The disclosure relates to a generator capable of transforming the translational movement of a body into an accumulation of electric charges.
Such a generator is known from the document “Magnetostrictive-Piezoelectric composite structure for energy harvesting,” Journal of Micromechanics Microengineering, No. 22, 2012 by T. Lafont et al., which includes:
The translational movement of the magnetic field source in a parallel and overhanging plane of the converter results in the accumulation of charges in the converter. These charges can then be taken for storage and/or to supply energy to a circuit.
U.S. Pat. No. 6,984,902 discloses a device for recovering the vibratory energy of a body that also uses a converter and a field source.
However, for a given level of accumulated charge, known devices are relatively cumbersome or inefficient, making them incompatible with some targeted applications. This is particularly the case when trying to recover the energy from a small push element of a more complex device, when this push element is operated by a user (switch, operating button, etc.). In this type of application, it is important to be able to recover as many charges as possible, even when the movement is of small amplitude (from a few mm to a few cm) and low speed (from 0.01 to less than 1 m/s).
One of the aims of the disclosure is, therefore, to propose a generator, capable of transforming the translational movement of a push element into an efficient and compact accumulation of charge.
In order to achieve this goal, and according to a first aspect, the object of the disclosure proposes a generator to transform a translational movement of a push element into an accumulation of electric charges comprising:
By placing the converter in the field source housing, a compact generator is formed. The movement of the push element results in the variation of the magnetic field that the converter of a first configuration is subject to, resulting in the generation of electric charges.
According to other advantageous and unrestrictive characteristics of the disclosure, considered individually or in any technically possible combination;
According to a second aspect, the object of the disclosure proposes a generator to transform a translational movement of a push element movable from a first position to a second position, according to a translational direction, into an accumulation of electric charges, the generator comprising:
By placing the converter in the field source housing, a compact generator is formed. The movement of the push element is transmitted into a rotational movement varying the magnetic field with respect to the converter, which results in the generation of electric charges in the converter.
According to other advantageous and unrestrictive characteristics of the disclosure, considered individually or in any technically possible combination:
The disclosure will be better understood in the light of the following description of the specific and unrestricted embodiments of the disclosure with reference to the attached figures, including:
This disclosure relates to an electrical generator 1 capable of transforming the translational movement of a body, even of small amplitude (from a few mm to a few cm) and low speed (from 0.01 to less than 1 m/s), into a generation and accumulation of electric charges.
The push element 5 can be moved along a translational direction from a first position to a second position. This can be, for example, a push button that can be directly or indirectly activated in translation by a user. This translational movement can take different forms, for example, in a direction perpendicular to a main surface of the case 1a as shown in
The push element 5 can be included in a part of a more complex mechanical device, such as a switch, resulting in the translational movement of the push element 5, when this complex mechanical device is operated by the user.
As shown as an example in
The converter 2 includes a magnetostrictive layer 20 of magnetostrictive material with a preferred magnetostriction coefficient, in absolute value and in saturation, above 10 ppm, above 100 ppm, or even above 1,000 ppm. It should be recalled that this coefficient is defined by the quotient AL/L where AL is the elongation of the material in the presence of a magnetic field saturating the material, and L is the length of this material in the absence of a magnetic field.
Preferably, the material of the magnetostrictive layer 20 is chosen to be inherently isotropic or to exhibit isotropic behavior in the generator 1, as is the case when an anisotropic material is subject to a field of sufficient intensity to saturate it magnetically. It can be made of a Terfenol D, FeSiB, or a FeCo alloy block, for example.
As can be seen in
As is well known per se, the application of a magnetic field to the magnetostrictive layer 20 in a given direction in the reference plane causes the layer to deform along this determined direction (an elongation when the magnetostriction coefficient of the magnetostrictive layer 20 is greater than 0).
