The present invention relates generally to an electromagnetic or magnetic induction heating assembly. More specifically, the present invention discloses, in an illustrated embodiment, a magnetic or electromagnetic induction furnace or heat pump which incorporates a combination circular/rotary and outer vane shaped electrically conductive plate integrated into a central elongated and rotating element for simultaneously inductive heating the proximate located magnetic plates as well as redirecting the heated air out of the furnace cabinet. A controller is provided for adjusting the strength (or turning on and off) of a plurality of electromagnets secured to each of the magnetic plates and in order to switch the furnace between a thermostat heat adjustable mode or a non-heating fan mode in which the electromagnets are deactivated and the generation of heat prevented from occurring. When conductive plates are demagnetized the fluid flow will absorb heat from the fluid generating cold and reverting the functionality of the device into a magnetic refrigerator or magnetic air conditioner. The individual rotating conductor plates incorporated into the rotating element can also include varying interior chamber designs with different combination airflow or fluid flow configurations in order to provide the combined aspects of inductive heating (owing to rotation relative to the magnetic plates) and concurrent air redirection through the furnace outlet. Other variants include applications of the present technology reconfigured as a magnetic heat pump (MHG), such utilizing a magneto-caloric effect (MCE), for providing either of heating or cooling properties resulting from the magnetization (heat) or demagnetization (cold) cycles.
The phenomena of induction heating is well known in the prior art by which heat is generated in an electrically conductive object by the generation of eddy currents. The typical induction heater includes an electronic oscillator which passes a high frequency alternating current through an electromagnet. The eddy currents flowing through the resistance of the material in turn heat it. Put another way, the eddy currents result in a high-frequency oscillating magnetic field which causes the magnet's polarity to switch back and forth at a high-enough rate to produce heat as byproduct of friction.
One known example of a prior art induction heating system is taught by the electromagnetic induction air heater of Garza, US 2011/0215089, which includes a conductive element, a driver coupled to the conductive element, an induction element positioned close to the conductive element, and a power supply coupled to the induction element and the driver. Specifically, the driver applies an angular velocity to the rotate the conductive element about a rotational axis. The power supply provides electric current to the induction element to generate a magnetic field about the induction element such that the conductive element heats as it rotates within the magnetic field to transfer heat to warm the cold air flow streams. The cold air flow streams are circulated about the surface of the conductive element and directed by the moving conductive element to generate warm air flow streams from the conductive element.
Also referenced is the centrifugal magnetic heating device of Hsu 2013/0062340 which teaches a power receiving mechanism and a heat generator. The power receiving mechanism further includes a vane set and a transmission module. The heat generator connected with the transmission module further includes a centrifugal mechanism connected to the transmission module, a plurality of bases furnished on the centrifugal mechanism, a plurality of magnets furnished on the bases individually, and at least one conductive member corresponding in positions to the magnets. The vane set is driven by nature flows so as to drives the bases synchronically with the magnets through the transmission module, such that the magnets can rotate relative to the conductive member and thereby cause the conductive member to generate heat.
The present invention discloses, without limitation, an electromagnetic or magnetic induction heating system, this including each of a housing having a fluid inlet (can be an air or liquid fluid either hot or cold), a sleeve shaped support extending within the housing, and a plurality of spaced apart magnetic or electromagnetic plates, each of which can include an individual sub-plurality of electro-magnets, communicated with the air or other fluid inlet, the plates extending radially from the sleeve support.
An elongated conductive component is rotatably supported about the sleeve support, the conductive component incorporating a plurality of linearly spaced apart and radially projecting conductive plates which alternate with the axially spaced and radially supported electro-magnetic plates. A motor rotates the conductive component such that rotation of the conductive plates relative to the electro-magnetic plates results in the creation of an oscillating magnetic field for conditioning of the fluid by either heating or cooling of the fluid.
A controller adjusts an intensity of the magnetic fields in order to adjust a level of conditioning of the airflow or fluid flow produced by rotation of the conductive component. The conductive component, via its rotation, communicates the conditioned fluid through an outlet of the housing.
A shaft extends from the motor to the conductive component and is configured to dissipate heat generated within the conductive component at a mounting location with the shaft. In one non-limiting configuration the shaft is configured to induce a heat dissipating airflow through the mounting location to an external location of the housing.
