JPH04222479A - Method of getting power with permanent magnet - Google Patents

Abstract

PURPOSE:To get a power source with a permanent magnet by making use of the action that the repelling and attracting forces of each magnet become strong when the corner or its vicinity of the rear end of the pipe-shaped magnet and the end of a rectangular magnet come close to each other. CONSTITUTION:The plane of a magnet 1 is of a pike shape, and a magnet 2 is of a rectangular shape, and both its ends are inclined. The pike-shaped magnet 1 is placed in the middle, and rectangular magnets 2 are fixed on both ends. It is so arranged that it can rotate or shift, with the interval between the magnets 1 and 2 between, for example, 2m/m and 3m/m at the clossest approach point. At this time, the action that the repelling and attracting forces of three magnets 1 and 2 become strong when the corner or its vicinity of the rear end of the magnet 1 and the end of the magnet 2 come close to each other is made use of. Moreover, by arranging the magnets 1 and 2 in both forms in fixed rows and driving rows and making use of magnetism increasing phenomena and magnetism phenomena for multiparallel arrangement, the driving force is elevated further, and it is made use of as a power device. Hereby, clean energy can be taken out constantly.

Description

DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention utilizes a device combined with permanent magnets as a power source.

[Prior Art] Regarding the use of permanent magnets, it seems that no permanent magnets have been put into practical use as a power source.

[Problem to be solved by the invention] In order to obtain a power source using a permanent magnet, the repulsive force and attractive force between the magnetic lines of force emitted by the magnets are used. The power source was discovered based on the mutual relationship between the two forms, and the driving method was clarified.

[Means for solving the problem] To explain the relationship between the basic form of magnets and the power source, all the magnets in Figure 8 have the same height, and (10), (11), and (12) have the same volume. It is a magnet with an unusual shape, the plane of (10) is an equilateral triangle, and the inclination angle of (11) (
16) is 30°, magnet (13) is twice that of (10), and magnet (
14) has a volume three times that of (10), and the above five types of magnets are weighed using a repulsion type driving method. In Figure 9, the magnets on both sides are fixed, and the center magnet is movable. The closest distance between the magnets on both sides is 2m/m to 3m/m.
The device is moved in the driving direction (3) by pulling it with a weight (20) from the front position, and the resistance force is the value required to pass between the magnets on both sides. 20
), and the value required for passage is used as the propulsion force. Figure 11 shows the device, and except for the magnet, paramagnetic materials and magnetically insensitive materials are used. Figures 12, 13, 14, and 15. , 16th
The diagram shows the combination of each magnet and magnetic pole, and the metric value of the propulsive force in FIG. 12 is set as 100, and the values of each metric ratio are shown in the following table.

In the combination shown in Figure 16, the magnet (11) is fixed to the fixed bases (6) on both sides with the same width as the vertical width, and the magnet (14) is attached to the pulley base using the device shown in Figure 17. Fixed to (5), first
When you let go of the position shown within the dotted line (22) in Figure 8, the magnet (1
4) is the repulsive force with the magnet (11), and the pulley stand (5)
In the case of an adsorption type arrangement that advances in the driving direction while gaining acceleration, when the magnet (14) is released from the position within the dotted line (23) shown in Fig. 19, the pulley stands (5) will move in the driving direction. Proceeding, these phenomena are used with magnets (11) and (14).
) Figure 20 shows the pattern of magnetic lines of force of magnet (11) and magnet (14), and the sides of each line (26) and (25) near the center are polar. The center of magnetization in Figure 21 is the center of magnetization, with scales dividing the length of the magnet (14) into 10 on the left and right.
This is a graph showing the values of propulsive force and resistance force depending on the positional relationship of magnets (11) and (14) for the repulsive type.
The zero point located near the rear end of the magnetized line (25) of 14) and exhibiting neither propulsive force nor resistance to the magnets (11) on both sides is defined as the static line (30), and the left and right lines are separated from this line. Propulsive force is applied in the direction of arrow (27) with respect to the zero point of
The maximum value of the propulsive force (
31) indicates the propulsive force value of 81 in the row of Figure 16 of the table, and the maximum resistance value (32) similarly indicates the resistance value of 39. In the case of the Naho adsorption type, Driving direction arrow (
3) is in the opposite direction, the graph is left and right opposite with the stationary line (30) as the border, and the values are exactly the same as the rebound type.

In the arrangement shown in Figs. 18 and 19, the propulsive force constantly exceeds the sum of the propulsive forces and the sum of the resistive forces that the magnet (14) receives, and the driving force is generated. However, it is a very basic phenomenon.