The magneto-electric converter 2 also comprises, assembled integrally with the magnetostrictive layer 20, at least one piezoelectric layer 21a, having electrodes 22a. In the example shown in
As the piezoelectric layers 21a, 21b are integrally joined to the magnetostrictive layer 20, the deformation of this magnetostrictive layer 20 in the reference plane also results in the deformation of the piezoelectric layers 21a, 21b in a plane parallel to this reference plane.
The piezoelectric layers 21a, 21b are preferably polarized along a polarization direction contained in the plane they define. When several piezoelectric layers 21a, 21b are present, they are advantageously arranged on the magnetostrictive layer 20 so that their polarization axes are arranged parallel to each other. It will be considered that this is the case in the coming description.
The deformation of the piezoelectric layers 21a, 21b along their polarization directions results in the creation of electric charges in these layers and the accumulation thereof on the electrodes 22a, 22b. Such deformation is obtained when the magnetostrictive layer 20 is subject to a magnetic field the orientation of which has a component parallel to the polarization direction of the piezoelectric layers 21a, 21b.
Advantageously, when the converter 2 is subject to a rotating magnetic field, the control circuit is configured to collect the charges created upon each quarter turn, for angles θ of 0°, 90°, 180° and 270°, within 30°.
A magneto-electric converter 2 is thus formed that is able to transform the variations, in the reference plane defined by the magnetostrictive layer 20, of a magnetic field into a charge accumulation at the electrodes 22a, 22b of the piezoelectric layers 21a, 21b.
It should be noted that the generator according to the disclosure is by no means limited to a converter 2 of the precise form just described. Thus, a converter 2 comprising a single piezoelectric layer 21a or comprising a plurality of magnetostrictive layers is fully compatible with the disclosure. Similarly, the electrodes 22a, 22b may take other forms or be deployed differently from what has been described in the previous paragraphs.
A generator 1 also includes a magnetic field source 3. The magnetic field source 3 defines a housing wherein a magnetic field prevails. In
The housing 4 and the source 3 are configured so that the converter 2 can be placed in the housing in such a way that at least one part of the field is placed in its reference plane. The source 3 and the converter 2 are free to move relative to each other, so that a rotating field can be created in the housing 4 opposite the converter.
Preferably, the field prevailing in the housing 4 is uniform, i.e., it has a relatively constant direction and/or intensity at least in a central part of the housing and preferably at any point of the housing. This makes it easy to place the converter in the housing 4 without having to accurately position it in a particular location.
There are multiple ways to realize the field source 3.
According to a first approach, the source 3 is formed by a flat assembly of permanent magnets oriented relative to each other so as to confine a magnetic field on one side of this plane. This assembly is well known as the “Halbach network.”
By placing two of these assemblies facing each other, with the fields facing each other, the housing 4 is defined as the space between these two planes. This configuration is shown in
In a second approach, a plurality of permanent magnets are arranged relative to each other along a closed contour to define the housing 4 and create a field within it. For example, it may be a Halbach cylinder configuration, shown schematically in
As a complementary example, it can be a closed structure made of soft iron, defining the housing, two permanent magnets of identical magnetic moment are placed opposite each other in the housing as shown in
Regardless of the chosen source 3 configuration, the converter 2 is placed in the housing 4 so that at least part of the prevailing field is placed in the reference plane.
Apart from the housing 4, there is a peripheral field that can correspond, for example, to the terrestrial magnetic field. The configuration of the peripheral field (i.e., the intensity, direction thereof) is different from the configuration of the field prevailing in the housing 4.
This disclosure takes advantage of the various elements that have just been described in detail to form a device capable of transforming the translational movement of a body into an accumulation of electric charges.
In this embodiment, the magnetic field generated by the source 3 in the housing 4 can be rotated with respect to the converter 2 along an axis perpendicular to the reference plane. This forms a rotating and, therefore, variable field in the reference plane resulting in the generation of charges on the electrodes 22a, 22b of the converter 2.
The rotation of the field can be obtained by rotating the converter 2 about itself about an axis of rotation perpendicular to the reference plane and able to pass through its center.
