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Book of Ra Tricks \u0026 Cheats for Free - vasnas.nuWann ist so ein Spiel durchgespielt für die Challenge hier? Super Mario Land. Du musst alle Bosse besiegen, der letzte ist King Dedede.

Da bin ich doch gerne auch dabei! Parodius Da! Wobei ich auch mit Master System zufrieden gewesen wäre und dann auch das gleiche Spiel zuerst durchgespielt hätte Die Schlümpfe.

Ich mache gleich mal weiter mit: King of the Zoo. Bubble Ghost hab heute das erste mal im leben bubble ghost ohne save states durchgespielt.

Hab mir Mickey's Dangerous Chase gegeben, sieht so harmlos aus, aber gegen Ende wird es doch recht knifflig! Leben sind rar und Continues gibts auch nicht, ab Stage 5 hab ich mir vorher lieber ein Playthrough angeschaut.

Balloon Kid eines meiner lieblingsspiele noch schnell hinterhergeschoben. Zuerst mal die ganz einfachen Double Dragon. Gameboy find ich klasse.

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Nemesis 2 Loops. Ich musste für eines der Level sogar YouTube bedienen, da man bei einem der Schweiz-Level Tresor in einer bestimmten Reihenfolge aufsprengen muss, aber es keinerlei Anhaltspunkt zu geben scheint, in welcher.

Wählt man die falsche muss man zum Beginn des Levels zurück und alle Tresortüren sind wieder zu, der Infrogamestypische Leveltimer beginnt jedoch nicht von neuem.

Positiv ist Grafik und Musik zu benennen, gerade ersteres ist wirklich sehr hübsch umgesetzt, wobei natürlich hier zusätzlich von der speziellen Portierung auf den GBC profitiert wurde, ist bei letztem die Musik zwar schön, aber bei einigen Sounds hat man die gleichen genommen, wie bei den Schlümpfen.

Während das Aufquiken bei einem erlittenen Treffer bei den blauen Hüpfern jedoch passend wirkte, ist es bei Obelix völlig Fehl am Platze.

Mein Fazit zum Spiel: Leider viel verpasstes Potential und ohne die Passwortfunktion, die bei der ansonsten spielerisch identischen GB-Version noch fehlte, hätte ich das Spiel wohl kaum durch gespielt.

Geniales Gameplay und fantastische Musik! Godzilla Den meisten gefällt es nicht, aber ich mochte es schon immer sehr.

Besonders auch die Musik. Made My Day XD erst jetzt gesehen wahr gerade am Kirby Dreamland durchzocken und hat schon jemand da muss ich mir jetzt ein anders Game einfallen lassen :D.

Orientier dich nicht zu sehr an der Liste, da kann durchaus mal ein Spiel durchrutschen. Letztere macht das Spiel natürlich deutlich leichter und dementsprechend könnte man hier durchaus sagen, dass die GB-Version extra zählt, aber gibt ja noch einige Spiele, bei denen dann wirklich nur die Farbe neu ist, die sollten nicht extra nochmal durchspielbar sein.

Dabei sind das doch komplett unterschiedliche Spiele, oder? Zelda: Link's Awakening DX wäre auch so ein Kandidat, wo hauptsächlich nur die Farbe hinzugefügt wurde, aber immerhin auch ein zusätzliches Dungeon.

Also man könnte die natürlich als ein einzelnes Spiel auffassen, andererseits wiederum sind das jeweils einzelne physische Veröffentlichungen.

Link so wie es aussieht sitzt Bastian schon dran. Abgesehen davon, wer schneller ist, trägt es ein. Ich nutze die Gelegenheit um endlich mal Gargoyles Quest durchzuspielen.

On nothing else. Notions as "spreading of interaction", "field. The unique mathematical conclusion, to which.

In other words the change of the local. We can write the electric and magnetic energies of the particle in the form.

I calr ' ' the expression on the right side of 8 the full potential force. It is. Newton who considered only a space energy. Obviously, if the time derivatives of the.

The time derivative of the magnetic potential can be written in the following form. On the left side we have the simple kinetic force of the current element I'dr' and.

An equation similar to 15 gives the simple kinetic force d df of the cur-. Considering dr as a constant vector, we can write 15 in the form of the so-cal-.

One would be able to aive a direct experimental verification of this formula if. Making then the connection of these. All authors assert that it. The simple kinetic forces of two interacting current elements are not equal.

So, for example, Pan of sky and. The result on the right side of 17 , can be obtained in three different way s:. Meanwhile if a.

Here singularities do not appear as the line element. Summing the kinetic forces of many consequent current elements one can calculate.

Formula 16 shows that these kine-. I shall elucidate the problem calculating the kinetic forces of the simple loops.

The size of the rectangle A'B'C'D' is taken twice the size of. The currents flow counterclockwise. The wires CD. Let us choose the sizes of the rectangles enough big and neglect.

According to the Biot-Savart formula 16 , the kinetic force of the current ele-. The indefinite integ-. The calculation by the help of formula 16 has led to a nonsensical result, name-.

The results obtained above can be checked experimentally very easily. Let us rea-. The n when letting currents. The size of the bulge can be.

Indeed, in such a case the kinetic force of the current element I'dr',. Ampere did not give a clear and logical deduction of his formula from the i-n-.

Maxwell knew the exact form of the Newton-Lorentz equation , which unjustly. The motivation is that both formulas lead to identical results for.

