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03/2000 Discussion on the principles of Hybrid reluctance magnet

A closed magnetic tract that combines a permanent magnet and an electromagnet, the core of this invention, shall be referred to as the basic factor.
The basic factor is composed of a permanent magnet (a) and an electromagnet (b). The permanent magnet is obtained by sandwiching a neodymium magnet (hard magnetic) with pure iron bars (soft magnetic) in the ---- direction. The electromagnet is obtained by winding a copper wire coil around a core ( -shaped soft magnetic (pure iron)).

Regarding the basic factor, interfaces between the permanent magnet and the electromagnet "p" and "q" are important.
[1] When no electricity passes through the electromagnet (b) (off)
The line of magnetic force from the permanent magnet (a) merely circulates the closed magnetic tract of the basic factor, and almost leakage of magnetic flux occurs into air. Therefore, the interfaces "p" and "q" strongly attract each other. In this case, attraction of "p" and "q" is due to the permanent magnet alone.
[2] When electricity which generates magnetic fluxes in a larger number than magnetic fluxes from the permanent magnet (a) is passed through the electromagnet (b) with the two poles in opposite positions
The line of magnetic force of permanent magnet (a) is released into the air if it is pushed back by the line of magnetic force of electromagnet (b) above the "p" and "q" contact surface and exceeds the saturation of permanent magnet (a). In this case, if the number of magnetic fluxes is large enough, the line of magnetic force released in the air is the synthesis of permanent magnet (a) and electromagnet (b). Therefore, the "p" and "q" contact surface shows strong adsorption, which is solely due to electromagnet (b).
[3] When electric current which generates magnetic fluxes in the same number as permanent magnet (a) in electromagnet (b) is passed and the residual magnetic flux density of the basic factor is not yet saturated, the "p" and "q" contact surface does not either attract or repel each other (powerless status).
This means that in this status, the line of magnetic force of permanent magnet (a) and that of electromagnet (b) do not communicate each other via the "p" and "q" surface. The number of magnetic fluxes of permanent magnetic (a) and that of electromagnetic (b) that exceed the saturation of residual magnetic flux density of the basic factor are equal and large, contact surfaces "p" and "q" repel each other and the line of magnetic force of each surface leaks into the air as magnetic flux.

[4] In status mentioned in [3] above, the action surface of the basic factor is defined as (x), and a mobile material composed of a soft magnetic material (pure iron) adjacent to (x) as (y). In the status mentioned in [3] above, electric current input into electromagnetic b is defined as a (value at a point where the "p" and "q" contact surface is powerless).

In the status mentioned in [4] above, the a value decreases gradually as the air gap between the basic factor and mobile material (y) is reduced. This means that the line of magnetic force of permanent magnet a forms a magnetic tract via the air gap vs mobile material (y) and generates attractive power on action surface (x) without forming a closed magnetic tract within the basic factor beyond the "p" and "q" contact surface. In this case, the amount necessary to block the line of magnetic force of permanent magnet (a) on the "p" and "q" contact surface can be large enough for being an a value input into electric magnet (b). Consequently, the easier it is for the line of magnetic force of permanent magnet to form a magnetic tract with mobile material (y), i.e., the greater the attractive power on action surface (x), the smaller the a value. Naturally, the attractive power on action surface (x) is determined by the performance of the permanent magnet. However, if a large amount of electric current is inputted into the electromagnet (b) as in [2] above, the attractive power on action surface (x) is the synthesis of the lines of magnetic force from permanent magnet (a) and electromagnet (b). This results in a great attractive power but energy utilization efficiency decreases.
In order to increase the attractive power on action surface (x) and decrease the value in the status mentioned in [4] above, thee conditions can be considered:
1. To reduce the air gap on action surface (x)
2. For the core of permanent magnet (a) and the soft magnetic of movable part (y), to use a material whose saturation magnetic flux density is greater than that for the material used for the core of electromagnet (b).
3.To make the distance of the magnetic tract that forms movable part (y) via permanent magnet (a) and the air gap (L2) shoter than that of the closed magnetic tract in basic factor (L1). Needless to say, it is important to improve the performance of the permanent magnet (Br, BH) in order to increase the attractive power on action surface (x). New materials that may replace neodymium (e.g., super-conducting magnet) are under development.
An appropriate distance (width) of the permanent magnet in the flux direction (L) and an appropriate length of permanent magnet (a) (XL) can be calculated from the cross section area (Z), Br, BH curve, and permeance coefficient. This makes it possible to determine the optimal size of permanent magnet (a) and mobile material (b). An electromagnet b) compatible with permanent magnet (a) should be designed taking statuses [1] through [4] into account.

@[Conclusion]
A. Combination of electromagnet (b) and mobile material (y).
B. Combination of the basic factor and mobile material (y).
For comparison, the air gap, material, distance of the magnetic tract, area of the cut surface, volume, coil thickness, and other conditions for "A" and "B" above must be the same as much as possible. If the attractive power on the action surface in "A" and "B" above is the same, the electric power input in the case of "B" above is several times smaller than in the case of "A" above. In the case of a reluctance motor in the form of "A" above, the energy conversion rate is usually about 30%. If a reluctance motor produced in the form of "B" above requires 30% or less of electric power input compared to a motor produced in the form of 1 above, electric output greater than input can be theoretically expected. This proves that energy of a permanent magnet is converted into dynamic power.