Fig. 28A is partial cross section view of a craft that is one of the embodiments as illustration of usage of the ring shown in Fig. 24 and antenna shown in Fig. 11A.

Fig. 28B is shematic view of the craft shown in Fig. 28A.

Fig. 29 is partial cross section view of the ring shown in Fig. 24 and antenna shown in Fig. 11 A.

Fig. 30A is partial side view of another embodiment of the ring shown in Fig. 24.

Fig. 30B is profile view of the embodiment of the ring shown in the Fig. 30A.

Fig. 31 A, 31 B and 31C are side view as illustration of few of the embodiments of the craft shown in Fig. 28A.

Fig. 32A and 32B are side view as illustration of craft shown in Fig. 28A during the operation mode.

Detailed description of drawings: Detailed description of drawings will start with description of new and novel method of this invention. Then devices designed by that method will be described here, but only few of them, as many various shapes and forms may be reproduced by this new method.

Refering to Fig. 1A and Fig. 1 B. we see comparation and analogy of mechanical and electrical oscillations. Mechanical oscillations are created by spiral steel spring with heavy lead ball of the end of it, as in Fig. 1A. Electrical oscillations are created by simple LC circuit, with condenser and inductor as in Fig. 1 B. The mechanical oscillator is charged with energy by pulling lead ball down, as in Fig. 1A, and electrical oscillator is charged with energy by charging capacitor as in Fig. 1 B, lower plate of capacitor is charged with positive and upper with negative charge. Chart with values for displacement and speed for both mechanical and electric oscillators are shown in Fig. 1 C, where displacement value for both oscillators is maximum negative, and speed is at null. Energy of ball and inductor are at the minimum, and energy of spring and capacitor are at the maximum.

When ball is released, restoring force from spring produces an acceleration of ball, and transfering its energy to the ball, and pulls it up in position as in Fig. 2A. The similar process is with electric oscillator, force from capacitor is transforming into energy of inductor as in Fig. 2B. Now chart in Fig. 2C. reflects new values of both systems, where displacement value for both mechanical and electrical oscillators is zero, but speed is at the maximum.

Energy of the ball and inductor are at the maximum, and energy of spring and capacitor are at the minimum.

Now energy stored in the ball and inductor will transform into energy of spring and capacitor, but in opposite direction of charge then at the begining. Displacement value of spring measured by distance D and displacement value of capacitor measured by voltage will grow but in opposite. The result is in Fig. 3A. and Fig. 3B. Chart in Fig. 3C. shows that displacement value for both oscillators is maximum positive, but speed is at null. Energy of ball and inductor are at the minimum, and energy of spring and capacitor are at the maximum.

Since this invention relates to electromagnetic systems, the open oscillating antena with electrical and magnetic fields is shown in Fig. 4. That antenna is similar to oscillator in Fig. 1 B, but is open, not closed, thus having very small inductance and capacitance which allows it to oscillate at higher speed. The current in such transmitting antenna is not equal in all parts of conductors on left and right sides, but is strongest in area closest to the center,

and weakest in the area farthest from the center. Thus magnetic and electic flux are greatest in the center of such antenna. Electric and magnetic fields expand and then collapse as current varies as in typical AC (alternating current) systems. While they expand, they create outward force directed from the center, or in other words force is created from the area with highest electric and magnetic flux towards area with lower flux, as shown in Fig. 5A. When electric and magnetic fields colapse, they create inward force, which is in opposite direction as shown in Fig. 5B. The most interesting part of oscillating cycle is when outward force is created, which for this open antenna is the same period as for oscillating circuit from Fig. 2B. when it oscillates towards state which is in Fig. 3B. In other words, when speed of change of displacement value of voltage is at highest level, which is from zero to maximum, when capacitor is not charged and just starting to charge, which was confirmed many times in practice. That period is shown on Fig. 2C as period from 90 degrees to 180 degrees.

This new method will allow oscillator of special form and shape to be permanently at highest level of speed and acceleration, as in Fig. 2C is point at 90 degrees, and to permanently create outward force, like that in Fig. 5A, and to eliminate unwanted state when inward force is created like in Fig. 5B. The new oscillator is of such quality to be permanently in state of highest acceleration and to permanetly create outward force. Description of such special type of oscillator follows.

The only known form of permanent acceleration is rotational motion, as shown in Fig. 6. with ball rotating around center C. The acceleration value for rotating body is shown in Fig. 7. and is permanently at the same highest level, unlike value of acceleration in Fig.