Recently this was shown by Ly-. But for the action of a current element on a closed loop both for-. The answer is that nobody has been able to measure.

Ampere and Biot-Savart forces - S. We accordingly attempt to construct. This in turn compels us to assume that the energy of the system of.

Being unable to explain such a simple thing as the interaction of stationary cur-. The Ampere and any other formula. The interaction between current elements, as well as the inte-.

Ionian sense and all hypotheses about a "propagation of interaction", "transmission. As I said, if one calculates the action of a closed loop on a current element,.

Ampere formula one must take into account that the repulsive action of the wire a. E'A' -2a. The whole calculation is a tedious mathematical problem and I have not.

According to me, one has to. The physical explanation is to be given only by considering the interaction. I shall give a confirmation of this assertion analysing the first electromagnetic.

If an electric current flows downwards. In Ref. The torque of all. The rotation of the magnet is due to the Biot-Savart forces originated by the current.

The forces are the. A magnet, on whose "south bottom" a piece of platinum is fasten so that it can swim. In this experiment again the rotation is due to the action of the cur-.

The electrons streaming in the mercury. The conclusion is: there is no action of the magnetic field on the "poles" of a mag-.

The interaction is al way s "point-to-point" interaction between the current ele-. If we suppose that the visbsity of the. The theoretical explanation of the experiment shown in fig.

Faraday's experiment by the schematical drawing in fig. The circular loop AB and. The loop BCFE is drawn only for symmetry.

Let us consider the interaction of the circular horizontal loop AB with the vertical. So if making the contacts at points A, C and D sliding,.

For definiteness , I call the rotation of a copper disk in the field of a cylin-. However, mankind. I shall give here. In fig. In this. The point C of the radial wire is connected with a metal cylinder.

Both metal. The whole system represents a rigid body. A synchro-. The apparatus works in two stages. First fig. The n fig. The magnetic interaction between the currents in the cir-.

The n one repeats both steps and the whole rigid system comes into a con-. Electromagnetic energy is consumed for covering of the Ohmic. The above consideration is valid when the inductance L of the system is practi-.

Now the chopper must operate with a. The driving rotational moment is proportional to the capacitance. Maybe, for small periods T.

If the outcome of the experiment shown in fig. According to Maxwell, during the char-. We see that the negative outcome of this experiment can be considered as a.

Of course in the case of a negative outcome of the experiment one has to make an. The experiment consisted of two. Its description is as follows fig.

The wire is suspended by thin threads. Current from. As the kinetic forces of any of the legs are equal. Thus the kinetic force of the shoulder will be take into account that there are.

In table 1 I give certain of the forces measured by Pappas and the calculated by me. Thus there is no an "interaction" which propagates.

The re are only electrons. It must be clear that the velocity of the single electrons is neither the. Any electron moves. It is possible that some of the supplied surplus electrons may cover the.

The same type of a current conducting spiral fig. I showed that human ignorance about the interaction of electric currents is cata-. The followers of Einstein have a large deal of responsibility for this ignorance.

The theories which are given such prominence in scientific and general literature. This effect, first, is known to a. The history of the discovery of the ball-bearing motor represents rather a curiosity.

In I was imprisoned in a psychiatry in S of ia and cured by horse doses of. In the psychiatry. He has earned good money and, evidently, the.

Milroy describes the effect without giving. Thus the ball-bearing motor is a. The re is, however, another. Only this small "contact part" of the ball dilatates and the dilatation.

As the balls and the races are made of a very. At the new contact, when again current passes. Thus, as a result of the mechanical motion, the.

The whole heat. If the. The n I started the motor and applied. According to the energy conservation law,asinboth cases the same amount of.

The temperature increase in the second case was with. Even if the friction of the ball-bearing motor is very low let us assume zero ,.

At this maximum. Tir, where r is the. Such an apparatus had no torque. Another pro of is. Currents even of A.

The ball-bearing motor has a higher efficiency at the following conditions:. Pappas, P. Aspden, H. Pan of sky, W. Classical Electricity and Magnetism Wesley Publ.

Jeans, J. The mathematical theory of electricity and magnetism Cambridge,. Pappas 1. The force FJ. Proceeding from the axiomatics of my absolute space-time theory, I derive.

I present the description and the ex-. The analysis. I make a new systematization of the dc machines, calling the unipolar.

The n I describe the closed half polar and the unipolar machines inven-. I invented two types of unipolar machines: with magnets. The present paper shows clearly that one must.

One must be careful when. The terminology and symbolism which we use in physics sometimes deviate from. Thus we can present the "total" time derivative of the magnetic potential as fol-.

In my theory, the equation of motion of the test particle 1 or 5 , or 6 is. The equation of motion considered in a laboratory which. Lorentz equation.

The latter is to be used when observing the motion of an electric. Thus let us suppose that the velocities of the test charge and of the charges of.

If working with a higher accuracy i. For the. Lorentz invariance there is a change in the momentum and energy of the observed par-.

For the theory of relativity it is of no significance whe-. The "total" time derivatives of the absolute and relative magnetic potentials.

Comparing formulas 5 and 10 , we see that the "potential" i. Later I shall show the reasons for which. Indeed, the last term in formula 10 shows clearly that the V-vector-gradient of.

The results 14 and 15 are not identical. Meanwhile, as it can be easily seen ,. The above analysis leads to another extremely important conclusion.

The value of. However the value of the magnetic potential at a certain. The reader sees clearly that at the light of these conclusions.