Alternatively, the rotating field can be obtained by holding the converter stationary and rotating the field source 3 about the axis of rotation perpendicular to the reference plane and passing through or near the center of the converter 2. This configuration, wherein the converter 2 is stationary, is particularly advantageous, as it enables the control device to be simply connected to the converter 2.
Of course, the converter 2 and the source 3 can simultaneously be rotated, as long as they are in relative movement with respect to each other, in order to rotate the field with respect to the converter 2.
Regardless of the approach chosen, the converter 2 is held in the housing and subject to the variable (e.g., rotating) magnetic field in its reference plane.
In this first embodiment of the disclosure, the generator 1 also includes a device for transmitting the translational movement of the push element 5 into a rotational movement of the source 3 or the converter 2, with an axis perpendicular to the reference plane. In other words, the translational movement of the push element 5 from a first position to a second position results in the rotational movement of the source 3 or the converter 2, preferably on itself, and along an axis perpendicular to the reference plane. As we have seen, this rotational movement results in the formation, in the housing 4 of the source 3, of a rotating magnetic field with respect to the converter 2, and in the generation and accumulation of electric charges on the electrodes 22a, 22b of the converter 2.
In this example, the field source 3 is a Halbach cylinder generating a uniform field in at least one part of the housing 4 it defines. The core of this cylinder defines the housing 4 wherein the converter 2 can be placed. As can be seen in
The configuration of the rack 9 and the gear wheel 6 should be chosen so that the movement, even of small amplitude, of the push element 5 results in the rotation of the magnetic field by an angle sufficient to accumulate a required quantity of electric charges. The source 3 can be moved in rotation by several turns when the push element 5 moves in translation from its first to its second position, or by a portion of a turn, depending on the energy required for the application.
To facilitate this, a gear reduction mechanism or a gear train 10 can be provided between the rack 9 and the gear wheel 6, a particular example of which is shown in
Advantageously, the generator 1 can be provided with a return element 11, such as a spring, to reposition the push element 5 in its first position after it has reached the second position. The return movement of the push element 5 from the second position to the first position can be used to continue generating and accumulating charges. For this accumulation to be useful, it must be ensured that the control device is capable of collecting charges in this dual mode of operation.
To ensure a maximum charge generation, especially when the rotational movement of the magnetic field is less than one revolution when the push element is activated, it is particularly advantageous to orient the converter 2 toward the field so that, in the first position, the polarization axis of the piezoelectric layer is aligned with the magnetic field prevailing in the housing 4 (or perpendicular thereto). Thus, when the push element 5 is positioned in its first position, the deformation of the converter along the direction of the polarization axis is extreme (maximum or minimum).
Many variations of this example of the first embodiment of the disclosure are possible.
Thus, the gear wheel 6 is not necessarily placed against a circular face of the cylinder 3 as shown in
In the example shown in
According to another alternative solution to this first embodiment, the push element 5 and/or the rack 9 can be equipped with a limit switch locking device, which has the effect of holding the push element 5 in this position once it has reached this extreme position. The locking device can be released by applying an additional force to the push element, and this element put into translation by taking advantage of the returning forces exerted by the return element 11. As mentioned above, this return movement can also make it possible to generate and accumulate electric charges.
The screw 15 in the example shown is positioned in a direction perpendicular to the reference plane. The screw cooperates with a nut 12, itself attached to a gear wheel 13 so that the translation of the screw along its longitudinal axis drives the nut 12 and the gear wheel 13 in rotation. The nut 12 is free to rotate about the main axis of the screw 15 only. The thread of the screw 15 and the grooving of the nut 12 are chosen to enable the reversible transmission of the rotational and translational movements of each of these parts. The gear wheel 13 engages a pinion 14 attached to an axle 7, driving the field source 3 in rotation. A return element 11, such as a spring, is used to return the push element 5 to its starting position.
Similar to the previous example, a more complex gear train, such as the one shown in
The integration of pinion and bevel gear type elements into the gearing can also enable the movement of the push element 5 so that it is placed in a different angular position than the one shown and described. And in this example, a limit switch locking device can also be provided as described in relation to the first example.
