The present specification generally relates to heat transfer systems and, more specifically, directing radiated heat from one object to another object.
Heat transfer systems generally use heat conduction and/or heat radiation principles. In these systems, heat is transferred via conduction and/or radiation amongst objects near a heat source. Most commonly, heat receiving structures are positioned to surround the heat source. As such, as heat is emitted from the heat source, each of the heat receiving structures receives a portion of the heat emitted from the heat source. This is inefficient and does not direct the heat to a specific heat receiving structure.
In one embodiment, a multi-mode heat transfer system is provided. The heat transfer system includes an emitter device. The emitter device includes an inner core surrounded by an outer core having a thickness and an outer surface. A composite material pattern extends through at least a portion of the outer surface and at least a portion of the thickness of the outer core and is thermally coupled to the inner core. The composite material pattern directs a heat from the inner core to an object other than the emitter device.
In another embodiment, a power transfer system is provided. The power transfer system includes an emitter device and a receiver device. The emitter device includes an inner core and an outer core having a thickness that circumferentially surrounds the inner core and a composite material pattern. The outer core having materials that includes at least one high thermal conductivity material inlay and a low thermal conductivity material matrix. The composite material pattern is formed by the materials. The composite material pattern extends a length of the emitter device in a system vertical direction and is positioned within a portion of the thickness of the outer core. The emitter device is positioned spaced apart from the receiver device. The composite material pattern directs a power from the emitter device to the receiver device.
In yet another embodiment, a multi-mode heat transfer system is provided. The heat transfer system includes an emitter device and a receiver device. The emitter device includes an inner core and an outer core having a thickness that circumferentially surrounds the inner core, and a composite material pattern. The outer core having materials that alternate between a high thermal conductivity material inlay and a low thermal conductivity material matrix. The composite material pattern is formed within the alternating materials. The composite material pattern extends a length of an outer surface of outer core in a system vertical direction and is positioned within a portion of the thickness of the outer core. The composite material pattern includes a tear drop region that surrounds the inner core, a flux field region surrounds at least a portion of the tear drop region, a plurality of curved segments that surround the inner core and are positioned within and outside of the tear drop region, and a plurality of partial ellipses segments are positioned within the tear drop region. The composite material pattern further includes a plurality of curvilinear segments and a plurality of non-linear segments positioned within the flux field region but not within the tear drop region. The emitter device is positioned spaced apart from the receiver device. The composite material pattern is directed to the receiver device and directs a heat from the emitter device to the receiver device.
These and additional features provided by the embodiments described herein will be more fully understood in view of the following detailed description, in conjunction with the drawings.
The embodiments set forth in the drawings are illustrative and exemplary in nature and not intended to limit the subject matter defined by the claims. The following detailed description of the illustrative embodiments can be understood when read in conjunction with the following drawings, where like structure is indicated with like reference numerals and in which:
Embodiments described herein generally relate to a multi-mode (i.e., radiation and conduction) heat transfer system. In some embodiments, the multi-mode heat transfer system is used in thermal protection systems. In other embodiments, the multi-mode heat transfer system is used in high temperature thermal energy harvesting and the like. The multi-mode heat transfer system includes an emitter device and at least one spaced apart receiving device. The emitter device is positioned to selectively transmit a heat and/or power in the far field towards a colder body receiver, such as the at least one spaced apart receiving device. As such, the multi-mode heat transfer system takes a heat from the emitter device and directs the heat to an area where the heat may be beneficial and/or may not cause harm. For example, a heat generated by a hot body engine may be directed, by the emitter device, to the receiving device positioned in an engine compartment area that has ample intake of air to cool the heat. In another example, a heat generated by a component in an aerospace application, such as a hot body solar receiver, may be directed, by the emitter device, to another receiving device, such as a sail that is coupled to another component (e.g., a fly-by-light sailcraft) that requires, or works more efficient, when receiving heat and associated directed radiated power.