I showed that the existence of the term q v. In front of these decisive experiments, the followers of Einstein try to save the relativity.

I showed for the first time, measuring the Earth's absolute velocity in a closed laboratory. The se objections, however, are raised al way s. The magnitude.

The most interesting. The present paper is dedicated only to basic problems in electromagnetism. I shall. Some of these machines lead to violation.

Concerning the violation of the energy. Before giving a simple verification of the above assertion, let me note that the. As I showed , although the so-called "drift.

The magnetic field is originated by the energy velocity of the. I must emphasize, however,. As announced by N. Rudakov , an amount of several million dollars has been paid for.

If the number of elec-. Let us now have a system of closed wires loops along any of which a constant elec-.

On the left side of equation 16 we have the kinetic force of the electric charge. The term "motional -transformer induction" is introduced.

The calculation of the motional induction can be done directly by formula Thus for the case of the motional -transformer in-. The calculation with formula 19' is difficult and only in simple cases can be car-.

Now I shall give a very simple and clear example for the use of formula 19'] which. Substituting now 23 into. If the loop rotates about an axis which is not an axis of rotational symmetry of.

This tension, however, is al way s alternating and the average tension for a whole rota-. The demonstration of this more general theorem is.

Thus if a loop rotates together with a cylindrical magnet about the axis of the lat-. Let me cite the. The dispro of of the movinq-line theory is thus completed; electromagnetic in-.

He reali-. It is evident in the light of equation 24 that one cannot make Kennard's motio-. However, if one lets a certain part of.

Such was the case of a copper disk rotating together with a cylindrical. The relevant experiment was done 75 years before. J copper disk was cemented upon the end of a cylinder magnet with paper.

The galvanometer needle moved and. Hence, rotating the magnet causes no. Let us have a wire imagine al way s for simplicity a wire's line element and a cur-.

Taking a rotation from both sides of the definition equality for the electric intensity. The motion of the valence electrons with respect to the wire under the action of the.

Coulomb , motional , and transformer electric tensions. The tenand. The terminology and symbolism in physics are of high importance for understanding.

If considering. The tragedy is that in the system of units SI one introduced the highly perni-. Now I shall explain the physical essence of the electromotive effect due to the.

If there is no magnetic field but our unclosed wire is under the action of chemical,. The tensions are. As in equation 16 , also in the last equation,.

But I am afraid, nobody understands all aspects of the difference between tension and. We know that the interaction of the electrons in a wire closed or unclosed, along.

The explanation of the ponderomotive effect due to the Coulomb intensity is commonly. Another special case of a ponderomotive effect due to no one of the potential forces.

I called this effect the "current jet" effect. The same effect forr elec-. The Hall. The sum of these two forces will be balan-. I have met nowhere in the literature this explanation of the ponde-.

The causes are exactly the same, the results. The essence of the mechano-braking effect was revealed by Lenz in the early era of. The motor Lenz rule can be formulated in a similar manner: The current induced by a.

The physical explanation of the generator Lenz rule is the following: In any elec-. The se valence electrons mo-. However, if the extremities are closed.

Now the. The appearing potential difference. The physical explanation of the motor Lenz rule is the following: In any electro-.

The se cur-. The motion of the wire leads to the appearance of a convection. Now the electrons. I observed section 13 a violation of the generator Lenz rule in the cemented Faraday.

This signifies that for the Faraday disk the left side of equation Thus I presume. The description of the Barlow disk is given in the next section.

The uncemented Faraday disk is shown in fig. The copper disk 1 is solidly attached to the axle which can rotate.

Its magnet 2 and the yoke 3 are solid to the laboratory. The copper disk 4 is solid to its magnet 5 and both are. If the polarization of the magnets and the ro-.

If current should be sent along the radii of the disks 1 and 4, they will begin to. The cemented and uncemented Faraday and Barlow disks have been constructed in the.

Recently Das Gupta. The effect in the Barlow disk can easily be explained in a manner similar as in. When, however, the disk is homogeneous,. The big surprise comes, however, from the fact observed first by Bruce de Pal-.

On the. The bul-cub machine is a generator and motor for direct current with many windings. The scheme of the machine is shown in fig.

The position corresponds to the position of. The bul-cub machine consists of a cylindrical magnet I had an electromagnet but a. The coil's wires between the marginal points p and q resp.

I showed that the rotation of a cylindrical magnet about its axis is irrelevant with. Thus, as the rotation of the cylindrical magnet.

In this section I shall consider the generator aspects of the bul-cub machine and in. I shall calculate the tensi ore induced in the different wires.

If looking at figs. Magneto-yoke at rest, coil rotating. The following motional inductive electric. The average inductive electric intensity along.

Let us assume that the cross-section of the yoke is rectangular with a side s pa-. If n wires pass through a unit of length on the circumfe-. However, the distribution of the inductive intensities.

The explanation of the electro-. Speaking about the problems. The present eruption will be tremendous. I think, however, that concerning the general.

As an example I shall look at the "seat" of the motional -transformer induction in. For completeness. The sign "o" signifies.

The sign "Q" signifies that the respective element rotates moves and the. Thus I shall give here only a simplified calculation of the motional -transformer.

The tensions induced along the wires cd jji and outside can be calculated exactly in. I repeat, this numerical equality of the. Another method of non-contact short.

The most. For comparison it is to be noted that al-. As the rotation of the cylindrical pole is immaterial, we have to. Proceeding from the fundamental equation 16 , where.

