NEGATIVE INDUCTOR

previous FIELD OF NEGATIVE ENERGY

As a result of interpretation along the general principle of relativity, it can be found that the opposite self-induction phenomenon is caused by the change of the relative flow quantity between the same kind of electric charges. In applying the phenomenon, it would be possible to generate an electric power from a space while making the entropy decrease. So, I will now introduce a basic circuit element to do that.

A conduction current is the relative flow between the free electrons bearing negative charges and the ion atoms bearing positive charges. In short, it is the relative flow between the different kind of charges. On this occasion, a normal self-induction occurs. In order to the different kind of charges. On this occasion, a normal self-induction occurs. In order to produce an opposite self-induction in the conduction current, it is necessary to make a relative flow between the same kind of electric charges. To do it, the positive ion atoms should be changed into the negative ion atoms , or the free electrons should be changed into the positrons. However it is impossible to be realized judging from the constructions of the materials. Also a trial, to bring the relative flow between the same kind of charges by electrifying the surroundings of the conductor into negative, is unrealistic. The reason is that it is necessary to concentrate the negative charges closely to the conductor contraly to the Coulomb force. Furthermore a greater quantity of the negative charges than of the positive charges of the ion atoms in the conductor is needed. Of course, it is impossible.

First, let's envision a conduction current which would not bring the self-induction. This means the current without its magnetic field, that is, the two-way currents. When two kinds of currents, that have the same quantity and the opposite directions, flow into the tightly fit two electric wires one by one, the magnetic fields never appear to be resisting each other. Thinking these double-wires as a single conductor, from the viewpoint of the ion atoms, the flow quantity of the free electrons flowing to the left is equal to the one flowing to the right. Accordingly, the magnetic field does not appear from the viewpoint of the ion atoms. Thinking of this condition from the sight of the free electrons flowing to the left, half as many the free electrons as the ion atoms flow to the right at double the speed of the ion atoms. That is, the flow quantity of the free electrons is equal to the one of the ion atoms. Accordingly, the magnetic field does not appear as well from the viewpoint of the free electrons flowing to the left. On the other hand, considering the situation from the sight of the free electrons flowing to the right, half as many the free electrons as the ion atoms flow to the left at double the speed of the ion atoms. That is, the flow quantity of the free electrons is equal to the one of the ion atoms. Accordingly, the magnetic field does not appear as well from the viewpoint of the free electrons flowing to the right.

( CHART 4 ) relative flow of charges in double electric wires (In each case, magnetic field does not appear.)

Assume that two currents with the same quantity in the opposite directions flow in the double electric wires. When the currents change, the variation of the flow quantity of the positive electric charges is always equal to the variation of the flow quantity of the negative electric charges in the background of the flowing free electrons. Accordingly, the variation of the flow quantity of electric charge occuring in the background of the free electrons do not bring any variations of the magnetic field. Without the variation of the magnetic field, the induced electric field cannot appear. At this time, the relative selfinduction doesn't occur between the free electrons flowing and the background.

When the current changes under the condition that the background of the double electric wires is charged into negative, the relative flow quantity changes between the free electrons flowing in the conductors and the free electrons being in the background. That is, it is possible to change the relative flow quantity of the same kind of charges. At this time, the opposite self-induction phenomenon with a negative energy appears.

( CHART 5 ) When the background of double electric wires are electrified into negative, magnetic fields with negative energy appear at the viewpoints of free electrons in Group A and Group B by opposite-self-induction.

Double coils can be made by winding up the two electric wires to the magnetic core. After we electrify the magnetic core into negative, we flow the electric current in the double coils, just then the relative opposite self-induction phenomenon appears between the free electrons attached to the magnetic core and the free electrons flowing in the double-coils. As a result of that, a negative energy can be stored in the surroundings where the relative magnetic field appears. We give the name negative inductor to the inductor which consists of the magnetic core electrified into negative and the double coils (non-inductive coil) in which the currents with the same quantity and the opposite directions flow.

(CHART 6) NEGATIVE INDUCTOR

CHART 6 is a sample of the simplest negative inductor. In order to increase the electrostatic capacity of the magnetic core , two aluminium cylinders with different diameters are set coaxially as a magnetic core. Winding up the two immediate enameled wires thickly to the outer cylinder (in the chart, a wire is indicated with blue, another with red), the ends of one of the wires close and the ends of other open. The two opened ends become the connecting terminals of the negative inductor. To make the relative magnetic field which is observed from the free electrons flowing in the coil, appear in the direction which brings the opposite self-induction, it is necessary to electrify the outer cylinder into negative and the inner cylinder into positive. If the cylinders are charged with the opposite polarities, the positive inductance occurs in the double coils.

In CHART 6, the conditions are as follows ; a = 0.03(m), b = 0.05(m), c = 1.2(m), the semidiameter of the electric wire (copper) forming the coil , the applied voltage to the magnetic core , the inner cylinder is electrified into positive and the outer cylinder into negative. And the two connecting terminals close. Provided that the the outer cylinder into negative. And the two connecting terminals close. Provided that the double coils of this negative inductor is boosted with 500 Volts, the electromotive force of the opposite self-induction is 15 Volts in the initial time.

The direction of the electromotive force of the opposite self-induction induced in the increasing current is equal to the direction of the initial applied voltage. Accordingly, in the situation above, at the same time that the initial voltage 500 Volts is applied, the total voltage reaches 515 Volts instantly. Then, much larger currents and electromotive forces in the direction which helps the current increasing is induced. With such endless inductions, the current can easily reach the physical limit point in a short time. And when the current is made decrease by handling the voltage, the electromotive force in the direction which helps the current decreasing is induced, and after the current reaches zero instantly, the current begins to accelerate in the opposite direction rapidly.

The negative inductance of the negative inductor is proportional to the product of the rate of change of the relative magnetic fluxes piercing the coil and the number of turns of the coil, like the general inductor. By rising the voltage aplied on magnetic core, the total number of the relative magnetic fluxes piercing the double-coils can be increased.

In order to actuate the circuit including the negative inductor, it is necessary to cancel the magnetic fields as much as possible in the circuit, for keeping the total inductance of the circuit negative.

The negative inductor stores a negative energy in a space where the relative magnetic field appears, and as a counteraction, the inductor generates an electric power with a positive energy. The free electrons which got a kinetic energy from a space as accelerating returns the kinetic energy to the space as decelerating. In a normal conductor, the free electrons lose the kinetic energy by colliding with the atoms. In this case, the atoms which enhanced their vibration energy by the collisions with the free electrons radiate heat. In the electric wire of the negative inductor, the kinetic energy of the electrons go in and out the space, so that the electrons influence the atoms just a little. For this reason, the free electrons work to buffer the thermal vibrations of the atoms. That is, the negative inductor becomes cool in the actuation. The same phenomenon occurs in a conductor just charged into negative as well. Though the free electrons in the conductor are making motions in their random directions while colliding with the atoms, these free electrons cancel out each other's speed, so the current does not appear macroscopically. This situation is equal to the one in which the two currents with the same quantity and different directions flow into the non-inductive double coils. Provided that the conductor electrifies into negative, each free electron making the thermal motion can bring the opposite self-induction while accelerating or decelerating. Accordingly, the conductor with a negative charge is refrigerated, and the field of negative energy appears in the surroundings. Thus the conductor which become negatively charged can be considered as a negative conductor which is working.

Our future tasks are to develop perpetuum mobiles using the negative inductor and to study the effect of anti-gravity brought by the negative inductor.

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