1 C which changes from positive to negative during oscilating cycle, and is proportional to voltage displacement, but opposite in direction.

Refering again to Fig. 4. and Fig. 5A. now period of oscillation will be derived in order to produce field of such shape that will create outward force, from area with high field flux towards area of lower field flux as shown in Fig. 5A. But Fig. 5A shows symmetrical fields and symmetrical force that is created by them, and sum of the force is zero in such symmetrical system. Thus that symmetry needs to be broken, and in such way that it will resemble the fields that are created in period of cycle when antenna, or capacitor, is just staring to charge, from zero to maximum value, which is period that is shown in Fig. 1 C. from 90 degrees to 180 degrees. Those two goals, breaking the symmetry of antenna's fields, and simulating the period of initial charging as shown in Fig. 1C from 90 degrees to 180 degrees. are solved as shown in Fig. 8. In Fig. 8. right part of antena 1 is shown and area of

fields 2 that represent the form of fields in the central part of Fig. 4. Since left part of antenna doesn't exist in Fig. 8. it has to be added in form of metalic plate 2 in Fig. 9A. and right part of antenna is still in form of long metalic stick 1 on Fig. 9A. The Fig. 9B is the same shape of antenna as in Fig. 9A. but when looking from a side, the same elements are shown, element 1 is long metalic stick and element 2 round metalic plate is perpendicular to it, but at some distance from stick 1. Fig. 9A. and Fig. 9b. are the same special shape of asymmetrical antenna that is basic shape derived from symmetrical antenna on Fig. 4.

Futher shapes can be derived now from basic asymmetrical antenna shown in Fig.

9A. One of the examples is shown in Fig. 10A. with the same example but from different point of views shown in Fig. 10B. and Fig. 10C. On all three Fig. s, element 2 is still round metalic plate, similar as element 2 in Fig. 9A. but element 1 has now shape of metalic cylinders perpendicular to element 2 in Fig. 10A. The element 1 might consist of one or more then one cylinders, and three of them are shown in Fig. 10A. also in Fig. 10B. and Fig. 10C.

The Fig. 10B. is view from the top. The central cylinder is always longest, and length of cylinders decreases as distance from the center increases, in order to keep cone shape of fields as shown in Fig. 8. Example with three cylinders with various lengts is shown in sectionplan in Fig. 10A. and under different angle of view Fig. 10C. The central cylinder, closest to the center of plate 1 is the longest, the middle cylinder next to it is shorther, and the cylinder farthest from the center of plate 2 is the shortest. The dielectric 3 can be added to the antenna in order to decrease distance between electrodes 1 and 2 and thus have even greater electric flux.

Even further shape can be developed from basic asymmetrical shape of antenna shown in Fig. 9A. One example is shown in Fig. 11A. which is the same shape as in Fig.

11 B. but from different angle of view. In those two figures, the element 1 is in form of plate, and might be only one plate or more then one plate. If more then one plate, then they might be separated from each other as shown in Fig. 11 B. The side view of that shape of antenna will be the same as for that in Fig. 10A. with central pair of plates being longest, and the pair of plates closest to the end of plate 2 being shortest, as shown in Fig. 11A. The shape of plate 2 in this type of antenna is square, as shown in Fig. 11 B. but does not have to be, it might be of rectangle shape, which is presented in Fig. 11 C. The same relation of lenght of plates 1, having central pair longest and those at the end shortest, is kept in embodiment shown in Fig. 11 C. The simpliest form of such type of antenna is shown in Fig. 11 D. and

under different angle of vies on the same antenna in Fig. 11 E. and Fig. 11 F. There, metalic plate 1 is the only one plate and is perpendicular to metalic plate 2, and there might be a dielectric 3 between them. That is a simpliest form, but as shown in Fig. 11A. and Fig. 11 B. and even in Fig. 11 C. there might be more then one plate, and if there is more then one plate, the prefered embodiment is such as to have even number of plates, although one central plate might exists and in such case uneven number of plates will be in such design.

The next shape of asymmetrical electrodes for radiating antenna is shown on Fig. 12, with plate 2 and small sphere 1. The plate 2 is round metalic plate, the same form as plate 2 in Fig. 9A. Another embodiment is shown in Fig. 13A. which is side view of it. Part 2 in Fig.