[Effect]

The above describes the phenomenon in which driving force is obtained in a combination of the basic forms of magnets. First, we modify the form to be usable as a power source, and then explain the action of the standard form of the magnet. do. The magnet (14) is shortened in length in order to increase the torque efficiency for rotational drive, and the rear end is enlarged in order to increase the propulsive force.
11) is completely lacking in capacity, and as shown in Fig. 23, it is changed to magnet (2) with the same capacity as the volume from the magnetization center line (25) to the rear end of magnet (1), and the shape is changed to magnet (2). The corner (16) and the length (17) are selected so that the driving force is optimized depending on the shape of the magnet (1).
1). The stationary line (30) in (2) can be determined by drawing out the common line of the array of magnets in the stationary state in the attraction type arrangement of magnets (1), (2) and magnetic poles shown in Fig. 24. In the standard arrangement shown in Figure 25, the magnet (1)
And (2), the vertical spacing between magnets (1) and (2) is such that if they are too close together, demagnetization will occur due to repulsive force. In order to short-circuit the lines of magnetic force, a magnet (1
) Adding a yoke (29) to (2) provides a synergistic effect of reducing resistance. To describe the action of a standard type magnet, Figure 27 is a graph when the magnet (2) is fixed on the left and right sides of the repulsion type and the magnet (1) is driven singly in the direction of the arrow (3). Propulsive force (35), resistance force (36) in the middle, net driving force (37) in the lower part, and a driving force of 30% or more of the propulsive force can be obtained on average. ．． (2) and the arrangement of magnetic poles are shown in Figures 4, 5, and 6.
As shown in Fig. 7, it can be used as a power source.

〔 Example 〕

The example described so far is one in which magnets (1) and (2) are arranged in three vertical rows, and it is more economical to use them in parallel, and the magnets increase the magnetism between each other as a result. The demagnetization phenomenon is observed in the magnet (1) used in the present invention. The arrangement of magnets and magnetic poles shown in Fig. 28 can further increase the driving force by taking advantage of the characteristics of the form (2).
When the arrangement (2) is between the vicinity of the magnetization line (25) and the rear end, demagnetization occurs at the magnetic poles (38) and (39), and in the attracting type on the right, the magnetic poles (40) and ( 41) The magnetization phenomenon occurs in the magnet (1) as shown in Figure 29.
13 on average from near the center (42) to the rear end of the
There is an increase/decrease effect on the order of %, and the effect on the tip side of the magnet is extremely reduced from near the center (42), returning to the normal state.This is due to the increased distance between the magnets on both sides and the magnetic field lines of the magnet (1) itself. Due to this phenomenon, which is thought to be due to a synergistic effect that reduces the capacitance, the fourth magnet (1) is used for multi-parallel use by changing part of its shape as shown in Figure 30 without changing the capacitance of the magnet (1).
In the repulsion type arrangement shown in the figure, the magnet (1) is placed in the 31st row.
The magnets (1) are arranged alternately as shown in the figure to increase the driving force due to demagnetization of the resistive force, and in the adsorption type shown in Fig. 5, the horizontal rows of magnets (1) are arranged in a straight line as shown in Fig. 32. The driving force is increased by concentrating only on the mutual magnetizing effect of the propulsive forces. [Effects of the invention] The use of the invention as a constant source of clean energy is highly effective.

[Brief explanation of the drawing]

FIG. 1 shows the standard form of the magnet used, FIG. 2 is a perspective view thereof, and FIG. 3 shows the basic rotary drive device. FIG. 4 and subsequent figures are diagrams sequentially explaining the arrangement of magnets and the driving phenomenon. 1... Spearhead magnet 2... Oblong magnet 3... Driving direction 25... Magnetization center line 30... Stationary line FIG. 33 shows a multi-parallel drive device.

Claims (1)

[Claims] 1. A magnet (1) whose flat surface is in the shape of a tip, and a magnet (2) which is oblong and has sloped ends, the magnets (2) are fixed on both sides, and the magnet (1) is located in the middle, magnet (2)
A magnet (as shown in Fig. 4) is installed so that it can be rotated or moved in a straight line with an interval of 2 m/m to 3 m/m at the re-approach point.
1). (2) and a method of arranging the magnetic poles and driving the magnet (1) in the direction of the arrow (3) 2. In the magnets (1) and (2) according to claim 1, an apparatus as described in claim 1 is provided,
Magnet (1) as shown in Figure 5. (2) and a method of arranging the magnetic poles and driving the magnet (1) in the direction of the arrow (3) 3.
In the magnets (1) and (2) according to claim 1, the magnet (
1) is fixed on both sides, magnet (2) is located in the middle, and the distance between the magnets (1) on both sides is 2 m/m to 3 m at the closest point.
The magnet (1), (2) and magnetic poles are arranged as shown in Figure 6, and the magnet (2) is driven in the direction of the arrow (3). Method 4. In the magnets (1) and (2) according to claim 1, the magnets (1) and (2) are arranged as described in claim 3, and the magnets (1) and (2) and magnetic poles are arranged as shown in FIG. Method of driving in the direction of arrow (3) 5. In the driving method according to claim 1, when the magnets (1) and (2) are arranged in parallel, the magnets (1) and (2) are arranged in parallel.
) and a method of driving by arranging magnetic poles 6. According to the driving method according to claim 2, when arranging multiple magnets in parallel, a method of arranging magnets (1) and magnets (2) and magnetic poles as shown in FIG. 31 and driving them.