The emitter device may be generally cylindrical in shape with an outer core that has a thickness and circumferentially surrounds an inner core. It should be understood that the emitter device may be other shapes including rectangular, square, hexagonal, non-regular geometries, and the like. In some embodiments, the outer core may be formed from a plurality of annular rings that include alternating materials between a high thermal conductivity material inlay and a low thermal conductivity material matrix, such as carbon aerogel or polydimethylsiloxane (PDMS) material that circumferentially surrounds the inner core. In other embodiments, the outer core may be formed from three-dimensional printing alternating between the high thermal conductivity material inlays and the low thermal conductivity material matrix that circumferentially surround the inner core. That is, an anisotropic thermal conductivity of the outer core and its surface emissivity of the outer surface is optimized to direct heat from the emitter device to the at least one receiver. A focused radiation is attained by optimizing the layout of the high thermal conductivity material inlays and the low thermal conductivity material matrix plus angularly varying the emissivity surface profile.
A composite material pattern extends a length of the emitter device in a system vertical direction and extends through at least a portion of the outer surface and the thickness of the outer core. The composite material pattern is thermally coupled to the inner core of the emitter device. Further, the composite material pattern directs the heat from the inner core to the receiver device without directing heat, or significantly less heat, to other objects such as a second receiver device.
As used herein, the term “system longitudinal direction” refers to the forward-rearward direction of the system (i.e., in the +/−X-direction depicted in
Now referring to
In some embodiments, each of the receiver devices 14, 16 is generally cylindrical in shape with an outer surface 34a, 34b respectively. In some embodiments, the cylindrical shape is formed from a solid conductive material 36a, 36b. In other embodiments the cylindrical shape is formed from a plurality of layers. As such, the outer surface 34a, 34b of each of the receiver devices 14, 16 is generally a solid surface. In some embodiments, the solid conductive material 36a, 36b is copper. In other embodiments, the solid conductive material 36a, 36b is titanium, aluminum, silver, gold, silicon, graphite composite, and the like. In other embodiments, each of the receiver devices 14, 16 is a square shape, a flat shape, a rectangular shape, a hexagonal shape, an octagonal shape, and the like. Further, in other embodiments, the shape of each of the receiver devices 14, 16 is an irregular shape.
In some embodiments, each of the receiver devices 14, 16 are equally spaced from the emitter device 12. In a non-limiting example, each of the receiver devices 14, 16 are spaced apart 350 millimeters from the emitter device 12. It should be understood that each of the receiver devices 14, 16 may be spaced apart greater than 350 millimeter distance and/or less than the 350 millimeters distance. Further, in some embodiments, the receiver devices 14, 16 may be offset in unequal distances from the emitter device 12. For example, the first receiver device 14 may be positioned 350 millimeters from the emitter device 12 and the second receiver device 16 may be positioned 300 millimeters from the emitter device.
It should be appreciated that each of the receiver devices 14, 16 may extend 500 millimeters in the system vertical direction (i.e., in the +/−Z direction) from a coupling component 31a, 31b (i.e. a cooling structure, another device that can take on the heat from the emitter device 12, and the like). It should be appreciated that this is a non-limiting example and each of the receiver devices 14, 16 may extend more than or less than 500 millimeters. It should also be appreciated that each of the receiver devices 14, 16 may extend at different heights than the emitter device 12, at different heights than the other one of the receiver devices 14, 16, and the like. Further, in some embodiments, the distance between the receiver devices 14, 16 that define the gap 18 and/or the distance between each of the receiver devices 14, 16 and the emitter device 12 may be a ratio based on the height that the emitter device 12 extends in the system vertical direction (i.e., in the +/−Z direction) from a heated coupling component 30, as discussed in greater detail herein. Further, in some embodiments, each of the receiver devices 14, 16 may have a diameter of 200 millimeters. It should be appreciated that in some embodiments, the first receiver device 14 may have a greater diameter than the second receiver device 16, and vice versa. Further, in some embodiments, each of the receiver devices 14, 16 may have an equal diameter that is greater than and/or less than 200 millimeters.
Now referring to
In other embodiments, the emitter device 12 is a square shape, a rectangular shape, a hexagonal shape, an octagonal shape, other uniform and non-uniform geometric shapes, and the like. Further, in other embodiments, the shape of the emitter device 12 is an irregular shape. Further, in some embodiments, regardless of the shape, the high thermal conductivity material inlays 26a and the low thermal conductivity material matrix 26b may extend radially from and/or may circumferentially surround the inner core 22 such that the inner core 22 may be positioned to extend in the system vertical direction (i.e., in the +/−Z direction) within the shape of the emitter device 12. In some embodiments, the inner core 22 is centrally positioned with respect to the outer surface 20 of the emitter device 12. In other embodiments, the inner core 22 is positioned offset to the center with respect to the outer surface 20 of the emitter device 12.