13A. is no longer plate as part 2 in Fig. 12, but dome shape and sphere 1 is in the center between egdes of dome 2. Between them might be dielectric 3. The Fig. 13B. is side view of the same embodiment, with 2 being dome shaped metalic plate, 1 metalic sphere, and 3 dielectric material in between them. The similar solution is in Fig. 14. and diffrance is that plate 2 is in form of semi cylinder and central electrode 1 is not in form of sphere but in form of long wire streaching paralel to plate 2, with dielectric material 3 between them.

The polarity of electrodes 1 in all above described embodiments, as in Fig. s Fig.

13A, 13B, 11A-F, 10A-C and 9A and 9B is not important, electrodes 1 can be either positive or negative, and electrode 2 is always of opposite polarity as electrode 1, thus keeping the most of the energy of electric field concentrated in small area. The space between them might be filled with dielectric material, having as prefered material polyimide film capible to withstand stress of high voltage during long period of time. The shape of electrodes, quality of material between them, can be made in wide variety of forms, not limited to above described form of radiating antennas. The common for all of them is asymmetry of shape of electrodes, or asymmetry of dielectric material between them, either also in shape of dielectric or its dielectric properties. The more asymetrical electrical flux created by electrodes and dielectric, or the more gradient of electrical field is created in space around electrodes, the better because then antenna will affect space around it in asymmetrical way, transmiting its power more to one direction then to other, which allows such antenna to be set in unidirectional motion, or structure that holds and uses such antenna. For example, the gradient in space between electrodes shown in drawing Fig. 10B and 11A is such as to look like a wall paralel to the plate number 2, when high voltage potential is applied to their electrodes. The gradient of electric field is asymmetrical, which means that most of the area around the electrodes will be affected more by one polarity and less by other, although

potential applied to electrodes is equal and of opposite polarity which allows high concentration of energy in small area of electrodes to be used. That wall of gradient and how to use it will be explained in later description of drawings, after description of embodiments with asymmetrical magnetic field will be given bellow.

The next set of drawings and description relates to embodiments where magnetic field of magnet is shaped in special form in order to break symmetry of magnetic potential thus having that field influencing surrounding space with different force in different directions.

It has to be noted that number of possible asymmetrical shapes of magnetic field is less then those for electrodes above described for asymmetrical electrical antenna. That is first disadvantage of magnetic filed based asymmetrical antenna over the asymmetrical electrical antenna. The next disadvantage is lower power that can be used, because generally permanent magnets will be used to generate strong magnetic fields. High temperature superconductors might be used also. Next disadvantage will be relativly small number of such magnets with asymetrical fields in space close to each other, because if placed too close to each other, their magnetic fields will interact with each other, which will have effect of distorting asymmetry of their magnetic field. This is because magnetic field can not be shielded that well as electrical fields can be shielded by dielectrics with high dielectric constant, like for example polyimide films. One big advantage of using permanent magnets is that there is no need to supply them with energy, like in case of antena with electrodes that needs supply of high voltage.

In order to make the asymmetrical shape of magnetic field which can be used for unidirectional transmition of electromagnetic fields, the Fig. 4. will be used as sample, and only right part of those symmetric magnetic fields are shown in Fig. 15. Magnetic field on Fig.

15. is already asymmetrical, but lower part of magnetic field lines will be cut, which is presented in Fig. 16. What is shown in Fig. 16. is one quoter of magnetic field lines from Fig.

4. Such form of magnetic fields in Fig. 16. is easily reproducible by emobodiment of magnet as shown in Fig. 17A. The shape of magnet 1 in Fig. 17A. is triangle form, with North side on upper side of magnet in Fig. 17A. and South pole of magnet in lower side of magnet 1. The Fig. 17B. is view of the same magnet, but from the back, 1 is magnet, 2 is material that lets magnetic fields from bottom side of magnet pass through it easily, thus increasing asymmetry of magnetic field, as shown in the same Fig. 17B. Magnetic field of such form of magnet is concentrated in upper part of magnet, and propagate between North and South

poles of magnet. South pole is shown on right side of the magnet in Fig. 17B. and North pole in the left side of the same magnet in the Fig. 17B. Magnetic field in the same Fig. 17B. is more non-linear then field on the lower side, because part 2, which is made of high permiabillity material is not letting lower part of magnetic field to propagate in the same direction and distance as field on the lower part of magnet. Thus, highly asymmetrical magnetic field, almost the same shape as that in Fig. 16. is achieved by shaping magnet as in Fig. 17A. and Fig. 17B. and adding to the lower part of it material with high permiabillity.

