The present invention relates to an electromagnetic linear motor. The motor can be used to move the movable parts of various apparatuses, e.g. a reciprocating linear compressor, a linear actuator, or a solenoid valve.
As an example application we refer to the field of compressors, in which numerous types are known: piston-operated, screw-operated, lobed, with propellers, centrifugal etc., for the most part moved by rotary motors.
There are other systems of linear compressors mostly applicable in refrigeration systems. This sector may be improved by the introduction of a suitable linear motor.
The main object of the present invention is to propose an electromagnetic linear motor, in particular to produce linear compressors, actuators, and solenoid valves. Thanks to the linear motor one can e.g. make a linear reciprocating compressor with double efficiency compared to the current reciprocating compressors driven by rotary motors; in general the motor is integrable into systems that require compression of a fluid, into compression systems, into refrigerant systems, heat pumps or volume compressors for internal combustion engines.
With the electromagnetic linear motor one is able to accomplish:
The same advantages are shared in the production of linear actuators and/or solenoid valves, in particularly for distribution valves, with fully-electronic control, in reciprocating endothermic engines.
A linear motor and its advantageous variants are defined in the appended claims, while features and advantages of the present invention are illustrated by the following description of some embodiments, illustrated with reference to the following figures:
In the following, identical numbers indicate identical or similar parts; and the letters N and S indicate respectively North and South magnetic poles.
As a first application of the motor we refer to a compressor.
In
Each electromagnet 2 comprises a core U on which are wound reels or windings 3. In particular, the core U comprises a central linear segment 4, with an axis q, from the ends of which extend orthogonally to said axis q two polar expansions 5 parallel to each other. The central linear segment and the two polar expansions 5 together form a ferromagnetic core in the shape of a “C” or a “U” or a “horseshoe”. Preferably, the polar expansions 5 are recessed in the shape of an arc 6, in the part distal to said axis q, with a radius slightly greater than the diameter 10 of the permanent magnet 7 that they will skim. The longitudinal dimensions of the ferromagnetic core are determined by the length R between the extreme edges of the polar expansions and by the distance r between the inner edges of the polar expansions (
The electromagnets 2 are stacked to constitute a cylindrical chamber 100 with a longitudinal axis W, so that the stator 1 has a generally tubular shape. Preferably the electromagnets 2 are applied on the side walls of a hollow cylinder 401 (
Within the stator 1 is placed a cylindrical permanent magnetic component 7 which is mounted to slide along the axis W. The stator 1 surrounds the permanent magnet 7 with the electromagnets 2, whose magnetic poles, i.e. the polar expansions 5, are arranged radially and orthogonally with respect to said component 7 and consequently extend radially and orthogonally relative to the axis W. The arcuate shape of the expansions 5 facilitates their symmetric distribution about, and to skim, the permanent magnet 7 (
The electromagnets 2 are linearly packed and stacked with their axes q aligned to form columns A, B with axis Q, so that the expansions 5 of a column A are offset along the axis W compared to those of another column B. Each electromagnet 2 is arranged linearly with another electromagnet 2, with coincident axes q, so that the respective expansions 5, the poles, form along the columns a longitudinal sequence parallel to the axis W. The poles of the permanent magnet 7 are oriented along the axis W.
In other words, there are columns of electromagnets 2 placed radially side by side, arranged around the permanent magnet 7, and each column with axis Q parallel to the axis W (axis of the stator 1, and thus longitudinal axis of the chamber 100). The electromagnets 2 when powered generate respective magnetic poles that are placed in a row radial and parallel to the axis W and, consequently, to the permanent magnetic component 7 which they have to skim. The magnetic field closes from an N pole to an S pole hitting the permanent magnetic component 7 and the axis W.
In particular, the linear motor comprises at least a first plurality of electromagnets 2 with related coils 3 with the cores' axes q linearly arranged to form one of the columns A with axis Q. In the example shown (
The electromagnets 2 constituting the columns are linearly arranged with coincident axes q to constitute an axis Q parallel to the axis W, with a spacing Z between the poles of each adjacent electromagnet. The spacing Z may vary according to design and operational requirements.
The electromagnets 2 are preferably identical to each other, regardless of the column they belong to.
The electromagnets 2 of a column A are arranged staggered along the axis W, with respect to the electromagnets 2 of an adjacent column B, by a distance h. The order of magnitude of the offset h between the columns A and B may vary according to design and operational requirements.