In some embodiments, the inner core 22 is a high thermal conductivity material. For instance, the inner core 22 may be a copper material. In other embodiments, the inner core 22 may be a diamond material, a silver material, a gold material, an aluminum nitride material, a silicon carbide material, an aluminum material, a tungsten material, a graphite material, a zinc material, a combination thereof, and the like. Further, in some embodiments, the inner core 22 is an embedded heat source such as a cartridge heater. In this embodiment, the inner core 22 may be tubular and configured to receive a heat from another component, such as an engine, a semiconductor device, and the like. In some embodiments, the diameter of the inner core 22 is 20 millimeters. In other embodiments, the diameter of the inner core 22 is greater than and/or less than 20 millimeters. The inner core 22 is thermally coupled to the composite material pattern 28 such that the heat from the inner core 22 is directed to the first receiver device 14 via the composite material pattern 28, as discussed in greater detail herein. For example, in experimentation, the inner core 22 was a 100 W heat source.
Still referring to
The emitter device 12 may extend in the system vertical direction (i.e., in the +/−Z direction) from the heated coupling component 30 (i.e., an engine, a semiconductor device, and the like) and each of the receiver devices 14, 16 may extend 500 millimeters in the system vertical direction (i.e., in the +/−Z direction) from the coupling component 31a, 31b, as shown in
Further, in some embodiments, the emitter device 12 and one or both of the pair of receiver devices 14, 16 may extend in the system vertical direction (i.e., in the +/−Z direction) from the heated coupling component 30. In other embodiments, the emitter device 12 and one or both of the pair of receiver devices 14, 16 may extend in the system vertical direction (i.e., in the +/−Z direction) from either or both of the coupling components 31a, 31b. In other embodiments, it is understood that the emitter device 12 and one or both of the pair of receiver devices 14, 16 may extend in other directions besides in the vertical direction from the heated coupling component 30, from either or both of the coupling component 31a, 31b, and the like. For instance, the emitter device 12 and one or both of the pair of receiver devices 14, 16 may extend in a lateral direction (i.e., in the +/−Y direction) in the longitudinal direction (i.e., in the +/−X direction) and a combination thereof from the heated coupling component 30, from either or both of the coupling component 31a, 31b, and the like. As such, it should be appreciated that there may be a plurality of spatial relationships between the receiver devices 14, 16 and the emitter device 12.
Now referring to
Referring to
In some embodiments, the first receiver device 14 is positioned in an area that is configured to receive heat. For example, in aerospace applications, one component, such as a sail may be coupled to another component (e.g., a fly-by-light sailcraft) that may need, or works more efficient, when receiving additional heat and associated directed radiated power. As such, the one component may be coupled to the first receiver device 14 such that the emitter device 12 may direct radiated heat to the first receiver device 14 in order to provide heat to the coupled component. In another example, a heat generated from a hot body engine may be captured by the inner core 22 and then transferred to the first receiver device 14 such that unwanted heat from the hot body engine may be transferred to another area within the vehicle. In other embodiments, the heat radiated from the emitter device 12 is forced into ambient air. For example, heat from the engine hot body may be directed, by the composite material pattern 28 of the emitter device 12, to an object positioned in an area of an engine compartment in which air is directed out of the engine compartment.
The composite material pattern 28 may be a plurality of shapes. As such, it should be appreciated that the composite material pattern 28 may be optimized for each specific application. In some embodiments, the composite material pattern 28 includes a plurality of uniform shapes. In other embodiments, the composite material pattern 28 includes irregular shapes. In other embodiments, the composite material pattern 28 includes both uniform and irregular shapes.
Now referring to
It should be appreciated, that in some embodiments, the composite material pattern 28 spans θ=−90° to θ=90° nearest to the second receiver device 16 with the composite material pattern 28 focusing the high thermal conductivity material inlays 26a directed towards the first receiver device 14. In some embodiments, the high thermal conductivity material inlays 26a are 2 millimeters thick at a 3 millimeter spacing in the composite material pattern 28. It should be understood that the high thermal conductivity material inlays 26a may be less than or more than 2 millimeters thick at less than or more than 3 millimeter spacing in the composite material pattern 128.