In another configuration, the shaft includes a grid of air passageway inducing and intersecting radial and axial channels. In a further configuration, the shaft alternatively exhibits a spiraling pattern. A still further configuration includes the shaft having a squirrel fan arrangement with a plurality of axial extending louvers within the mounting location.
Additional features include each of the conductive plates being arranged as a pair of opposing plates assembled into a disk package and defining an interior airflow or fluid flow influencing an outwardly spiraling pattern. The conductive plates can further include an outer circumferential array of channeling and redirecting vanes for pushing the inductive heated or cooled air or fluid through the fluid outlet. A second and inner circumferential array of channeling and redirecting vanes are provided for pushing the inductive heated air through from the inlet to the outer array of redirecting vanes.
Other features include brackets extending from the sleeve to end mounting locations within said housing, a cylindrical outer wall extending between the mounting locations to define an outer cylindrical chamber surrounding the electro-magnetic plates. The conductive component further includes end walls and an interconnecting second cylindrical wall interconnecting each of the conductive plates and extending around the electro-magnetic plates to define an inner cylindrical chamber within the outer cylindrical chamber.
A thermostat is provided in communication with the controller and operates in a first mode for adjusting the intensity of the electro-magnetic fields, with the controller operating in a second mode to turn the electro-magnets off in order to operate in a fan mode. When conductive plates are demagnetized the fluid flow will absorb heat from the fluid generating cold and will operate as magnetic refrigerator or magnetic air conditioner.
Reference will now be made to the attached drawings, when read in combination with the following detailed description, wherein like reference numerals refer to like parts throughout the several views, and in which:
As previously described, the present invention discloses a magnetic or electromagnetic induction system for providing either of heating or cooling of a conditional fluid flow. In the non-limiting illustrated embodiment, the present invention further discloses a magnetic induction furnace, illustrated at 10 in
As will be further described in detail, the conductive plate geometry concurrently redirects the conditioned (heated or cooled) fluid out of the furnace cabinet. The fluid in the illustrated embodiment is further shown as an airflow however the invention also contemplates utilizing other gases or liquids as heat transfer mediums according to a desired assembly for convecting or conducting the inductive conditioned fluid flow to a suitable outlet.
Referring initially to
The central support is fixedly mounted in the variant of
It is further understood, without limitation, that the electromagnetic plates can be solid or can include an outermost disk portion from which extend radial rib supports as further shown at 40 for selected plate 30). Additional non-limiting embodiments of the present invention further contemplate substituting the electromagnetic plates with magnetic plates (such as configured from rare earth materials).
A controller 42 is located within the furnace housing (such as in the illustrated embodiment being located within the central sleeve 18). A plurality of wiring connections, see at 44, 46, 48, et seq., extend from the controller 42 both along the inner sleeve support 18 and radially outwardly along the extending rib supports 40 and connect to individual pluralities of electromagnets arranged around a circumference of each plate, and as shown at 50, 52, 54, et seq. for selected magnetic plate 30.
A thermostat input of conventional design is connected to the controller 42 (such as wired or wirelessly connected) and can be programmed or adjusted in order control the intensity of the magnetic fields induced into the individual pluralities of electromagnets, and which in turn varies the intensity of the inductive heat generated by the oscillating field created between the alternating pluralities of conductor plates and electro-magnetic plates. The controller can also deactivate (turn off) the electromagnets incorporated into the electromagnetic plates in order to operate the furnace in a fan mode, and without any inductive heat being generated between the rotating and airflow redirecting conductor plates and the alternating array of electromagnetic plates.
As is further understood, alternative assemblies and applications of the present invention further envision integrating with any known type of external air conditioner or other refrigeration device while engaged in the fan mode, as well as the ability to contribute to a magnetic refrigeration operation during demagnetization. This further contemplates combining ambient air or other fluid along with a further chilled air inlet source (such as associated with an outside AC compressor), this further provided through any of separate or combined fluid flows, and in order to vary the output fluid flow properties from the housing.
A blower style motor 74 or like rotational inducing component is provided with an extending stem or rotating shaft 76 (see also direction of rotation 77), the shaft in turn being anchored to a first location 78 for supporting and rotating the elongated conductive element (56/58) proximate to the location of the motor. The shaft 76 is further supported in a journaled or channeled fashion at one or more additional rotational support locations, such as depicted at 80 in order to position and stabilize the elongated conductor plate assembly during rotation relative to the interior arrayed and alternating electromagnetic plates 30-38. In the illustrated embodiment, the motor 74 is static mounted within the interior of the furnace enclosure 10 however it is envisioned that, in future embodiments, the motor can be repositioned outside of the furnace enclosure. Without limitation, the present invention further contemplates the motors described herein being housed in the cabinet so as to capture the heat losses generated by the motor drives, these having been calculated to account for up to 8% of the actual motor power.