In some configurations, the pinion 14 can be omitted by providing the outer contour of the magnetic field source 3 with teeth cooperating with the gear wheel 13.
The walls 8 of the case make it possible to keep the elements of the generator 1 inside a compact volume.
As in the preceding two examples, a circular converter 2 is placed on a wall 8 of a case 1a, inside the housing 4 of a magnetic field source 3 consisting of a Halbach cylinder. The field source 3 is not attached to the support wall 8, so it is free to rotate. This movement can be facilitated by providing the support walls 8, with which it is in contact, with ball bearings, rollers, lubricants, etc.
The transmission device consists of a cylindrical body 16, with a first pattern 17 such as a groove or a helical rib. The push element 5 is attached to a circular face of the cylindrical body 16. The inside of the cylinder 3 is provided with a second pattern, a rib or a groove, complementary and cooperating with the first pattern 17 of the cylindrical body 16. A pressure on the push element 5 causes it to move in translation along an axis perpendicular to the reference plane, and causes the source 3 to rotate. The choice of the pitch of the pattern 17 makes it possible to determine the angular movement of the source 3 for the amplitude of the permitted translation of the push element 5. It is also chosen to enable the reversible transmission of the rotational and translational movements of each of these parts.
Return element 11 is in contact with the wall of the support (or with the converter 2 as shown in
As in the previous examples, the translational movement of the push element 5 results in the formation of a rotating magnetic field in the reference plane of the converter 2 and in the accumulation of charges that can be collected by the control device associated with the generator 1.
The push element 5 is fixedly attached to a transmission belt 19. The movement of the transmission belt 19 and the push element 5 is guided by at least two rollers 18a, 18b attached on a wall 8 but free to rotate on themselves. Advantageously, the transmission of the movement between the transmission belt 19 and the rollers 18a, 18b is carried out without slipping. For this purpose, a synchronous belt with teeth of a chosen shape can be used to mesh with the teeth that can be fitted to the rollers 18a, 18b. Alternatively, a transmission belt 19 can be chosen in the form of a chain.
The transmission belt 19 and the two rollers 18a, 18b form the transmission device for the translational movement of the push element 5 into a rotational movement of the magnetic field source 3 to vary this magnetic field in the reference plane of the converter.
For this purpose, a circular converter 2 is placed on the wall 8, inside the housing 4 of a magnetic field source 3 consisting of a Halbach cylinder, which can be driven into rotation by the transmission belt 19.
The translational movement of the push element 5 causes the movement of the transmission belt 19 and the rotation of the magnetic field source 3. This rotation results in the formation of a rotating magnetic field in the reference plane of the converter 2 and in the accumulation of charges that can be collected by the control device associated with the generator. The same principle could be used to move the converter 2 in rotation rather than the field source 3, in order to produce a variable field in the reference plane of the converter 2.
In this second embodiment, the push element 5 is integral with the field source 3 or the converter 2. The push element 5 can be moved in a direction perpendicular to the reference plane, and thus moves the source 3 or the converter 2 to which it is attached.
In a first position of the push element 5, the converter 2 is placed in the housing 4 of the source 3 in a foreground position and subject to a first field configuration.
“Field configuration” means the intensity and orientation of the magnetic field (in particular, with respect to the polarization direction of the converter 2) at any point in the space of the housing 4 occupied by the converter 2, at its reference plane.
The push element 5 moved to a second position moves the source 3 or the converter 2 to which it is attached. When the push element 5 is in the second position, the converter 2 is subject to a second field configuration in its reference plane. This second field configuration is different from the first.
The field variation between the first position and the second position of the push element 5 at the reference plane results in the generation of charges in the piezoelectric layer(s) 21a, 21b of the converter 2, and the accumulation thereof on the electrodes.
A return element 11, such as a spring, enables the push element 5 to be repositioned in its first or second position.