In the example illustrated in
The electromagnets 2 of a first column A are electrically powered and biased in sequence, simultaneously or alternately to the electromagnets 2 of a second column B staggered with respect to the first by the distance h.
In the following description, any spatial reference will refer to the spatial arrangement as shown in the accompanying figures.
In
The permanent magnet 7 is keyed on a stem 8 connected at the two ends respectively to a first plunger 9a and a second plunger 11a placed, in this case, symmetrically with respect to the permanent magnet 7; in the example each plunger 9a, 11a is placed at a respective end of the stem 8.
In particular the first plunger 9a is inserted airtightly in a first cylinder 9b, and the second plunger 11a is inserted watertightly in a second cylinder 11b.
When the permanent magnet 7 moves upwards, moving in the direction of arrow D1, a vacuum is created in the lower part 9c of the first cylinder 9b, below the first plunger 9a, leading to a depression and consequent suction of fluid through a first suction opening 10a intercepted by a non-return suction valve.
At the same time, the fluid aspirated in the previous cycle and contained in the top part 9d of the first cylinder 9b, above the first plunger 9a, is compressed and pushed through a first delivery opening 10b, intercepted by a non-return delivery valve which communicates with a storage tank under pressure.
Symmetrically, the second plunger 11a, dragged by the displacement of the permanent magnet 7, moves in the direction of arrow D1 causing a depression in the bottom part 11c of the second cylinder 11b, under the second plunger 11a, leading to a suction of fluid through a second suction opening 12a intercepted by a non-return-suction valve.
At the same time the fluid previously sucked and contained in the upper part 11d of the second cylinder 11b, above the second piston 11a, is compressed and pushed through a second delivery opening 12b, intercepted by a non-return delivery valve that communicates with the storage tank under pressure.
In
The first plunger 94 by moving to the direction of arrow D2 determines a depression in the top part 9d of the first cylinder 9b, resulting in a suction of fluid through a third suction opening 13a intercepted by a non-return suction valve.
The previously-sucked fluid and contained in the lower part 9c of the first cylinder 9b is compressed and pushed through a third discharge opening 13b intercepted by a non-return delivery valve that communicates with the storage tank under pressure.
Symmetrically, the second plunger 11a, dragged by the displacement of the permanent magnet 7, moves to the arrow direction D2 causing a depression in the top part 11d of the second cylinder 11b, resulting in a suction of fluid through a fourth suction opening 14a intercepted by a non-return suction valve.
At the same time the fluid previously sucked and contained in the lower part 11c of the second cylinder 11b is compressed and pushed through a fourth non-return delivery valve 14b that communicates with the storage tank under pressure.
For each complete cycle, a displacement upwards in the direction D1 and a displacement downwards in the direction D2, the compressor compresses a volume of fluid equal to the volume of one of the two cylinders 9b, 11b less the volume of a plunger 9a, 11a multiplied by four:
V
cycle=(Vcylinder−Vplunger)*4, where V stands for volume (e.g. in m3).
This taking into account that the first and the second cylinder 9b, 11b have an identical volume, and that the first and the second plunger 9a, 11a have an identical volume.
A small volume occupied by the stem 8 must be subtracted from Vcycle.
The capacity of the compressor, usually expressed in cubic meters per minute, will be determined by Vcycle times the frequency of cycles per second multiplied by sixty:
Capacity(m3/min)=(Vcycle*cycles/sec)*60
A compressor as described and configured with two pistons is able to compress a volume of fluid equal to that compressed by a reciprocating compressor, moved by a rotary motor, with four pistons. The number of pistons being equal and with the same size, it can compress a double quantity of fluid.
In
For sake of simplicity, there are indicated columns A and B consisting of three electromagnets 2.
Despite the electromagnets 2 being power-supplied individually, in order to reduce the number of connections necessary for the motor's operation, the coils 3 of the electromagnets 2 of each column are preferably connected in series with each other. The power-supply of the individual coils takes place by applying voltage to the terminals T of the coils 3. It can be observed that the series connection allows to power-supply three electromagnets with only four terminals instead of six.
In this example the movable magnetic component is represented by a single cylindrical permanent magnet 7.