The motor 74 is thus configured to rotate the elongated conductive element (see again end wall 56 and outer perimeter wall 58) along with the associated conductive plates 60-68 according to a given rotational speed. This is again necessary to both induce the varying electromagnetic fields to inductive heat the electromagnetic plates 30-38 (with their individual electromagnet arrays) owing to the alternating fields generated by the rotation of the proximate located metallic conductive plates, as well as the air inducing and redirecting architecture of the conductive plate disk packages, these operating to concurrently draw outwardly and redirect the air from the central (cold) inlet, across the magnetic plates in conductive heating fashion, and out an upper end furnace exit 82. It is further envisioned that the present assembly can be applied to any material which is magnetized, such including any of diamagnetic, paramagnetic, and ferromagnetic materials without exemption also referred to as magnetocaloric materials (MEMs).
Additional variables can include varying the designing of the conductive plates, such as not limited varying a thickness, positioning or configuration of a blade or other fluid flow redirecting profile integrated into the conductive plates, as well as utilizing the varying material properties associated with different metals or alloys, such including ferromagnetic, paramagnetic and diamagnetic properties.
A blower door (a portion of which is illustrated at 83 in
One issue encountered with the arrangement of the motor 74 within the interior of the furnace or like housing enclosure is the instance of heat buildup from induction heating adversely affecting motor operation. In an attempt to ameliorate the effects of heat on the motor, the present invention further includes heat dissipation structure incorporated into the fixed axial mounting location depicted by the journal shaft support at 78, and such as is established between the motor extending shaft 76 and the axial supporting location of the conductor plate subassembly (this further again referenced by the mounting support provided again at 78 approximate the central location of end wall 56 of the conductor plate subassembly).
Referencing first
In each variant illustrated, the shaft is depicted at a channeled location (again at 80 in the example of
Referring now to
The conductive plate 114 (as well as the corresponding disk package of
Reconciling the partial cutaway illustration of the conductive plate location in
To this end, the sleeve 18 can be aperture or sectioned, in part or in whole, at locations which coincide with the arrangement of the individual conductive plates 60-68. The present invention further contemplates the fluid inlet being separate from the electromagnetic plate support sleeve 18 and by which the ambient fluid (e.g. air) admittance is provided a location between the outside of the sleeve 18 and the open interior of the electromagnetic plates as separated by the radial rib supports 40 (see also again
Proceeding to
Finally,
As with the previous embodiments, the vane patterns associated with the conductive plates can be configured in any shape or pattern to facilitate redirection of the inductive heated airflow from a central inlet location (arrows 176), interior redirecting location (arrows 178 across inner vane pattern), and outwardly (arrows 180 across second reversing vane pattern) in the manner illustrated in
Other and additional envisioned applications of the present technology can include adapting the present technology for use in magnetic heat pump (MHG) applications or magnetic refrigerators (MR), such utilizing a magneto-caloric effect (MCE) provide either of heating or cooling properties resulting from the magnetization (heat) or demagnetization (cold) cycles. The goal in such applications is to achieve a coefficient of performance (defined as a ratio of useful heating or cooling provided to work required) which is greater than 1.0. In such an application, the system operates to convert work to heat as well as additionally pumping heat from a heat source to where the heat is required (and factoring in all power consuming auxiliaries). As is further known in the relevant technical art, increasing the COP (such as potentially to a range of 2.0-3.5 or upwards) further results in significantly reduced operating costs in relation to the relatively small input electrical cost required for rotating the conductive plate(s) relative to the magnetic plate(s). Such magnetic refrigeration techniques result in a cooling technology based on the magneto-caloric effect and which can be used to attain extremely low temperatures within ranges used in common refrigerators.
As is further known in the relevant technical art, the magneto-caloric effect is a magneto-thermodynamic phenomenon in which a temperature change of a suitable material is again caused by exposing the material to a changing magnetic field, such being further known by low temperature physicists as adiabatic (defined as occurring without gain or loss of heat) demagnetization. In that part of the refrigeration process, a decrease in the strength of an externally applied magnetic field allows the magnetic domains of a magneto-caloric material to become disoriented from the magnetic field by the agitating action of the thermal energy (phonons) present in the material.