The moments of force with respect to the coil's axis, applied to a unit of length. For the average moment of force, applied to the wires ab,.

As the length of the wires ab is twice the length of. The n, according to the integral Biot-Savart formula , we conclude.

Thus the moment of force acting on the magneto-yoke when it has a possibility. The bul-cub motor will become effective if we short-circuit the windings passing either.

I called "core" the magnetic material s of t iron in the coil which closes the mag-. Until now the core was supposed to be solidly connec-.

Let us now suppose that the core has a rotational degree of freedom. The coil will be supposed solid. Of course, the magnet can be.

As many times noted, the rotation or rest of the cylindri-. The yoke rotates on the two small ball-bearings on the left side of the figure.

The outer rings of the big ball-bearings on the right side. The force acting on a magnetic pole is the pro-. If a magnetic monopole will be put in the inner space.

The core in fig. This conclusion, however, is wrong. The core cannot be set in rotation. One comes. But the coil acts on the.

To consider the action. The right consideration is as in the. I dedicated so much attention to the analysis of the bul-cub machine with a rota-.

The notion "pale" is simply a mnemotechnical tool. I should like. However, it is much more difficult to present graphically the magnetic action of the.

Conventional electromagnetism knows only two types of dc electromagnetic machines:. Besides the half polar machines executed in the form of Faraday and Barlow disks,.

The closed half polar machines, which. If at the place of the conducting ring we shall. Now the centers of the circular magnet's currents do not lie on.

The unipolar as well the bipolar machines. In the unipolar machines a direct current is flowing in the wires of the. The sliding brushes are used not for commutation.

The wires ab are called. The open. Swill become closed if the north and south poles of any. The most simple closed unipolar machine.

The difference between the half-polar closed machine in fig. The unique unipolar machine which I found described in the literature is by Fukai.

The author calculates and. The magnets arranged radially in fig. Francisco Mliller has investigated the unipolar generators made with this ring.

IC ab is the active wire and cd is the passive wire. The passive wire. The unipolar machine with a Mliller ring gives a very patent experimental confirma-.

Newton's third law at the interaction of current elements. To show this clearly, I. Generator: The re is a motional induction in the wire ab.

It must be noted see. Motor: The current wire ab is moved by the pole. It must be noted see fig. Savart formula 16 in ref. Generator: The effect remains the same as in the case 1 as the rotation of the.

Mliller ring does not introduce any change in the character of the currents interac-. In the opposite kind of motion, however, i. In table 3 I give a systematic presentation of all types of dc machines and of.

The experiment of Feilitzsch can be arranged in the class of. One can establish that the torque on the magnets in the. Ipr vice versa is possible only if a part of the axle is solid to the magnet and a.

One can easily explain the rotation of the cylindrical conductor in Fei-. Another important cylindric of ilar experiment which represents a certain variation.

The trough Q' and the magnets are solid to the vertical axle G, which is immersed. The current flows from the positive electrode of the battery,.

At this direction of. According to conventional electromagnetism see also p. The Kdnig-Martnov machine consists of two brass cylindrical conductors which are.

The magnet is mounted on both cylindrical conductors. The magnet consists of an in-. The se two. The right disk has a gap in. If the gap is as in fig.

The body. The current comes from the po-. A magnetic field is originated by the cylindrical conductor. The apparatus in fig. I showed the machine from fig.

If the prediction of a. The re will be no mo-. The seat of the electromotive and ponderomotive forces.

I shall shortly return to certain of those experiments and bring more light to the. The era of electromagnetism was heralded by the experiment of Oersted carried out.

I am afraid conven-. I shall call the plane of the fi-. In the figure the. The currents at the edges A and B point. The magnet can be brought to rotation about any other ver-.

The diagram in fig, 16 explains why there is no torque on the. Thus if we assume that the friction between the molecules of the mercury is big-.

The short axle e. At this direction of the current the magnets rotate counter-clockwise. This supposition is not true.

The magnets will. To be able to clearly demonstrate the seats of the electromotive and ponderomotive. The machine has three parts which can rotate.

The yoke rotates on the first and. The current when the machine. The bars can be made. The bars can be made solid to the disk by the help of the plastic "cap".

The disk can. The effects. Thus the tales about the "force lines". Indeed, in the first case the motionaltransformer.

The same eddy currents and braking of. Although the magnetic interactions of current elements violate Newton's third law,.

However, a violation of the energy conservation law at the electromagnetic interactions. The whole magnet can rotate about the.

Let the moment of inertia of any. At a disconnected circuit i. Supposing that the law of energy conservation is valid, we can write the following.

The energetic aspect of this experiment is exactly the same as of inelastic collision. In our experiment, however, there is no interaction between disk 1 and disk 2.

The interaction. The physical causes for. The re is also the question whether the cemented Barlow disk has an electro-resis-.

Motor", the Germans had invented such a motor during. The current on the inside end of the spiral goes into the. The tensions.

My coupled N-machine was a slight variation of the scheme shown in fig. Instead of one, I put 16 sliding contacts on the.

The carbon brushs sliding on the rim of disk 4 in fig. The n I started the apparatus. The apparatus stopped in 32 sec. This 2-second diffe-.

The experiment was not firmly convincing, as I had no tachymeter and the initial. The n a short switching of f of the current feeding the elec-.

This was a clear evi-. Barlow disk may be less than this one which is prescribed by formula The first.