In
In this first example, the converter 2 was driven out of the housing 4 defined by the source 3. It is then no longer subject to the field prevailing in this housing 4 but to a peripheral field that is different from the housing field, of much lower intensity, and of any orientation. This field variation induces the generation of charges on the piezoelectric layers 21a, 21b of the converter 2 and the accumulation thereof on the electrodes 22a, 22b (see
To maximize the variations in the field perceived in the reference plane by the converter 2 between the first and the second position, and to be protected from possible permanent or residual magnetization effects of the magnetostrictive layer 20 (
In this example, the field source is stationary, which allows greater freedom in its sizing. In this case, a larger source 3 can be chosen in order to generate a high intensity field in the housing 4 and to maximize the potential for generating charges.
As the converter 2 is stationary, its interface with the control device is simplified.
The operation of this alternative is similar in every respect to the operation of the first example that has just been made.
In this example, the field source 3 is composed of two distinct parts 3a, 3b, each of which is capable of generating a distinct field configuration. For example, the part 3a of the source 3 is capable of creating a first field configuration oriented in a plane parallel to the reference plane and along a first direction. The part 3b of the source 3 is capable of creating a second field configuration oriented in a plane parallel to the reference plane and along a second direction, different from the first. Advantageously, this second direction forms a 90° angle with the first one. The field strength generated by the first part 3a and the second part 3b are not necessarily the same. The source 3 can be simply an assembly or a stack of permanent magnets, the moments of which are chosen to direct the fields in the determined direction. This may be, for example, a stack of two identical Halbach cylinders, offset in the stack by an angular position of 90° , within 30°.
In this particular example, the converter is attached to a wall 8 of the case 1a, so it can be easily connected to the control circuit enabling, among other things, collection of the charges.
While remaining within the framework of this example, it can be considered to have a source 3 having more than two parts 3a, 3b, each of the parts enabling generation of a field configuration distinct from the field configurations generated by the parts directly adjacent thereto. By carefully choosing the configuration of each of the fields, for example, by shifting the fields of two adjacent parts by 90° (within 30°), it is possible to simulate the application of a rotating field in the reference plane of the converter 2, when moving it in the source 3 housing. This increases the amount of collectible charges.
As in the previous example, an alternative solution can be provided, wherein the push element 5 would be attached to the converter 2, and not to the field source 3.
As can be seen on the cross-section shown in
The converter 2 placed in the housing 4 is driven in translation from a first plane parallel to the reference plane to a second plane when the push element 5 (not shown in these figures) is moved from its first to its second translational position. These two positions are shown in
The first element and the second magnetic permeable elements 25a, 25b are configured to close and direct the magnetic field onto the converter 2 in a first field configuration when the converter is in the foreground (
The first and the second magnetic elements 25a, 25b are configured to close and direct the magnetic field from the source 3 to the converter 2 in a second field configuration when the converter is in the second plane (
As in the previous examples, the field variation in the reference plane of the converter 2 between the two positions results in the generation of charges in the converter 2 and the accumulation thereof on the electrodes.
It should be noted that this exemplary implementation does not exclude that the source 3 and the converter 2, whether placed in the first or the second plane, can be moved in rotation with respect to each other to generate a variable (e.g., rotating) magnetic field with respect to the converter 2. Charges can thus be generated in the converter 2 and accumulated on the electrodes for both rotational and translational movements of the push element 5.
Of course, the disclosure is not limited to the methods of implementation described and alternative embodiments can be made without going beyond the scope of the disclosure as defined by the claims.
Number | Date | Country | Kind |
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1659088 | Sep 2016 | FR | national |
This application is a national phase entry under 35 U.S.C. § 371 of International Patent Application PCT/FR2017/052524, filed Sep. 20, 2017, designating the United States of America and published as International Patent Publication WO 2018/060568 A1 on Apr. 5, 2018, which claims the benefit under Article 8 of the Patent Cooperation Treaty to French Patent Application Serial No. 1659088, filed Sep. 27, 2016.
Filing Document | Filing Date | Country | Kind |
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PCT/FR2017/052524 | 9/20/2017 | WO | 00 |