If the material is isolated so that no energy is allowed to (re)migrate into the material during this time, (i.e., again the adiabatic process) the temperature drops as the domains absorb the thermal energy to perform their reorientation. The randomization of the domains occurs in a similar fashion to the randomization at the curie temperature of a ferromagnetic or paramagnetic material, except that magnetic dipoles overcome a decreasing external magnetic field while energy remains constant, instead of magnetic domains being disrupted from internal ferromagnetism (or paramagnetism) as energy is added. Applications of this technology can include, in one non-limited application, the ability to heat a suitable alloy arranged inside of a magnetic field as is known in the relevant technical art, causing it to lose thermal energy to the surrounding environment which then exists the field cooler than when it entered.
Other envisioned applications include the ability to generate heat utilizing either individually or in combination rare earth magnets placed into a high frequency oscillating magnetic field as well as static electromagnetic field source systems including such as energized electromagnet assemblies which, in specific instances, can be combined together within a suitable assembly not limited to that described and illustrated herein and for any type of electric induction, electromagnetic and magnetic induction application.
Additional features may include the ability to configure turbine blades as magnetized elements that can generate heat or cold. It is further envisioned that the present assembly can be applied to any material which is magnetized, such including any of diamagnetic, paramagnetic, and ferromagnetic materials without exemption also referred to as magnetocaloric materials (MEMs).
Additional factors include the ability to reconfigure the assembly so that the frictionally heated fluid existing between the overlapping magnetic and rotating conductive plates may also include the provision of additional fluid mediums (both gaseous and liquid state) for better converting the heat or cooling configurations disclosed herein.
Other envisioned applications can include the provision of capacitive and resistance (ohmic power loss) designs applicable to all materials/different configurations as disclosed herein.
The present invention also envisions, in addition to the assembly as shown and described, the provision of any suitable programmable or software support mechanism, such as including a variety of operational modes. Such can include an Energy Efficiency Mode: step threshold function at highest COP (at establish motor drive rpm) vs Progressive Control Mode: ramp-up curve at different rpm/COPs).
Given the above description, the present invention additionally envisions numerous techniques, teachings and factors for modifying the temperature range of heating or cooling which can be accomplished for the variants described herein. This can include modifying the rotational speed (such as measured in RPM' s or revolutions per minute) of the conductive plates, thereby affecting the magnetic or electromagnetic induction (magnetic field created) and, consequently, adjusting the eddy currents created in the conductive plates. With higher rotation the oscillating high frequencies of the magnetic/electromagnetic induction increases the temperature in the case of heating and also creates higher demagnetization forces (once the magnetic/electromagnetic induction is “off”) that can absorb more heat if exposed to a fluid flow (in the case of inductive cooling).
Other heat/cooling adjustment variables can involve modifying the degree of magnetic friction created, such as by varying the distance between the conductive plates and alternating arranged magnetic/electromagnetic plates. A further variable can include limiting the exposure of the conductive fluid (gas, liquid, etc.,) to the conductive component, such that a no flow condition may result in raising the temperature (and which can be controllable for certain periods of time).
As is further generally understood in the technical art, temperature is limited to Curie temperature, with magnetic properties associated with losses above this temperatures. Accordingly, rare earth magnets, including such as neodymium magnets, can achieve temperature ranges upwards of 900° C. to 1000° C.
Ferromagnetic Materials, such as again which can be integrated into the conductive plates, can include any of Iron (Fe) having a Curie temperature of 1043K (degrees Kelvin), Cobalt (Co) having a Curie temperature of 1400K, Nickel (Ni) having a Curie temperatures of 627K and Gadolinium (Gd) having a Curie temperature of 292K.
According to these teachings, Curie point, also called Curie Temperature, defines a temperature at which certain magnetic materials undergo a sharp change in their magnetic properties. In the case of rocks and minerals, remanent magnetism appears below the Curie point—about 570° C. (1,060° F.) for the common magnetic mineral magnetite. Below the Curie point—by non-limiting example, 770° C. (1,418° F.) for iron—atoms that behave as tiny magnets spontaneously align themselves in certain magnetic materials.