Now referring to
In the second aspect, the composite material pattern 128 includes a teardrop region 138 that surrounds the inner core 122. The teardrop region 138 is centered around an axis A1 and extends in the longitudinal direction (i.e., in the +/−X direction) from one side of the inner core 122. The composite material pattern 128 further includes a plurality of linear segments 140 extending vertically from an apex 142 of the teardrop region 138 and extend a length of the outer surface 120 of the emitter device 112 in the system vertical direction (i.e., in the +/−Z direction) to transverse the outer core 124, illustrated as the plurality of annular rings.
That is, it should be appreciated that in embodiments in which the outer core 124 is the plurality of annular rings, the plurality of annular rings are stacked on one another to form a column, as best seen in
It should be appreciated that when the plurality of annular rings are stacked, the high thermal conductivity material inlays 126a and the low thermal conductivity material matrix 126b may align with the high thermal conductivity material inlays 126a and the low thermal conductivity material matrix 126b of an adjacent annular ring to form the composite material pattern 128. As such, it should be appreciated that the composite material pattern 128 in
A plurality of linear segments 140 of the composite material pattern 128 extend vertically along a portion of the outer surface 120 and into at least a portion of the thickness of the emitter device 112. In some embodiments, the plurality of linear segments 140 curve inward towards the inner core 122 at the apex 142 of the teardrop region 138. In some embodiments, the composite material pattern 128 is uniform along the length of the outer surface of the emitter device 112 in the system vertical direction (i.e., in the +/−Z direction). In other embodiments, the composite material pattern 128 includes a widening pattern in the system lateral direction (i.e., in the +/−Y direction) such that the widest portion of the composite material pattern 128 is near a center 144 of the outer surface 120 of the emitter device 112. That is, the composite material pattern 128 is narrower in width at ends 146a, 146b than at the center 144.
Further, in some embodiments, the composite material pattern 128 transverses the outer core 124 (i.e., extends the entire length of the outer surface 120 of the outer core 124 of the emitter device 112 in the system vertical direction (i.e., in the +/−Z direction)). In other embodiments, as best seen in
Now referring to
Further, it should be appreciated that, in some embodiments, the composite material pattern 228 spans θ=−90° to θ=90° nearest to the second receiver device 16 with the composite material pattern 128 focusing the high thermal conductivity material inlays 126a directed towards the first receiver device 14. In some embodiments, the high thermal conductivity material inlays 126a are less than 1 millimeter thick at a variable millimeter spacing throughout the composite material pattern 128. It should be understood that the high thermal conductivity material inlays 126a may be more than 1 millimeter thick and the variable millimeter spacing may be uniform and/or non-uniform as described herein with respect to the composite material pattern 228.
The composite material pattern 228 includes the teardrop region 238 that surrounds the inner core 222 and also includes the plurality of linear segments 240 extending vertically from the apex 242 of the teardrop region 238. Further, the plurality of linear segments 240 extend a length of the outer surface 220 of the emitter device 212 in the system vertical direction (i.e., in the +/−Z direction) to transverse the outer core 24 (i.e., extends the length of the outer surface 20 of the outer core 24 of the emitter device 12 in the system vertical direction (i.e., in the +/−Z direction)). In this embodiment, the composite material pattern 228 further includes a flux field region 258. The teardrop region 238 of the composite material pattern 228 is positioned within the flux field region 258.
A plurality of curved segments 260 surround the inner core 222 and are positioned within and outside of the teardrop region 238. Further, a plurality of partial ellipses segments 262 and a plurality of semi-circular segments 263 are positioned within the teardrop region 238. In some embodiments, the plurality of partial ellipses segments 262 and/or the plurality of semi-circular segments 263 are positioned to be centered in the system longitudinal direction (i.e., in the +/−X direction) with respect to the inner core 222. Further, in some embodiments, the further away the plurality of partial ellipses segments 262 and the plurality of semi-circular segments 263 from the inner core the smaller the radius. A plurality of curvilinear segments 264 and a plurality of non-linear segments 266 that form a portion of the composite material pattern 228 are positioned within the flux field region 258 but not within the teardrop region 238. In some embodiments, it should be appreciated that the plurality of curved segments 260, the plurality of partial ellipses segments 262, the plurality of semi-circular segments 263, the plurality of curvilinear segments 264 and/or the plurality of non-linear segments 266 that form a portion of the composite material pattern 228 are curved towards and/or about the axis A1.