The asymmetry of magnetic field can be futher increased by making a magnet in form as shown in Fig. 18A. Such magnet is also of triangle form, but not only in one plane as in Fig. 17A. , but triangle form is in two planes, and Fig. 18A. is back view of it. Magnet 1 has sticked to lower side of it a part made of high permiabillity material 3, and top 2 of the magnet which is in the center between North and South pole. The Fig. 18A. correlates to the Fig. 17B. in that they both are back view of magnet, and its clear that form in Fig. 18A. has sides cut in such way that they meet at the point 2 of magnet in Fig. 18A. which is in the middle of magnetic North and South pole sides. The next Fig. 18B. is top view of Fig. 18A.

The top edge 2 is the same as top edge 2 in Fig. 18A. and there is shart Tip on the left side, on opposide side of the Back of the magnet in the same Fig. 18B. The magnet 1 has also triangle form in that plane, so when looking at the magnet in Fig. 18B. it will look the same as magnet in Fig. 17A. because they both have triangle form in such way that distance from the middle point to the magnetic poles is decreasing, being maximum at one side, and decreasing towards another side of magnet, and finally both pole meet in the middle, as shown in Fig. 18B. having North and South pole closest to each other at the right part of magnet, and farthest at the left side of that magnet. The difference in shape of magnet in Fig. 17A. and the same magnet in Fig. 17B. when comparing it to the magnet in Fig. 18A. is clear when comparing only Fig. 17B. with Fig. 18A. , which both are back views of those two magnets. The magnet in Fig. 18A. has not rectangular back side as a magnet in Fig. 17B.

Those sides are cut in such way that the longest side of magnet will be at the bottom and they shorten with weight of the magnet. Of course, becuase of those cuts, the magnet will be also have odd sides in yet another plane as shown in Fig. 18C. which is side view of the same magnet. There in Fig. 18C. magnet 1 has high permiabillity plate 3 on lower side, and top of magnet 2, which is the same as tip 2 in Fig. 18A. and Fig. 18B., aslo is shown sharp Tip of the magnet 1, the same as Tip on the Fig. 18B. and their function will be described bellow.

This form of magnet will be best described as flat half-pyramid shape, which can be made if flat pyramid will be cut from the top to the bottom, along the one pair of the opposing edges.

The next embodiment of magnet with asymmetrical fields is shown in Fig. 19A. , with different view on it shown in Fig. 19B. and Fig. 19C. In this embodiment two magnets are used instead of one magnet as in previous two embodiments in Fig. 18A. and Fig. 17A. In Fig. 19A. two magnets, magnet 1 and magnet 2 are sticked together with their opposing magnetic poles, in such way that North pole of magnet 1 is at the top and next to the opposing South pole of magnet 2. The South pole of magnet 1 and North pole of magnet 2 are fixed on the plate 3 which is made of high permiabillity material. The shape of such embodiment is not ideal but it resembles the shape of magnetic field as in Fig. 16. and it is asymmetrical. It is also in triangle form, as shown in Fig. 19B. which is top view of that embodiment, with magnet 1 and magnet 2 being each in triangle form and connected with their longest side. Magnet 1 has North pole side from that view, while magnet has South pole side from that view. The Fig. 19C. is side view of the same embodiment, with magnet 1 and plate 2 made of high permiabillity material. The magnetic field flux shown in the Fig. 19C. is asymmetrical, with gradient of magnetic field growing from the right side to the left side.

Yet another possible embodiment, similar to that in Fig. 19A. is shown in Fig. 20A.

The difference is that magnets 1 and 2 are cut in such way that they are thinest at the center, and thickest at the end. The plate 3 made of high permiabillity material is also shown.

This embodiment is also in triangle form and when viewed from the top it will look the same as in Fig. 19B. Next Fig. 20B. is the side view of the embodiment of magnet in Fig. 20A. with one magnet 1 shown there, and with sharp Tip shown also, and with plate 2 made of high permiabillity material.

