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Chapter 4: The
momentum order at the electromagnetic engine The presupposition: The ripple current
and the alternate current The alternate current to think of here is so-called " the single-phase alternate current " of the sine wave. Its waveform becomes like the following figure. It has both positive and negative ingredients and the direction in which the electric current flows turns. Figure 13: Alternate current waveform
The ripple current passed through the electromagnetic engine is a direct current to have removed only either of the ingredients of the alternate current in the above figure by rectifying. The waveform becomes like the following figure. It is the electric current to have only either positive or negative ingredient and to flow only through one-way. As for the half time when it flows, the strength of the electric current is zero. But, it is the one which is made very low voltage. And, the wavelength is made equal to the length of a round of the loop of normal conductive electromagnet. This ripple current has very high frequency. Figure 14: Ripple current waveform
It is to think of the size of the electromagnetic force which this ripple current gives each electron pair. The strength of the magnetic field made by the ripple current is in proportion to the strength of the ripple current. Because of "F=BIL", the electromagnetic force which acts on the permanent current is in proportion to the strength of the magnetic field. The strength of the electromagnetic force which acts on the permanent current is in proportion to the strength of the ripple current. Also, because of "F=BIL", the strength of the electromagnetic force which acts on the ripple current is in proportion to the strength of the ripple current. Then, the strength of the electromagnetic force which acts on the permanent current as the reaction is in proportion to the strength of the ripple current. Therefore, according to the strength of the ripple current, the electromagnetic force acts on the superconductive magnet. The electromagnetic force of different strength acts on each electron pair in proportion to the strength of the ripple current, the height of the mountain of the ripple current. Figure 15: The size of the electromagnetic force by the ripple current
And, since the wavelength of the ripple current is equal to the length of the loop of normal conductive magnet, i.e. the loop of superconductive magnet, electron pairs in half part of the superconductive magnet receives zero of impulse. At each moment, the impulses with different sizes are given to electron pairs. Then, the moving velocity of the waveform of an alternate current is supposed to be near the velocity of light. Because of this, it takes the form that the waveform of ripple current foreruns electron pairs. Then, like figure 6, the impulse of different size is given to each electron pair which composes a permanent current in the constant time. Then, since the half waveform is electric current zero, I think at least one electron pair which receives the impulse below the constant value in the constant time exists. Therefore, it becomes the condition of figure 12, the impulse of the electromagnetic force to act on electron pairs which compose the permanent current is canceled and the repulsion or the attraction to act on the superconductive magnet is canceled. Because of this, only the repulsion or the attraction to act on the normal-conductive magnet remains and can be used as a driving force. However, even if supposing that the momentum of same size in the direction of electromagnetic force remains in each electron pair like figure 9 and that the repulsion or the attraction arised in the superconductive magnet, I think that it becomes sufficiently smaller than the repulsion or the attraction which arised to the normal-conductive magnet.
f1 becomes sufficiently bigger than f2. As a result, it is possible to use "F=f1-f2" as a driving force.
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