A plurality of outer nonlinear segments 268 surround the flux field region 258 such that the plurality of outer nonlinear segments 268 form the outer portion 250 of the emitter device 212 that surround the remaining portion of the inner core 222. In some embodiments, at least a portion of the plurality of outer nonlinear segments 268 are transverse to the composite material pattern 228.
It should be appreciated that the composite material pattern 228 is optimized for heat and/or power transfer between the emitter device 212 and the first receiver device 14 via the composite material pattern 228 while limiting the heat and/or power transfer to the second receiver device 16. The composite material pattern 228 generates the outer core anisotropic material thermal conductivity that is optimized for power transfer from the emitter device 212 to the first receiver device 14. That is, the composite material pattern 228 is an optimized composite material structure of the emitter device 212 to maximize power transfer via heat transfer from the emitter device 212 to the first receiver device 14 while limiting the power transfer to the second receiver device 16. As such, the composite material pattern 228 of the emitter device 212 may be a power transfer system that takes a heat from the emitter device 212 and directs the heat to an area where the heat may be beneficial and/or may not cause harm.
It should also be appreciated that the optimized composite material pattern 228 may be changed or altered to maximize the heat and/or power transfer to the first receiver device 14. In some embodiments, the optimized composite material pattern 228 may change based on the distance between the emitter device 212 and the receiver devices 14, 16. Further, the optimized composite material pattern 228 may change based on the type of material used in the emitter device 212. Further, it should be understood that while the composite material pattern 228 is optimized for heat and/or power transfer, composite material patterns 28, 128, 228 work in conjunction with an optimized emissivity distribution profile, that in some embodiments, is the surface coating and/or paint layer 20a on the outer surface 20, 120, 220 of the emitter device 12, 112, 212 respectively, for heat and/or power transfer, as discussed in greater detail herein.
Referring now to
ƒ0=∫GR1[1−Famb(φ)]dΓR1.
where the ambient view factor, Famb, is evaluated on the outer surface 34a of the first receiver device 14 based on the local angular position, φ, defined by the (x2,y2,z2) coordinate system (not shown) with origin coincident with the axial center of the first receiver device 14. The advantage of the optimization scheme, as described herein, is that it is highly adaptable to more complex scenes involving arbitrary, non-regular geometries with arbitrarily positioned receiver devices 14, 16.
With reference now to
It should be understood that the emitter devices 12, 112, 212 and the composite material patterns 28, 128, 228, the outer surface 20, the alternating materials of the outer core 24, and the like, provide a heat flow control in thermal metamaterials. That is, the emitter devices 12, 112, 212 and the composite material patterns 28, 128, 228, the outer surface 20, the materials of the outer core 24, and the like, directionally control the radiative transfer of heat between multiple bodies in a complex radiative scene. The emitter devices 12, 112, 212 are configured for the manipulation of heat transfer by conduction, where heat generated inside the inner core 22 is transferred by the composite material patterns 28, 128, 228, the alternating materials of the outer core 24, and the like to the outer surface 20.
For the numerical experiments, a steady-state conduction with surface-to-surface radiation heat transfer finite element solver is utilized to model the scene. The governing equation for heat conduction in a solid domain, Ω, is
∇·(k∇T)=−Q in Ω,
where k is the solid body anisotropic thermal conductivity tensor, and Q is the volumetric heat source.
Further, a frequency independent surface-to-surface radiative condition on the boundary, Γ, specified as
qr=ϵ(θ)[G−eb(T)] on Γ.
where radiative heat flux, qr, is a function of an angularly varying surface emissivity, ϵ(θ), the irradiation, G, and the blackbody hemispherical total emissive power, eb(T). The latter expression is governed by Stefan-Boltzmann's law, where eb(T)=n2σT4 with n as the refractive index (taken as unity) and a as the Boltzmann constant.