The electromagnet B1, of column B, is electrically powered with direct or pulsed DC current, with a polarity such as to magnetize it with a magnetic field having the same polar orientation of the permanent magnet 7. To obtain this object, for example an electronic control unit (not shown) is used connected to the windings 3. We will denote schematically the biasing mode with the symbols+B1− to indicate the positive pole applied to the lower terminal T of the coil and the negative pole to the upper terminal.
In this way, the S pole of the electromagnet B1 and the S pole of the permanent magnet repel; similarly, the N pole of the electromagnet and the N pole of the permanent magnet repel. Instead the N poles of opposite sign of the upper pole of the electromagnet and the lower S pole of the permanent magnet 7 attract.
The permanent magnet 7 at the end of the previous cycle is moved upwards relative to the electromagnet B1. The permanent magnet 7 receives a double thrust by the poles S-S and N-N and an attraction by the S-N poles upwards in the direction D1.
The permanent magnet 7 has preferably a length along the axis W equal to the distance that there is between the opposite edges of the polar extensions 5 measured parallelly to the same axis W or distance R.
The thrust, and therefore the force to compress the fluid, is proportional to the size of the electromagnets 3, the characteristics of the windings of the coils, the diameter of the permanent magnet 5, the applied voltage and resulting adsorbed amperage.
After a time in the order of milliseconds, see the right side of
After this first period of time, see
In
In
Although the linear motor can work simply by setting a timer on and alternating the power supply of the various electromagnets, it is preferable to insert two electromagnetic or photoelectric sensors 21 and 22 to signal when the permanent magnet 7 reaches the end of the stator 1 as shown in
With the sensor 22 the control unit detects the completion of the cycle and starts a new cycle as in
The operation described so far may take place by appropriately timing the biasing sequence of the coils of the electromagnets 2 by the control unit. In the calibration phase of the system one must determine at what interval such sequence should take place and what voltage to use according to the operating pressure of the compressor.
The control unit preferably comprises means for varying the voltage and frequency of the power-supply of the windings on the basis of variable operating needs. From
The stator 1 is equal to the first variant with the columns A and B offset by a distance h from each other. In this case the mode changes with which the biasing of the electromagnets 3 takes place by means of the central unit since, instead of biasing only one magnet at a time, two adjacent magnets for each column are biased at a time, that is, a pair of electromagnets at a time.
In
In the right part of
Similarly to what has been already seen in
In
Similarly to what has been already seen in
The latter double permanent magnet configuration shown in
According to the same principle, one may also use more than two stacked, adjacent permanent magnets.
At top of
In the lower part of
Note that, in the case of six columns, the corresponding columns are arranged in a tripod fashion with respect to the axis W thereby privileging axial and non-eccentric thrusts during operation. In the case of four columns, the homologous columns will be facing each other as will be seen later.
For a continuous and reliable operation the compressor may preferably envisage the use of cooled oil for the simultaneous cooling of the electromagnets 2 and the compression cylinders 9b, 11b, as well as the lubrication of the stem 8 and the bearing bushes 15 within which the stem 8 slides.
With reference to
In the abovementioned
In
In
With reference to
With reference to
In the example of
At this point,
The closure occurs with a reversed biasing mode.
With this configuration, the biasing of the electromagnets differs from what is described for the compressor and actuator, showing that the power supply and biasing mode of the electromagnets is dependent upon the number of electromagnets and the offset h between the columns.
In
With reference to
In the example of
At this point,
The closure,
Also in this case it is noted that the biasing mode of the electromagnets depends on the length of the columns A and B, the spacing Z between the poles of the electromagnets that constitute the columns, the offset h between columns A and B and the number and shape of the permanent magnetic component used. In the specific case of
For the motor, in general:
If the columns are six, three columns are to be placed in a tripod fashion each oriented towards the axis W and the same applies for the columns B, and so for more higher numbers of columns.
This way the central permanent magnet receives thrusts or attractions that compensate each other while not being subjected to eccentric but only concentric forces; and/or
the shape of the core of the electromagnets, and in particular the distance r between the expansions 5,
the spacing Z between the polar expansions of the electromagnets which make up the columns;
the magnitude of the offset h between columns;
the length of the permanent magnet;
the fact that the permanent magnetic component is constituted of a single permanent magnet or consists of several magnets stacked with opposed poles or with alternating poles in such case spaced;
Number | Date | Country | Kind |
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102015000066871 | Oct 2015 | IT | national |
Filing Document | Filing Date | Country | Kind |
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PCT/IB2016/056096 | 10/12/2016 | WO | 00 |