JPS61277364A - Magnetic-force rotating machine - Google Patents

Abstract

PURPOSE:To obtain revolving torque without requiring a power source by arranging magnets in parallel to fixing sections on the circumference and generating revolving torque by the change of the quantity of a magnetic material magnetized to these magnets and a reaction. CONSTITUTION:A plurality of magnets A-E, D', E' are disposed in parallel to a fixing section P, and magnetic materials F, I, F', I' are mounted to a rotating section O. The magnets A, B, C are arranged at regular intervals at the center so that magnetic poles are alternated. The magnet D is disposed to the right intermediate section of the magnets A, B, and a magnetic pole has the relationship of magnetic force of an unlike-pole on this side and a like-pole in the front. The magnet E is faced oppositely to the magnet D, and magnetic poles are also arranged alternately, and the relationship of a position to the magnets B, C and magnetic poles is the same as the magnet D. The magnets D', E' are disposed symmetrically to the magnets D, E on the left side of the magnets A, B, C. A rotating section O is turned by the change of the quantity of the magnetic materials, F, I, F', I' to these magnets A-E, D', E' and a reaction.

Description

DETAILED DESCRIPTION OF THE INVENTION (1) The present invention is a magnetic rotating machine that can rotate and obtain power only by a combination of magnets and magnetic machines installed in a fixed part and a rotating part.

Most conventional rotating machines require power sources such as electric current and fuel, and therefore face many problems such as resource depletion and environmental pollution.

(2) The present invention was conceived with the aim of eliminating the above-mentioned drawbacks, and is rotated by the change and reaction of the magnetization of a magnetic machine with respect to a magnet. It is a perspective view cut in two.

A to E, A' to E' are attached to the P of the fixed part with magnets, and FI,
F'I' is a magnetic machine and is installed at O of the rotating part.

(3) FIG. 2 is an expanded plan view of the one-point chain in FIG. 1. The magnets ABC are equally spaced in the middle, and SN indicates magnetic poles and are arranged alternately. Magnet D is placed in the middle on the right side of AB, and the magnetic polarity is such that the front side in the direction of the arrow has a different polarity, and the front side has the same polarity. The magnetic poles of E and D are also arranged alternately, and the position and magnetic pole relationship with BC are the same as D. D'
E' is placed symmetrically with DE on the left side of ABC.

F is a magnetic machine located between A and D, and F' is also symmetrical with F. GG' and HH' represent the positions when FF' moved, and the arrow indicates the direction of movement of F.

Note that II' in FIG. 1 is omitted in FIG. 2.

(4) Now, looking at magnets AB and D in Figure 2, we see that A and D (
Since the positions F) have different magnetic poles, they absorb each other and the magnetic force is attenuated. B and D (point G) are repelled by the same magnetic pole, and the magnetic force is enhanced.

Therefore, since the amount of magnetization is attenuated at the position F, the magnetic machine F is attracted by the increased magnetic force at the point G and moves in the direction of the arrow. As F moves to point G, it becomes strongly magnetized by the magnetic forces of D and B. Therefore, F reacts to B and D while also acting as a magnet.

In other words, since B has a large mass, it is attracted by its magnetic force and continues to move in the direction of the arrow, but D is repelled.

Therefore, the moving force of F is promoted by this, and since E, which is on the line of movement, is the magnetic pole of S, it is attracted by the magnetic force and reaches point H.

In other words, as F faces an attenuating magnetic field and a repelling magnetic field in sequence, the amount of magnetization increases or decreases due to the magnetic force of those magnetic fields, and this change causes the magnetic force to attenuate at the position of F, attracting movement, and when it reaches point G. Therefore, D becomes repulsive and moves to point H.

(5) Next, F, which has moved to point H, absorbs the magnetic force of the S pole of E, so the magnetic force of the magnetized N is reduced, and F returns to the properties of a magnetic machine. related to E
Looking at B, the mass of B is larger than ■, so at first glance F seems to be pulled back by the magnetic force of B, but
Looking at the arrangement of E, the movement line of F is biased to the right.

In other words, it is arranged closer to the left end of E than the right side end of B. Therefore, F is attracted to the left end of E and moves to point H.

This is due to the characteristics of the attraction relationship between the magnet and the magnetic machine, and although it is normal that objects with larger mass will be attracted, the attraction relationship also responds strongly to the degree of proximity. In other words, even if E has a small mass, it can attract F by setting the degree of proximity to F.

Therefore, F can come within the range of E.

Note that this proximity relationship is the same at point G, but in this case, F
is within the range of B, not D, which is nearby. The difference in the movement of F in this close relationship is because point G is in a repulsive magnetic field.

In other words, since point G is a repulsive magnetic field, the amount of magnetization increases under the magnetic machine, producing a repulsive force, and between it and D, the attractive force in the proximity relationship disappears due to the repulsive force. Since B has a large mass, F has a stronger attraction relationship with F as a magnetic machine, so it moves to B.

(6) If we look at the relationship between these magnetic fields, mass differences, and magnetic machine F in Figure 3, the position of F in Figure 3 is a half-step moved from the position of F in Figure 2, and point G is the same. G in Figure 2
This is a place that has moved half a step from the point. Although F is close to D, its mass is small, so the amount of magnetization remains weak.
It's on.

Therefore, F reacts to AB as a magnetic machine, that is, moves to the repulsion-enhancing magnetic field, and F at point G (Figure 3) increases the amount of magnetization due to B, so F reacts to AB as a magnetic machine and repulses as a magnet. It has power, and is repelled by D and attracted to E.

(7) That is, by alternately setting the attenuating magnetic field due to the attraction relationship and the reinforcing magnetic field due to repulsion, the increase and decrease in the magnetization amount of the opposing magnetic machine is repeated, and the movement of the magnetic machine continues.

(8) Furthermore, there are D' to H' on the left side of ABC, but these are arranged symmetrically to D to H, and their actions are also completely symmetrical, so the movement process from F to point H is Of, A
~ All movements related to E (left and right shaking phenomena) are canceled out.

(9) As described above, since the present invention rotates only by magnets and magnetic machines, it does not require any replenishment and can obtain power completely free from pollution.

[Brief explanation of the drawing]

FIG. 1 is a perspective view of the present invention, cut in two. FIGS. 2 and 3 are plan views developed from FIGS. 1 1' and 11 11'. (1) A to E and A' to E' are magnets, and SN indicates their magnetic poles. (2) FF' is a magnetic machine, and GG', which is a one-point chain, and HH', which is a two-point chain, represent the location where FF' has moved. (3) The arrow indicates the direction of movement of FF'. (4) II' in Figure 1 is omitted in Figures 2 and 3.

Claims (2)

[Claims] (1) As described in detail in the main text, a method of arranging magnets in which magnets are arranged in parallel on a circumferential fixed part, and the magnetic force relationship is alternately continuous with an attracting magnetic field of different polarity and a repelling magnetic field of the same polarity. (2) A method in which a magnetic machine installed on a rotating part having a shaft is opposed to each other between the magnetic fields of (1), and a magnetic force relationship is established in which the amount of magnetization is attenuated by an attractive magnetic field and the amount of magnetization is increased by a repelling magnetic field.