The surface irradiation is further expressed as G=Gm+Gext+Gamb, where Gm is the mutual irradiation, Gext is the irradiation due to external sources (assumed to be zero), and Gamb=Fambeb(Tamb) is the ambient irradiation. The ambient irradiation is a function of the ambient view factor, 0≤Famb≤1, which addresses the portion of the field of view not covered by other boundaries. Finally, in all prior expressions, T is the temperature state variable. The heat transfer by convection is neglected to isolate and investigate the physical effects of heat transfer by conduction versus radiation.
Now referring to
On either side of the peak view factor B1 (i.e., deviating from the x-axis or 180 degrees), the view factor begins to decrease between ranges of 0.26 to 0.17, illustrated by the bracket B2. Further, on either side of the bracket B2 (i.e., further deviating from the x-axis or 180 degrees) is another decreased range between 0.13 to 0.09, illustrated by the bracket B3. Finally, on either side of the bracket B3 (i.e., furthest deviation from the x-axis or 180 degrees) is another decreased range between 0.09 to 0.01, illustrated by the bracket B4. It should be appreciated that the view factor is the highest on the contours of the emitter device 212 and the receiver devices 14, 16 at the 180 degrees position, or the X axis, and then begins to taper off when there is a deviation from the X-axis. Further, it should be appreciated that the losses from the deviation and/or from the view factor at the peak B1 may be ambient losses.
The emissivity outer surface coating and/or paint layer 20a of the outer surface 20 may be in synchronization with the view factor scene to further enhance directional emission to a selected receiver, such as the first receiver. Through this example, it should be appreciated that the method is shown to be flexible and may be applied to complex multi-body scenes, where multiple modes of heat transfer exist.
Theta (θ), at the zero positon, is aligned with the X axis. Upon rotation of the emitter device 212, at 180 degrees, the emitter device 212 and the composite material pattern 228 is aligned and facing the first receiver device 14. As illustrated, at this position, the optimized emissivity profile 74 of the emitter device 212 is an optimized outer surface coating and/or paint layer distribution that includes an exponential function, which is increased exponentially at the 180 degrees position. That is, the optimization distribution of the optimized emissivity profile 74 of the emitter device 212 follows the exponentially function with a much sharper peak than that of the original painted profile 72. As such, the optimized emissivity profile 74 has a narrower profile to achieve the maximum peak aligned with the view factor compared to the original painted profile 72. For example, when the emitter device 212 is being rotated to the aligned 180 degrees, the optimized emissivity profile 74 has a starting/ending deviation of approximately +/−40 degrees during the rotation theta (θ). The original painted profile 72 has a starting/ending deviation of approximately +/−120 degrees. As such, the ambient losses of the optimized emissivity profile 74 are much less compared to the losses of the original painted profile 72.
As such, the optimized emissivity outer surface coating and/or paint layer profile 74 is focused more on the contours of the view factor creating higher levels that align along the 180 degrees (i.e., the composite material pattern 228 is aligned with the outer surface 34a of the first receiver device 14). That is, as the view factor increases, more power transfer may occur between the emitter device 212 to the first receiver device 14 because there is a greater amount of radiation and power transfer from the emitter device 212 to the first receiver device 14. As such, the optimized emissivity profile 74 (e.g., the optimized outer surface coating and/or paint layer 20a of the outer surface 20 of the emitter device 212 (
Now referring to
The radiative intensity graph 500 includes an origin 501 and an outermost portion 503 along an 180 degree axis. It should be appreciated that in some embodiments, the distance between the origin 501 and the outermost portion 503 is illustrated as the experimental setup of 350 millimeters, as discussed above with respect to
A uniform copper or uniform carbon aerogel emitter device 502, with a uniform emissivity of 0.8, illustrated as a longer dash separated by a short dash, has a uniform radiative intensity that is centered at the origin 501. That is, the uniform copper or uniform carbon aerogel emitter device 502 emits heat and/or power in a uniform or symmetrical 360-degree pattern around the origin 501 such that the emissivity distribution of the surface of the uniform copper or uniform carbon aerogel emitter device 502 is uniform. A pure copper emitter device 504, with the non-optimized directional emissivity coating 72 (
A pure carbon aerogel emitter device 506, with the non-optimized directional emissivity coating 72 (
A second combination emitter device 510, which is the emitter device 112 with the composite material pattern 128 (
A third combination emitter device 516, which is the emitter device 212 with the composite material pattern 228 (
That is, the third combination emitter device 516 with the optimized thermal composite metamaterial design coupled with the composite material pattern 228 (
The radiative intensity of the emitter device 212 may be enhanced with the optimized composite material pattern 228. That is, in some embodiments, it should be appreciated that the third combination emitter device 516 illustrates a maximized power transfer to the first receiver device 14. In some embodiments, the second combination emitter device 510 may be useful when a receiver device is configured to receive power to multiple locations. As such, in this embodiment, the second combination emitter device 510 may provide for an efficient transfer of energy to the multiple locations.