In ferromagnetic materials, such as pure iron, the atomic magnets are oriented within each microscopic region (domain) in the same direction, so that their magnetic fields reinforce each other. In antiferromagnetic materials, atomic magnets alternate in opposite directions, so that their magnetic fields cancel each other. In ferromagnetic materials (this defined as the pertaining to a substance such as ferrite in which the magnetic moments of some neighboring atoms point in opposite directions, with a net magnetization still because of differences in magnitudes of the opposite moments), the spontaneous arrangement is a combination of both patterns, usually involving two different magnetic atoms, so that only partial reinforcement of magnetic fields occurs.
As a further subset teaching, paramagnetic cooling can be simply described as employing materials that cannot be pulled by the magnet”. When a paramagnetic material is cooled excessively, the heat transfer of its molecules is reduced, as in other materials.
As a related teaching, magnetic cooling also exploits the relationship between the effects of the magnetic field strength of an applied field and the entropy of an object. One particular method of magnetic cooling is Adiabatic Demagnetization, which capitalizes on the paramagnetic properties of some materials to cool those materials (usually in gaseous form) down into the milli-Kelvin—or colder—range. This method can also be used to cool solid objects, but the most drastic cooling in the fractions of a kelvin range are generally accomplished for low-density gases that have already been greatly cooled (around 3-4 K).
The process of Adiabatic Demagnetization can include a sample first being cooled (typically a gas) and allowed to touch a cold reservoir (which has a constant temperature of around 3-4 degrees Kelvin, and is often liquid Helium), at which point a magnetic field is induced in the region of the sample. Once the sample is in thermal equilibrium with the cold reservoir, the magnetic field strength is increased, resulting in the entropy of the sample decreasing and as the system becomes more ordered as particles align with the magnetic field. While this is occurring, the temperature of the sample is still the same as that of the cold reservoir.
The sample is then isolated from the cold reservoir, and the magnetic field strength is reduced. At this point, the entropy of the sample remains the same, but its temperature drops in reaction to the reduction in the magnetic field strength. If the sample was already at a fairly low temperature, this temperature decrease can be ten-fold or greater. Repeating the process results in the sample being cooled to very low temperatures.
Given the above, raising the temperature to the Curie point for any of the materials in these three classes entirely disrupts the various spontaneous arrangements, and only a weak kind of more general magnetic behavior, called paramagnetism, remains. As is further known, one of the highest Curie points is 1,121° C. (2,050° F.) for cobalt. Temperature increases above the Curie point produce roughly similar patterns of decreasing paramagnetism in all three classes of materials such that, when these materials are cooled below their Curie points, magnetic atoms spontaneously realign so that the ferromagnetism, antiferromagnetism, or ferrimagnetism revives. As is further known, the antiferromagnetic Curie point is also referenced as the Néel temperature.
Beyond the instant disclosure, other factors or variable controlling the temperature output can include the strength of the magnets or electromagnets which are incorporated into the plates, such as again by selected rare earth magnets having varying properties or, alternatively, by adjusting the factors associated with the use of electromagnets including an amount of current through the coils, adjusting the core ferromagnetic properties (again though material selection) or by adjusting the cold winding density around the associated core.
Other temperature adjustment variables can include modifying the size, number, location and orientation of the assemblies (elongated and plural magnet/electromagnet and alternative conductive plates). Multiple units or assemblies can also be stacked, tiered or otherwise ganged in order to multiply a given volume of conditioned fluid which is produced.
Additional variables can include varying the designing of the conductive plates, such as not limited varying a thickness, positioning or configuration of a blade or other fluid flow redirecting profile integrated into the conductive plates, as well as utilizing the varying material properties associated with different metals or alloys, such including ferromagnetic, paramagnetic and diamagnetic properties.
Having described my invention, other and additional preferred embodiments will become apparent to those skilled in the art to which it pertains, and without deviating from the scope of the appended claims. The detailed description and drawings are further understood to be supportive of the disclosure, the scope of which being defined by the claims. While some of the best modes and other embodiments for carrying out the claimed teachings have been described in detail, various alternative designs and embodiments exist for practicing the disclosure defined in the appended claims.
The present application is a continuation in part of U.S. Ser. No. 16/519,437 filed Jul. 23, 2019. The present application also claims the priority of provisional application U.S. Ser. No. 62/765,131 filed Aug. 16, 2018.
Number | Date | Country | |
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62703128 | Jul 2018 | US | |
62765131 | Aug 2018 | US |
Number | Date | Country | |
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Parent | 16519437 | Jul 2019 | US |
Child | 16535331 | US |