The cemented Faraday disk, which has two permanent ring magnets, is above, the Ko-. The polarities, of course, can be reversed:. The electromagnet.

The yoke of the Kbnig-Mari-. All details of the machine have been coppered and then golded. The n the mercury. It was better to cover parts of the details having.

The resistance of the whole machine was about. The resistance was measured by sending current through the machine and. The n taking out the rotor and making short circuit between the electrodes,.

The resistance of the short-circuited machine was the sum of. The short-circuiting can. One makes the tension Up pro-.

The best relation is. However, my measurements showed that the machine ADAM violated the law of energy.

I established this in the following way : I measured the braking times. According to the energy conservation. The experiment, however, has not confirmed.

I made two Faraday disks: one of solid metal and one of mercury poured. The Faraday and Kbnig-Marinov generators coupled with the ball-bearing.

As the ball-bearing.

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Super Mario Land. Du musst alle Bosse besiegen, der letzte ist King Dedede. Da bin ich doch gerne auch dabei! Parodius Da! Wobei ich auch mit Master System zufrieden gewesen wäre und dann auch das gleiche Spiel zuerst durchgespielt hätte Die Schlümpfe.

Ich mache gleich mal weiter mit: King of the Zoo. Bubble Ghost hab heute das erste mal im leben bubble ghost ohne save states durchgespielt.

Hab mir Mickey's Dangerous Chase gegeben, sieht so harmlos aus, aber gegen Ende wird es doch recht knifflig! Leben sind rar und Continues gibts auch nicht, ab Stage 5 hab ich mir vorher lieber ein Playthrough angeschaut.

Balloon Kid eines meiner lieblingsspiele noch schnell hinterhergeschoben. Zuerst mal die ganz einfachen Double Dragon.

Gameboy find ich klasse. Und gleich weiter im Doppelpack: Double Dragon 2. Los gehts mit Kirbys Dreamland.

Kung Fu Master aka Spartan X sehr kurz und leicht, aber immer wieder gut. Nemesis 2 Loops. Ich musste für eines der Level sogar YouTube bedienen, da man bei einem der Schweiz-Level Tresor in einer bestimmten Reihenfolge aufsprengen muss, aber es keinerlei Anhaltspunkt zu geben scheint, in welcher.

Wählt man die falsche muss man zum Beginn des Levels zurück und alle Tresortüren sind wieder zu, der Infrogamestypische Leveltimer beginnt jedoch nicht von neuem.

Positiv ist Grafik und Musik zu benennen, gerade ersteres ist wirklich sehr hübsch umgesetzt, wobei natürlich hier zusätzlich von der speziellen Portierung auf den GBC profitiert wurde, ist bei letztem die Musik zwar schön, aber bei einigen Sounds hat man die gleichen genommen, wie bei den Schlümpfen.

I shall give a confirmation of this assertion analysing the first electromagnetic. If an electric current flows downwards. In Ref.

The torque of all. The rotation of the magnet is due to the Biot-Savart forces originated by the current. The forces are the. A magnet, on whose "south bottom" a piece of platinum is fasten so that it can swim.

In this experiment again the rotation is due to the action of the cur-. The electrons streaming in the mercury. The conclusion is: there is no action of the magnetic field on the "poles" of a mag-.

The interaction is al way s "point-to-point" interaction between the current ele-. If we suppose that the visbsity of the. The theoretical explanation of the experiment shown in fig.

Faraday's experiment by the schematical drawing in fig. The circular loop AB and. The loop BCFE is drawn only for symmetry.

Let us consider the interaction of the circular horizontal loop AB with the vertical. So if making the contacts at points A, C and D sliding,.

For definiteness , I call the rotation of a copper disk in the field of a cylin-. However, mankind. I shall give here.

In fig. In this. The point C of the radial wire is connected with a metal cylinder. Both metal. The whole system represents a rigid body.

A synchro-. The apparatus works in two stages. First fig. The n fig. The magnetic interaction between the currents in the cir-.

The n one repeats both steps and the whole rigid system comes into a con-. Electromagnetic energy is consumed for covering of the Ohmic.

The above consideration is valid when the inductance L of the system is practi-. Now the chopper must operate with a. The driving rotational moment is proportional to the capacitance.

Maybe, for small periods T. If the outcome of the experiment shown in fig. According to Maxwell, during the char-.

We see that the negative outcome of this experiment can be considered as a. Of course in the case of a negative outcome of the experiment one has to make an.

The experiment consisted of two. Its description is as follows fig. The wire is suspended by thin threads. Current from. As the kinetic forces of any of the legs are equal.

Thus the kinetic force of the shoulder will be take into account that there are. In table 1 I give certain of the forces measured by Pappas and the calculated by me.

Thus there is no an "interaction" which propagates. The re are only electrons. It must be clear that the velocity of the single electrons is neither the.

Any electron moves. It is possible that some of the supplied surplus electrons may cover the. The same type of a current conducting spiral fig.

I showed that human ignorance about the interaction of electric currents is cata-. The followers of Einstein have a large deal of responsibility for this ignorance.

The theories which are given such prominence in scientific and general literature. This effect, first, is known to a. The history of the discovery of the ball-bearing motor represents rather a curiosity.

In I was imprisoned in a psychiatry in S of ia and cured by horse doses of. In the psychiatry. He has earned good money and, evidently, the.

Milroy describes the effect without giving. Thus the ball-bearing motor is a. The re is, however, another. Only this small "contact part" of the ball dilatates and the dilatation.