It should be appreciated that the radiative intensity patterns and control thermal energy transfer through the composite material pattern 28, 128, 228 and the outer surface coating and/or paint layer 20a of the outer surface 20 (i.e. the design of both internal material layout and external surface properties) of the emitter devices 12, 112, 212 are customizable to achieve a desired heat and/or power transfer result.
Now referring to
As illustrated by the bar chart 600 in
It should be appreciated that the embodiments described herein relate to a multimode heat transfer system and/or a power transfer system. The system includes an emitter device and a receiver device. The emitter device includes an inner core surrounded by an outer core having a thickness and an outer surface. A composite material pattern extends through at least a portion of the outer surface and at least a portion of the thickness of the outer core and is thermally coupled to the inner core. The composite material pattern directs a heat from the inner core to an object other than the emitter device. The composite material pattern may be a plurality of shapes and sizes and may be optimized to maximize a heat and/or power transfer. Further, the outer core may be a monolithic structure or may be manufactured using a plurality of segments. As described herein, for experimental purposes, the outer core was formed from a plurality of annular rings. The outer core and the composite material pattern are formed from materials that includes a low thermal conductivity material matrix and a high thermal conductivity inlay material. The outer core may be painted or coated based on an optimized emissivity distribution.
The thermal composite metamaterials with co-optimized anisotropic thermal conductivity and external surface emissivity have been demonstrated through numerical experiments. Further, radiative intensity reveals that the optimized configuration provides the greatest control in the directivity of thermal power transfer beyond either standalone design of surface emissivity or material thermal conductivity. As such, the outer core and the composite material pattern with the outer surface coating and/or paint layer may be customizable such that radiative intensity patterns are customizable and control thermal energy transfer for complex multi-body scenes through informed combined engineering of internal composite material layout and external surface properties.
While particular embodiments have been illustrated and described herein, it should be understood that various other changes and modifications may be made without departing from the spirit and scope of the claimed subject matter. Moreover, although various aspects of the claimed subject matter have been described herein, such aspects need not be utilized in combination. It is therefore intended that the appended claims cover all such changes and modifications that are within the scope of the claimed subject matter.
Number | Name | Date | Kind |
---|---|---|---|
9927188 | Liu et al. | Mar 2018 | B2 |
20020167800 | Smalc | Nov 2002 | A1 |
20040233549 | Feygin | Nov 2004 | A1 |
20130340990 | Smolyaninov et al. | Dec 2013 | A1 |
Number | Date | Country |
---|---|---|
108376839 | Aug 2018 | CN |
20180113355 | Oct 2018 | KR |
Entry |
---|