The above decribed embodiments of magnets, in Fig. 17A, Fig. 18A, Fig. 19A and Fig. 20A are description of magnets with asymmetrical field flux, thus with gradient of magnetic flux, and which resemble the shape of magnetic field of transmitting antenna shown in Fig. 16. The prefered embodiment is the shape of magnet described in Fig. 18A., which is the same magnet as in Fig. 18B. and in Fig. 18C. The next part of description of this new method and device will be on how to use above described both asymmetrical magnets and electric antennas in order to achieve permanent effect of greatest creating of force, like that when electromagnetical devices are powered on, and to create unidirectional thrust with such method and devices.

In order to simulate expansion of magnetic fields shown in Fig. 16., that will be similar to the expansion of fields in radiating antenna in Fig. 4. with forces of expansion shown in Fig. 5A. , it is necessary to have magnetic fields of the prefered embodiment of magnet with asymmetrical field described in Fig. 18A. expand in time, in the same manner as magnetic fields expand in time as shown in drawings in Fig. 4. and Fig. 5A. The difference between antenna shown in the Fig. 4. to the magnet with its magnetic fields in Fig. 18A. is that antenna in Fig. 4. is stationary, in other words it stays in the same space, so it has to create fields that are chaning in time, but in the same space. The embodiment in Fig. 18A. is such that it can not change flux of permanent magnets, and also such change of intensity of magnetic fields, when fields are expanding and then colapsing is not desirable state of fields, since the gradient of fields will not be at the maximum all the time. While magnet in Fig. 18A. or in Fig. 18B. which is the same magnet, can not change magnetic flux in time, it can change it in space, if it will be set in motion, in direction from back of the magnet towards tip also shown in Fig. 18B. When set in motion, such magnetic field will be constantly expanding relativly to the space around it, since magnetic flux of the magnet 1 in Fig. 18C. which is the same magnet as in Fig. 18B. expands from the tip towards the back of the magnet 1. The best form of motion is rotational motion, as already described in Fig. 6. with body 1 rotating.

Now the place of body 1 in shown in Fig. 6. will take the embodiment of magnet described in Fig. 18A. also the same form of magnet being shown in different view in Fig. 18B. and Fig.

18C. The next Fig. 21 is the result of having magnet from Fig. 18A. set in rotational motion around the center, in direction shown by the arrow 2, which is the clockwise direction. It is clear that magnetic field flux of magnet 1 in the Fig. 21. will expand in time while the magnet will rotate in space in clockwise direction 2 around the center shown in the same Fig. 21. The advantage of rotational motion is that is constantly accelerating, and that acceleration depends on the speed of the rotation and the radius of rotation, the greater they are, the greater acceleration will be achieved. Thus magnetic field flux of magnet 1 shown in Fig. 21. will look like constantly accelerating magnetic flux, similar to the greatest change of displacement shown in Fig. 2C. under the 90 degrees mark, which is the same as when antenna or condenser just powers up and creates the greatest thrust.

Since it is not practical to have only one rotating element, total number of four of such magnets with asymmtrical field is shown in device in Fig. 22. which consists of four legs handle 2, with rotating magnets 1 with asymmtrical magnetic field flux, and at the bottom of the magnets 1 are plates 3 wich is made of material of high permiabillity, and it rotates

clockwise. The device shown in Fig. 22. is basic form of antenna transmiting electromagnetical radiation, in such manner that magnetic fields look like constantly being accelerated at the highest rate. It is also the best solution to make magnetic fields look like constantly accelerating, which is imposible in closed AC (Altemating Current) systems, because AC amplitude can not constantly accelerate or grow, it has to reverse and to decrease. But by using device shown in Firuge 22. it will create constantly expanding magnetic field flux. Mechanical and electronic oscillating systems are symilar, as shown in Fig. s 1A., 1B., 1C, 2A. , 2B., 2C., and in 3A. , 3B. , 3C, where mechanical oscilations create waves in surrounding mediam like air, so they create sound waves, and electrical systems create electromagnetic waves. Similar to that, device in Fig. 22. will also create electromagnetic waves, but in different form that oscillating LC circuit shown in Fig. 1 B. because LC circuit is using AC oscillations, while device in Fig. 22. is using source of permanent magnetic field, like permanent magnet specially shaped to have asymmetrical magnetic flux, and all those permanent magnets are rotated so it appears they are producing constantly growing and expanding magnetic field in the surrounding space around them.

Using analogy in naming, and having as compared names sound waves created by mechanical device in Fig. 1A. and electromagnetic waves created by LC circuit in Fig. 1 B., the best name that will describe special form of electromagnetic waves created by device shown in Fig. 22. is Electromagnetic Wind, and the whole device shown in Fig. 22. named as Electromagnetic Propeler.