As the balls and the races are made of a very. At the new contact, when again current passes. Thus, as a result of the mechanical motion, the. The whole heat.

If the. The n I started the motor and applied. According to the energy conservation law,asinboth cases the same amount of.

The temperature increase in the second case was with. Even if the friction of the ball-bearing motor is very low let us assume zero ,. At this maximum.

Tir, where r is the. Such an apparatus had no torque. Another pro of is. Currents even of A. The ball-bearing motor has a higher efficiency at the following conditions:.

Pappas, P. Aspden, H. Pan of sky, W. Classical Electricity and Magnetism Wesley Publ. Jeans, J. The mathematical theory of electricity and magnetism Cambridge,.

Pappas 1. The force FJ. Proceeding from the axiomatics of my absolute space-time theory, I derive. I present the description and the ex-. The analysis.

I make a new systematization of the dc machines, calling the unipolar. The n I describe the closed half polar and the unipolar machines inven-.

I invented two types of unipolar machines: with magnets. The present paper shows clearly that one must. One must be careful when. The terminology and symbolism which we use in physics sometimes deviate from.

Thus we can present the "total" time derivative of the magnetic potential as fol-. In my theory, the equation of motion of the test particle 1 or 5 , or 6 is.

The equation of motion considered in a laboratory which. Lorentz equation. The latter is to be used when observing the motion of an electric.

Thus let us suppose that the velocities of the test charge and of the charges of. If working with a higher accuracy i. For the.

Lorentz invariance there is a change in the momentum and energy of the observed par-. For the theory of relativity it is of no significance whe-.

The "total" time derivatives of the absolute and relative magnetic potentials. Comparing formulas 5 and 10 , we see that the "potential" i.

Later I shall show the reasons for which. Indeed, the last term in formula 10 shows clearly that the V-vector-gradient of.

The results 14 and 15 are not identical. Meanwhile, as it can be easily seen ,. The above analysis leads to another extremely important conclusion.

The value of. However the value of the magnetic potential at a certain. The reader sees clearly that at the light of these conclusions.

I showed that the existence of the term q v. In front of these decisive experiments, the followers of Einstein try to save the relativity. I showed for the first time, measuring the Earth's absolute velocity in a closed laboratory.

The se objections, however, are raised al way s. The magnitude. The most interesting. The present paper is dedicated only to basic problems in electromagnetism.

I shall. Some of these machines lead to violation. Concerning the violation of the energy. Before giving a simple verification of the above assertion, let me note that the.

As I showed , although the so-called "drift. The magnetic field is originated by the energy velocity of the. I must emphasize, however,.

As announced by N. Rudakov , an amount of several million dollars has been paid for. If the number of elec-.

Let us now have a system of closed wires loops along any of which a constant elec-. On the left side of equation 16 we have the kinetic force of the electric charge.

The term "motional -transformer induction" is introduced. The calculation of the motional induction can be done directly by formula Thus for the case of the motional -transformer in-.

The calculation with formula 19' is difficult and only in simple cases can be car-. Now I shall give a very simple and clear example for the use of formula 19'] which.

Substituting now 23 into. If the loop rotates about an axis which is not an axis of rotational symmetry of. This tension, however, is al way s alternating and the average tension for a whole rota-.

The demonstration of this more general theorem is. Thus if a loop rotates together with a cylindrical magnet about the axis of the lat-.

Let me cite the. The dispro of of the movinq-line theory is thus completed; electromagnetic in-. He reali-. It is evident in the light of equation 24 that one cannot make Kennard's motio-.

However, if one lets a certain part of. Such was the case of a copper disk rotating together with a cylindrical.

The relevant experiment was done 75 years before. J copper disk was cemented upon the end of a cylinder magnet with paper. The galvanometer needle moved and.

Hence, rotating the magnet causes no. Let us have a wire imagine al way s for simplicity a wire's line element and a cur-.

Taking a rotation from both sides of the definition equality for the electric intensity. The motion of the valence electrons with respect to the wire under the action of the.

Coulomb , motional , and transformer electric tensions. The tenand. The terminology and symbolism in physics are of high importance for understanding.

If considering. The tragedy is that in the system of units SI one introduced the highly perni-. Now I shall explain the physical essence of the electromotive effect due to the.

If there is no magnetic field but our unclosed wire is under the action of chemical,. The tensions are. As in equation 16 , also in the last equation,.

But I am afraid, nobody understands all aspects of the difference between tension and. We know that the interaction of the electrons in a wire closed or unclosed, along.

The explanation of the ponderomotive effect due to the Coulomb intensity is commonly. Another special case of a ponderomotive effect due to no one of the potential forces.

I called this effect the "current jet" effect. The same effect forr elec-. The Hall. The sum of these two forces will be balan-. I have met nowhere in the literature this explanation of the ponde-.

The causes are exactly the same, the results. The essence of the mechano-braking effect was revealed by Lenz in the early era of. The motor Lenz rule can be formulated in a similar manner: The current induced by a.

The physical explanation of the generator Lenz rule is the following: In any elec-. The se valence electrons mo-. However, if the extremities are closed.

Now the. The appearing potential difference. The physical explanation of the motor Lenz rule is the following: In any electro-.

The se cur-. The motion of the wire leads to the appearance of a convection. Now the electrons. I observed section 13 a violation of the generator Lenz rule in the cemented Faraday.

This signifies that for the Faraday disk the left side of equation Thus I presume. The description of the Barlow disk is given in the next section.