Swanwoo Park, Sunggu Kang, Howon Lee and Wonjoon Choi, “Tunable Multifunctional Thermal Metamaterials: Manipulation of Local Heat Flux Via Assembly of Unit-Cell Thermal Shifters”, Scientific Reports, Jan. 20, 2017, 40 pages, vol. 7, Article No. 41000, https://www.nature.com/articles/srep41000. |
Fei Chen and Dang Yuan Lei, “Experimental Realization of Extreme Heat Flux Concentration with Easy-to-Make Thermal Metamaterials”, Scientific Reports, Jun. 25, 2015, 21 pages, vol. 5, Article No. 11552, https://www.nature.com/articles/srep11552. |
Y.-J. L. Chu, E.M. Jansson, and G. A. Swartzlander, Jr., Phys. Rev. Lett. 121, 063903 (2018). |
E. M. Dede, J. Lee, and T. Nomura, Struct. Multidiscip. O. 49, 59 (2014). |
C. Z. Fan, Y. Gao, and J. P. Huang, Appl. Phys. Lett. 92, 251907 (2008). |
M. Wiener, G. Reichenauer, S. Braxmeier, F. Hemberger, and H.-P. Ebert, Int. J. Thermophys. 30, 1372 (2009). |
S. Hong, S. Shin, and R. Chen, Adv. Funct. Mater., 1909788 (2020). |
Y. Li, X. Bai, T. Yang, H. Luo, and C.-W. Qiu, Nat. Commun. 9, 273 (2018). |
C. Hu, G. Xu, and X. Shen, J. Alloys Compd. 486, 371-375 (2009). |
S. Wijewardane and D. Y. Goswami, Ren. Sust. Energy Rev. 16, 1863-1873 (2012). |
Y. Zhai, Y. Ma, S. N. David, D. Zhao, R. Lou, G. Tan, R. Yang, and X. Yin, Science 355, 1062-1066 (2017). |
A. P. Raman, M. A. Anoma, L. Zhu, E. Rephaeli, and S. Fan, Nature 515, 540-544 (2014). |
K. Ito, T. Watari, K. Nishikawa, H. Yoshimoto, and H. Iizuka, APL Photon. 3, 086101 (2018). |
B. J. Lee, C. J. Fu, and Z. M. Zhang, Appl. Phys. Lett. 87, 071904 (2005). |
M. De Zoysa, T. Asano, K. Mochizuki, A. Oskooi, T. Inoue, and S. Noda, Nat. Photon. 6, 535-539 (2012). |
X. Liu, T. Tyler, T. Starr, A. F. Starr, N. M. Jokerst, and W. J. Padilla, Phys. Rev. Lett. 107, 045901 (2011). |
K. Ikeda, H. T. Miyazaki, T. Kasaya, K. Yamamoto, Y. Inoue, K. Fujimura, T. Kanakugi, M. Okada, K. Hatade, and S. Kitagawa, Appl. Phys. Lett. 92, 021117 (2008). |
J. J. Greffet, R. Carminati, K. Joulain, J. P. Mulet, S. Mainguy, and Y. Chen, Nature 416, 61 (2002). |
D. G. Baranov, Y. Xiao, I. A. Nechepurenko, A. Krasnok, A. Alu, and M. A. Kats, Nat. Mater. 18, 920-930 (2019). |
M. Farhat, P.-Y. Chen, H. Bagci, C. Amra, S. Guenneau, and A. Alu, Sci. Rep., 5, 9876 (2015). |
G. Fujii and Y. Akimoto, Appl. Phys. Lett. 115, 174101 (2019). |
E. M. Dede, Comput. Mater. Sci. 50, 515, (2010). |
Y. Zhang, H. Xu, and B. Zhang, AIP Advances 5, 053402 (2015). |
M. Maldovan, Nature 503, 209 (2013). |
H. Xu, X. Shi, F. Gao, H. Sun, and B. Zhang, Phys. Rev. Lett. 112, 054301 (2014). |
E. M. Dede, T. Nomura, P. Schmalenberg, and J. S. Lee, Appl. Phys. Lett. 103, 063501 (2013). |
T. Han, X. Bai, D. Gao, J. T. L. Thong, B. Li, and C.-W. Qiu, Phys. Rev. Lett. 112, 054302 (2014). |
S. Narayana and Y. Sato, Phys. Rev. Lett. 108, 214303 (2012). |
R. Schillny, M. Kadic, S. Guenneau, and M. Wegener, Phys. Rev. Lett. 110, 195901 (2013). |
S. Guenneau and C. Amra, Opt. Express 21, 6578 (2013). |
T. Han, X. Bai, D. Liu, D. Gao, B. Li, J. T. L. Thong, and C.-W. Qiu, Sci. Rep. 5, 10242 (2015). |
T. Han, T. Yuan, B. Li, and C. W. Qiu, Sci. Rep. 3, 1593 (2013). |
S. Guenneau, C. Amra, and D. Veynante, Opt. Express 20, 8207 (2012). |
J. Y. Li, Y. Gao, and J. P. Huang, J. Appl. Phys. 108, 074504 (2010). |
T. Chen, C.-N. Weng, and J.-S. Chen, Appl. Phys. Lett. 93, 114103 (2008). |
Number | Date | Country | |
---|---|---|---|
20210285735 A1 | Sep 2021 | US |