While device in Fig. 22. was set of four rotating magnets described in the embodiment in Fig. 17A. , other embodiments of magnet with asymmetrical fields as in<BR> Fig. 19A. , 20A. and prefered embodiment of shape of the rotating magnet is described in<BR> Fig. 18A. , 18B. and 18C.

Also, Electromagnetic Propeler described in Fig. 22. uses magnetic field to produce electromagnetic radiation. Electrical field can be used also, and it will be described in the next Fig. 23. The device in Fig. 23 is similar to the device in Fig. 22. in that it consists of holding structure 4, which has eight legs, and at the end of those legs are antennas with asymmetrical Electric field flux, which were described in Fig. 9A., 9B. , 10A., 10B., 10C.,<BR> 11A., 11B. 11C., 11D., 11E., 11F., 12., 13A. , 13B. and Fig. 14. The antennas shown in Fig.

23. are antena described in Fig. 11A. and 11B. There is set of six electrode plates 2 at the front end of antenna, which is perpendicular to the electrode 1 at the back of that antenna, and it might have dielectric 3 in between them. The whole device, with eight antennas on the

end of eight supporting legs is rotating in clockwise direction as shown by arrow. The set of six plates is charged with high voltage potential and that potential is opposite of the potential applied to the plate 1, as will be shown in Fig. 29, and according to the method shown in Fig. 8., where one plate is charged with positive and one perpendicular stick with negative potential, and that drawing was derived from Fig. 4. Also, all eight antennas shown in Fig. 23. are under the angle of fourthy five degrees in respect to the rotation. That is for the purpose of creating unidirectional thrust and it will be explained in Fig. 29.

The next Fig. 24. is drawing of the ring 1 in which device from Fig. 23. can be wrapped, in order to avoid resistance of the air while rotating. Area 2 in the Fig. 24. is the part with antennas shown on the ends of supporting legs in Fig. 23. and upper part, where 2 is pointing at the upper plate which is made of material which is transparent for electromagnetic radiation and yet it will not let air or other surrounding medium go through canal 2 where electric antenna, preferebly that described in Fig. 11A. and 11B. is located.

The solid body 3 is shown in dark color, and it is made of material with high dielectric constant in order to prevent interaction of Electrical fields between antennas located in the ring 1. The futher description of the ring will be given in Fig. 29.

The Fig. 25 is closer description of usage of the device in Fig. 22., and it is a sectionplane. The magnet 1 with asymmetrical magnetic fields 5 is hold by supporting leg 3, which has the same shape and function as supporting leg number 2 in Fig. 22. In the center of the Fig. 25. there is a motor 2, preferbly electric motor, which will rotate supporting legs 3 and the magnets 1 that are fixed at the end of the supporting legs. While Fig. 22. is shown without motor in the center, Fig. 25. is shown with motor which will generate mechanical power in order to rotate Electromagnetic Propeler, also the magnets 1 are in perpendicular position in respect to the plane of the rotation, while in Fig. 22. they are paralel to the plane of the rotation. The part 4 is metalic plate in circular form, and since Fig. 25. is sectionplan, the best look at it will be when looking from the bottom, as shown by element 1 in Fig. 26.

The element 4 in the Fig. 25. is the same as the element 1 in Fig. 26. The element 4 in the Fig. 25. is oblique in respect to magnet 1, in order to reflect electromagnetic field created by the passing by rotating magnet 1, and while reflecting it to created upward thrust shown by arrow which point to the direction of the Force created. The magnetic field lines 5 from the electromagnetic radiation of passing by magnet 1, will cut a conducting metalic plate 4 and create current in that plate which will counter the electromagnetic radiation from the magnet 1. Thus, electromagnetic radiation 5 of magnet 1 will have counter electromagnetic force

(Counter EMF) on its way, which will create unidirectional, upward force, shown by the arrow, and also electromagnetic radiation will be reflected downward in the process, as shown by electromagnetic radiation 6 on the Fig. 25.