The uncemented Faraday disk is shown in fig. The copper disk 1 is solidly attached to the axle which can rotate. Its magnet 2 and the yoke 3 are solid to the laboratory.

The copper disk 4 is solid to its magnet 5 and both are. If the polarization of the magnets and the ro-. If current should be sent along the radii of the disks 1 and 4, they will begin to.

The cemented and uncemented Faraday and Barlow disks have been constructed in the. Recently Das Gupta. The effect in the Barlow disk can easily be explained in a manner similar as in.

When, however, the disk is homogeneous,. The big surprise comes, however, from the fact observed first by Bruce de Pal-. On the. The bul-cub machine is a generator and motor for direct current with many windings.

The scheme of the machine is shown in fig. The position corresponds to the position of. The bul-cub machine consists of a cylindrical magnet I had an electromagnet but a.

The coil's wires between the marginal points p and q resp. I showed that the rotation of a cylindrical magnet about its axis is irrelevant with.

Thus, as the rotation of the cylindrical magnet. In this section I shall consider the generator aspects of the bul-cub machine and in.

I shall calculate the tensi ore induced in the different wires. If looking at figs. Magneto-yoke at rest, coil rotating. The following motional inductive electric.

The average inductive electric intensity along. Let us assume that the cross-section of the yoke is rectangular with a side s pa-.

If n wires pass through a unit of length on the circumfe-. However, the distribution of the inductive intensities. The explanation of the electro-. Speaking about the problems.

The present eruption will be tremendous. I think, however, that concerning the general. As an example I shall look at the "seat" of the motional -transformer induction in.

For completeness. The sign "o" signifies. The sign "Q" signifies that the respective element rotates moves and the. Thus I shall give here only a simplified calculation of the motional -transformer.

The tensions induced along the wires cd jji and outside can be calculated exactly in. I repeat, this numerical equality of the. Another method of non-contact short.

The most. For comparison it is to be noted that al-. As the rotation of the cylindrical pole is immaterial, we have to.

Proceeding from the fundamental equation 16 , where. The moments of force with respect to the coil's axis, applied to a unit of length.

For the average moment of force, applied to the wires ab,. As the length of the wires ab is twice the length of. The n, according to the integral Biot-Savart formula , we conclude.

Thus the moment of force acting on the magneto-yoke when it has a possibility. The bul-cub motor will become effective if we short-circuit the windings passing either.

I called "core" the magnetic material s of t iron in the coil which closes the mag-. Until now the core was supposed to be solidly connec-. Let us now suppose that the core has a rotational degree of freedom.

The coil will be supposed solid. Of course, the magnet can be. As many times noted, the rotation or rest of the cylindri-. The yoke rotates on the two small ball-bearings on the left side of the figure.

The outer rings of the big ball-bearings on the right side. The force acting on a magnetic pole is the pro-. If a magnetic monopole will be put in the inner space.

The core in fig. This conclusion, however, is wrong. The core cannot be set in rotation. One comes. But the coil acts on the. To consider the action.

The right consideration is as in the. I dedicated so much attention to the analysis of the bul-cub machine with a rota-. The notion "pale" is simply a mnemotechnical tool.

I should like. However, it is much more difficult to present graphically the magnetic action of the. Conventional electromagnetism knows only two types of dc electromagnetic machines:.

Besides the half polar machines executed in the form of Faraday and Barlow disks,. The closed half polar machines, which. If at the place of the conducting ring we shall.

Now the centers of the circular magnet's currents do not lie on. The unipolar as well the bipolar machines.

In the unipolar machines a direct current is flowing in the wires of the. The sliding brushes are used not for commutation.

The wires ab are called. The open. Swill become closed if the north and south poles of any. The most simple closed unipolar machine. The difference between the half-polar closed machine in fig.

The unique unipolar machine which I found described in the literature is by Fukai. The author calculates and. The magnets arranged radially in fig.

Francisco Mliller has investigated the unipolar generators made with this ring. IC ab is the active wire and cd is the passive wire. The passive wire.

The unipolar machine with a Mliller ring gives a very patent experimental confirma-. Newton's third law at the interaction of current elements.

To show this clearly, I. Generator: The re is a motional induction in the wire ab. It must be noted see. Motor: The current wire ab is moved by the pole.

It must be noted see fig. Savart formula 16 in ref. Generator: The effect remains the same as in the case 1 as the rotation of the.

Mliller ring does not introduce any change in the character of the currents interac-. In the opposite kind of motion, however, i. In table 3 I give a systematic presentation of all types of dc machines and of.

The experiment of Feilitzsch can be arranged in the class of. One can establish that the torque on the magnets in the. Ipr vice versa is possible only if a part of the axle is solid to the magnet and a.

One can easily explain the rotation of the cylindrical conductor in Fei-. Another important cylindric of ilar experiment which represents a certain variation.

The trough Q' and the magnets are solid to the vertical axle G, which is immersed. The current flows from the positive electrode of the battery,.

At this direction of. According to conventional electromagnetism see also p. The Kdnig-Martnov machine consists of two brass cylindrical conductors which are.

The magnet is mounted on both cylindrical conductors. The magnet consists of an in-. The se two.

The right disk has a gap in. If the gap is as in fig. The body. The current comes from the po-. A magnetic field is originated by the cylindrical conductor.

The apparatus in fig. I showed the machine from fig. If the prediction of a. The re will be no mo-. The seat of the electromotive and ponderomotive forces.

I shall shortly return to certain of those experiments and bring more light to the. The era of electromagnetism was heralded by the experiment of Oersted carried out.

I am afraid conven-. I shall call the plane of the fi-. In the figure the. The currents at the edges A and B point.

The magnet can be brought to rotation about any other ver-. The diagram in fig, 16 explains why there is no torque on the.

Thus if we assume that the friction between the molecules of the mercury is big-. The short axle e. At this direction of the current the magnets rotate counter-clockwise.

This supposition is not true. The magnets will. To be able to clearly demonstrate the seats of the electromotive and ponderomotive. The machine has three parts which can rotate.

The yoke rotates on the first and. The current when the machine. The bars can be made. The bars can be made solid to the disk by the help of the plastic "cap".

The disk can. The effects. Thus the tales about the "force lines". Indeed, in the first case the motionaltransformer. The same eddy currents and braking of.

Although the magnetic interactions of current elements violate Newton's third law,. However, a violation of the energy conservation law at the electromagnetic interactions.

The whole magnet can rotate about the. Let the moment of inertia of any. At a disconnected circuit i. Supposing that the law of energy conservation is valid, we can write the following.

The energetic aspect of this experiment is exactly the same as of inelastic collision. In our experiment, however, there is no interaction between disk 1 and disk 2.

The interaction. The physical causes for. The re is also the question whether the cemented Barlow disk has an electro-resis-.

Motor", the Germans had invented such a motor during. The current on the inside end of the spiral goes into the. The tensions. My coupled N-machine was a slight variation of the scheme shown in fig.

Instead of one, I put 16 sliding contacts on the. The carbon brushs sliding on the rim of disk 4 in fig. The n I started the apparatus.

The apparatus stopped in 32 sec. This 2-second diffe-. The experiment was not firmly convincing, as I had no tachymeter and the initial.

The n a short switching of f of the current feeding the elec-. This was a clear evi-. Barlow disk may be less than this one which is prescribed by formula The first.

The cemented Faraday disk, which has two permanent ring magnets, is above, the Ko-. The polarities, of course, can be reversed:. The electromagnet.

The yoke of the Kbnig-Mari-. All details of the machine have been coppered and then golded. The n the mercury. It was better to cover parts of the details having.

The resistance of the whole machine was about. The resistance was measured by sending current through the machine and.

The n taking out the rotor and making short circuit between the electrodes,. The resistance of the short-circuited machine was the sum of. The short-circuiting can.

One makes the tension Up pro-. The best relation is. However, my measurements showed that the machine ADAM violated the law of energy.

I established this in the following way : I measured the braking times. According to the energy conservation. The experiment, however, has not confirmed.

I made two Faraday disks: one of solid metal and one of mercury poured. The Faraday and Kbnig-Marinov generators coupled with the ball-bearing.

As the ball-bearing. The condition for an eternal motion thus is that the electric power produced by the. A metal ring sandwitched between two permanent ring magnets with the indicated.

The outer race of the big ball-bearing is fasten by the help. The circuit "shaft - small. When the stopper is removed, the tension of a driving battery can be applied to the.

At the indicated polarity of the applied tension, the ring which now represents. The current thermal dilatation effect will inmediately support the rotation and.

The tension induced in the rotating ring will be opposite. If the current thermal dilatation torque will. One can, before. When the magnets in the machine presented in fig.

The external force with which I drove. This kind of external torque was used also in the next. I calculated the efficiency of the machine first when the magnets were not taken.

From the geometry of the rotor and the specific gravity of the iron, I found its moment. When the rotor. If we assume a linear decrease. The efficiency which I calculated only for.

The tension induced in the apparatus in fig. Thus here. The elements 1, 2, and 3 form a frame which maintains the vertical axle 4 solid to. The axially magnetized.

In this way I diminished substantially the mechanical. The rings 16 and 17 are of plastic: the ring 16 holds. The moment of inertia of the.

The half-time interval in which the motor reached the steady. Thus the mechanical power of the motor. As the ohmic resistance of the. The motional -transformer inductor coupled with an a.

My discovery see section 11 that the seat of the motional -transformer induction. In such a case a magnetic interaction,.

In these cases the motional -transformer. More interesting is the case of motional -transformer. Here the whole wire is "outside the poles". The braking,.

Moving the magnet with respect to the loop a motionaltransformer. Which is the conclusion? If, however, the metal plate. For a quick calculation.

The n we shall have for the. If R is the ohmic resistance of the wire, the power produced will be. The same result can be obtained directly from the relative Newton-Lorentz equation 10 ,.

If we shall increase and decrease. Consequently an alternating. The magnitude of the induced tension can be very easily calculated.

If the momentary velocity of expansion is. Such an experiment can be carried out very easily by making the wire of the primary.

As far as. The induction in the delineated experiment is not transformer but motional -transformer. In a generator.

This is also the case in our "generator": the. Indeed, looking at the right cross-section of the. I found fig. The space between the sectors is non-magnetizable material.

The one disk is solid to the torus and the other one can be rotated.

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Ich denke, dass es der falsche Weg ist. Und von ihm muss man zusammenrollen.

Ich meine, dass Sie nicht recht sind. Ich biete es an, zu besprechen. Schreiben Sie mir in PM, wir werden umgehen.

Jetzt kann ich an der Diskussion nicht teilnehmen - es gibt keine freie Zeit. Sehr werde ich bald die Meinung unbedingt aussprechen.