The Fig. 27. represents the whole structure, or craft, which includes parts already shown in Fig. 25. and Fig. 26. The magnets 1 are again in the perpendicular position to the plane of their rotation, they are supported by legs 3, and they rest on the bearing 2, which is on the bottom 5 of the structure. The rounded cylinder is shown in element 9, and rounded metalic plate 4, in oblique shape, are also shown in Fig. 26. which is bottom view of the device in Fig. 27. There are three rounded cylinders in the device in Fig. 27., as shown in the Fig. 26. but only one is shown. The purpose of cylinders with rounded end is double, first to be used as lending legs, on which device will rest while on the ground, and also as housing for a motor 11, preferbly electric motor, which is supported to the housing cylinder 9 by holder 10. The motor 11 is producing mechanical power to rotate Electromagnetic Propeler 3 with magnets 1. The power from the motor 11 is transfered from the shaft 12 of the motor to the another shaft 7, and then to the round holder 6 which is hollow circle at the top in order to be connected to the shaft 7 through contact gear 8, and thus mechanical power is transfered from the motor 11 to the legs 3. The unidirectional thrust is created by the method of creating the upward Force already described in Fig. 25. The flow of electromagnetic radiation created by rotating magnets 1 is propagating not only towards the plate 4 from the magnets 1, but also towards magnets 1 through hollow space 20 between the walls, and also in the central canal 15 which is fixed to the top of the device with circular holder 16. The canal 15 is rounded, thin metalic stick 13 is in its center, but it is longer then cylindrical canal 15 and thus looks like antenna. The 19 is unvisible door which is the entrance to the room 18 which can be used for occupants inside the device, and the electromagnetic energy is passing around the door in the hollow space around it, which was shown by 20. Thus, electromagnetic radiation 14, also 21, is propagating towards the magnets, starting at the entry points at the top of the cylindrical canal 15, and also through entry point 17 which is circular shape, and also represents generator of electrical energy which is generated by the electromagnetic radiation on its way towards bottom of the device, to the magnets 1. Energy supplied by generator 17 can be used for internal needs for electric energy of the device. The biggest flow of incoming electromagnetic radiation 14 and 21 is throught cylindrical canal 15, and less through generators 17 that extract part of that energy before letting it go through hollow empty space 20, which is circular

since the whole device has round shape, as already shown in Fig. 26. The plate 22 is made of such material that is transparent to the flow of electromagnetic energy. The directionof the upward thrust extends along the longitudinal axis of this craft.

Fig. 28A. is device that uses rotating ring with asymmetrical antennas which was described in Fig. 23. and 24. The ring 1 in the Fig. 28A. has antennas which are hidden behind the wrapper 2 whose purpose is to protect antennas from the surrounding medium, like air or water, and yet to be transparent to the flow of the electromagnetic radiation. The dielectric body 3 is between each of the antenna, to protect them from the fields of high voltage that are supplied to the electrodes of the antenna, thus saving the intended shape of the electrical field gradient in each separate antenna. The whole device looks like two cupolas sticked together and with a rotating ring between them. The upper cupola 13 is solid and of even form, but is shown with cut in it in this drawing to show details inside the device.

At the lower part, which is in the space of lower cupola 10, there is a motor 4, preferbly electric motor, whose rotating shaft is transfering its power to through gears in the box 5 to the shaft 6 that goes upward towards the top of the upper cupola, and another shafts, one of them is shown in element 7. The shaft 7 is transfering its power throught gear 8 to the outside ring and makes it to rotate in clockwise direction. In the same time, shaft 6 is transfering its rotational power through contact 9 to the cupola 13 but in opposite direction of the rotation of the ring 1. The cupola rotates counter-clockwise, and ring with set of antennas rotates in clockwise direction, when looking from the top, so the sum of the rotational energy is zero, which allows interior of the device to be stationary, like room for the occupants of the craft, shown as number 14. In the lower cupola there is a door 11 for entrance to the craft, and the whole craft stands on the three struts 12 while on the ground. They are retracted when craft takes off, which will be explained later. The creating of upward thrust is done by rotating ring 1 with antennas with asymmetrical electric fields, which will create counter electromagnetic force (EMF) in the surrounding space which will make presure perpendicular to the surface of the antennas, and since angle of antennas is under the angle, the resulting thrust will be upwards, along the longitudinal axis of this craft. Futher explanation of upward, unidirectional thrust will be given in Fig. 29.

Fig. 28B. is simplified view on the craft shown in the Fig. 28A. The rotating ring is presented by element 1, upper cupola 2, then door 3 in the lower cupola, and three struts 4.

Fig. 29. describes the method of creating upward thrust, and elements of the

asymmetrical antenna. Antenna shown in the Fig. 29. is the same as antenna shown in Fig. 11A. and 11 B. The elements are the same for the antenna in Fig. 29. and that is six metalic plates 1, perpendicular to the electrode 2 and with dielectric material 3 between them. On both sides of the antenna there is a body 4 which is made dielectric material. The antenna is located inside the canal, and canal is under the angle of fourthy five degrees relativly to the ring and the direction of the rotation. At both ends of the canal there is plate 5 which is letting go through electromagnetic radiation created by antenna while it is in rotational motion, but will stop surrounding medium like air. The prefered material of plate 5 is such that will be also be transparent for the light radiation that will be created in the process, from the high voltage that is applied to the electrodes of the antenna. High voltage potential is applied to both electrodes, in drawing is shown that electrodes 1 are positive, and electrode 2 is negative, but it can be opposite, with electrode 1 having negative and electrode 2 positive potential. The potential applied to the electrodes is DC (Direct Current).

The upward Force is created when ring and antennas under high potential with it rotate, and create counter electromagnetic force (EMF) in the surrounding space. Because presure on the antenna from that counter EMF is always perpendicular to its surface, thus antenna has to be under the angle relativly to the direction of rotation so the net resulting of the Force will point upward, which is used for unidirectional thrust for the craft as shown in the Fig. 28A.

Fig. 30A. is yet another embodiment of the rotating ring shown in the Fig. 24., and Fig. 29. While canal in the ring described by the Fig. 29. is under the angle of fourthy five degrees only relativly to the direction of the rotation, the canal in the ring 2 in the Fig. 30A. is also under the same angle of fourthy five degrees relativly to the direction from the ring to the center of its rotation. In Fig. 30A. the part of the cupola 5 is shown, with elements on the ring like 1 being entrance to the canal for the electromagnetic radiation, 4 being exit of the canal, and the canal 3 inside of the ring. The antenna which is inside of the ring is not shown in this drawing, because it is the same as the antenna in Fig. 29. The best view this type of ring form in Fig. 30A. is shown in the sectionplan view of it in Fig. 30B. The cupola 5 is shown, with entrance 1 to the canal, exit 4 of the canal, and canal with number 3. The solid body 2 is part of the ring and it is dielectric. Arrows A and B shows that radius A for the entrance point 1 to the canal3 is shorter then exit point 4 which is radius B, thus having more acceleration force and as a result a greater upward thrust. Such form of ring with its canal being under the angle relativly to the two planes is generally thicker then the rings with canals under angle only to the one plane of the rotation.

The total upward thrust created by the rotation ring and its antennas depends on the speed of the rotation and also on the electric potential which is applied to the electrodes of the antenna, and on dielectric constant of the material that might be between the electrodes of the antenna. The greater those values are, the greater the upward thrust will be created. It is understandible that angle under which canal in rings is build can be fourthy five degrees, but it might be of different values.

Fig. 31 A. is one of the possible shapes of the craft with rotating ring, and the shape is round globe, with ring 2 and its exits from the canals 3, which devides the globe to the upper part 1 and lower part 4.

Fig. 31 B. is another variation in the shape of the cupola, having the same elements, rotating ring 2 with exits from the canals 3, and upper part of the craft being a cupola 1, and a lower cupola 4.

Fig. 31 C. is yet another variation, with upper cupola 1, and lower part of the craft 4 being almost flat, rotating ring 2 with exits from the canals 3. being a cupola 1, and a lower cupola 4.

Fig. 32A. is drawing of craft with rotating ring that looks like if it is in the fire. The reason for such intense light is that since the electric potential that is applied to the antennas in the ring is very high, preferbly around million of volts, the resulting electromagnetic radiation from the rotating ring will also be very high, and will ionize the air while the craft is in the lower parts of the atmospera near the surface.

Fig. 32B. is similar drawing but with the whole craft engulfed in the cloud of the ionized air, since electrical field lines tend to follow the surface of the body near them, and with tips at the top and bottom. Since electrical fields lines are concentrated on the sharp parts of body they encounter, if there are some cracks, bulges or details that stick out, they will be subject of violent attack from the strong electrical fields and might be destroyed. Thus prefered embodiment of the cupola on both lower and upper parts will be to have it as smooth as possible.

The above description of this new method and devices is only illustrative, since the devices build based on this novel method can be of wide variety of forms, shape, type of materials used, and it will fully transfer the essence and the scope of the invention to those skilled in the art.