The following disclosure(s) are submitted under 35 U.S.C. 102(b)(1)(A):
“All-day passive radiative cooling using common salts,” Authorea, Mariana Desiree Reale Batista, Alyssa L. Troksa, Hannah V. Eshelman, Michael Bagge-Hansen, and John D. Roehling. Posted on 10 Mar. 2023, [online 10.22541/au.167845407.79020772/v1].
“All-day passive radiative cooling using common salts,” Material Horizons, Mariana Desireé Reale Batista, Alyssa L. Troksa, Hannah V. Eshelman, Michael Bagge-Hansen, and John D. Roehling. Accepted on 28 Sep. 2023, [online 10.1039/d3mh01139a].
The present invention relates to cooling a surface, and more particularly, this invention relates to infrared transparent aerogel composite for deep sub-ambient cooling of virtually any surface.
Thermal radiative heat loss occurs continuously for any surface facing the sky. Radiation from a surface can escape to space because the atmosphere is transparent to thermal infrared (IR) radiation having wavelengths between 8 and 13 microns (μm), encompassing the peak of thermal radiation at room temperature. In practice, a surface undergoes radiative heat exchange with the sky having a very low apparent temperature. The cold heat-sink of space can therefore be used to absorb heat generated from a surface without additional energy input. This radiative heat exchange is a radiative cooling effect that occurs on every sky-facing surface and may allow cooling to sub-ambient temperatures.
In fact, daily ambient temperature swings between night and day are due to (1) surface cooling via infrared (IR) radiation escaping into the cold of space, and (2) surface heating from solar absorption outpacing IR cooling. Therefore, by avoiding the pathway of heating a radiating surface (e.g., avoiding the absorption of sunlight), it may be possible to achieve sub-ambient cooling during the day. Passive day-time radiative cooling (PDRC) is a viable method that can provide 24 hour, electricity-free cooling.
Sunlight may be reflected from a surface so that the surface may be cooled by redirection (e.g., by reflection) of sunlight and loss of infrared radiation. Two factors have been the focus of surface cooling: (1) high reflectivity for solar light, (2) high IR emission for cooling. However, there is a theoretical gap. Theoretically, considering only IR radiation and sunlight, a surface should be able to be cooled to 60 to 50° C. to below ambient temperature; however, reports demonstrate only a 5 to 10° C. at maximum reduction.
Different studies have achieved daytime cooling through engineering the optical and IR properties. This kind of daytime sub-ambient cooling effect has been demonstrated by numerous materials (i.e., emitters) that are highly effective at reflecting and/or blocking to solar radiation resulting in reduced reducing solar absorption, and also highly emissive in the 8-13 μm band (i.e., nearly maximum loss of heat to space). These radiating surfaces typically reach a few degrees below ambient temperature (<2 to 10)° ° C. Small temperature differences are a typical result because the radiative cooling effect is negated by parasitic heating from the surrounding warmer air (once a surface gets cold, the surface regains heat from the warmer surroundings). Thus, a significant drawback of these studies include parasitic losses from the surrounding air severely limiting the ultimate performance of most engineered surfaces.
Therefore, if parasitic heat gains are minimized, eliminated, etc. much lower temperatures may be possible with increased cooling power. In fact, theoretical work has shown that cooling up to 60° C. below ambient is possible under optimal conditions. In short, if a cooling surface is sufficiently insulated from its surroundings while still allowing IR radiation to escape to space, much more effective radiative cooling can be realized.
One recent demonstration engineered to overcome the heat loss included a vacuum chamber with an IR transparent (ZnSe) window that can reach 43° ° C. below ambient temperature when using a strong IR emitter. However, while this method demonstrated effective cooling, the approach is not scalable to large areas which is an essential aspect for most practical cooling applications, such as air conditioning.
To reduce costs, an inexpensive IR material is needed that can insulate large areas of cooling emitters. Polyethylene (PE) aerogels have been fabricated to this end for improved performance over un-insulated emitters, and while they are effective, PE aerogels will not survive typical outdoor conditions due to sunlight degradation and they are somewhat costly to produce. PE films only last weeks to months in direct sunlight before completely falling apart. Additionally, ultraviolet (UV) light from the sun degrades the plastic drastically reduces IR transmission within a few days, which reduces the ability to allow an underlying surface to cool.
Features and advantages of the disclosed apparatus, systems, and methods will become apparent from the following description. Applicant is providing this description, which includes drawings and examples of specific embodiments, to give a broad representation of the apparatus, systems, and methods. Various changes and modifications within the spirit and scope of the application will become apparent to those skilled in the art from this description and by practice of the apparatus, systems, and methods. The scope of the apparatus, systems, and methods is not intended to be limited to the particular forms disclosed and the application covers all modifications, equivalents, and alternatives falling within the spirit and scope of the apparatus, systems, and methods as defined by the claims.
Applicant's apparatus, systems, and methods accomplishes the requirements of: (1) losing heat to space and (2) preventing heating from sunlight and ambient surroundings by being (a) infrared transparent in the 8-13 μm wavelength range, (b) highly optically reflective to reduce heating from sunlight in the 300 nm-2500 nm range (solar spectrum), and (c) thermally insulating to avoid heating from surrounding air. The various embodiments Applicant's apparatus, systems, and methods provides a material composite that enables sub-ambient radiative cooling of virtually any sky-facing surface, when the disclosure is placed on top in close contact. Applicant's apparatus, systems, and methods work similar to a solar heater vacuum tube, but instead of providing heating, it provides cooling by maintaining a temperature difference between a surface and ambient air. In a preferred embodiment Applicant's apparatus, systems, and methods comprises of an IR transparent aerogel or aerogel, made from an inexpensive IR transparent material, such as common table salt (NaCl, KCI), and an optomechanical frame (multiple designs are possible) that physically protect the delicate IR transparent aerogel, and can serve to concentrate emitted radiation to the most transparent part sky (near vertical) to improve the net cooling power and serve as a mechanical support to the aerogel. NaCl and other water soluble salts have many of the desired properties for this application (high transmittance in 8-13 μm band) but are typically not considered for outdoor use. The insulating aerogel contains a certain size distribution and porosity to add optical reflectance and maintain 3 Other aspects and implementations of the presently described inventive concepts will become apparent from the following detailed description, which, when taken in conjunction with the drawings, illustrate by way of example the principles of the invention. strength, while continuing to provide high thermal resistance for insulating power and high IR transparency in the 8-13 μm band. In the preferred embodiment the water-soluble aerogel/aerogel can be coated with a hydrophobic coating and/or anti-caking agents (i.e., potassium ferrocyanide) to minimize moisture absorption and negative effects from outdoor weather. Additionally, a UV-stabilized, IR transparent plastic film with thin-film water-vapor transmission barriers can be used to encapsulate the whole device to serve as an improved moisture barrier, mitigating the issue of water-solubility and hygroscopicity.
Applicant's apparatus, systems, and methods can be used to cool virtually any surface for such uses as electricity-free air conditioning, remote refrigeration, potable water collection, etc. It could be used to cool buildings or vehicles directly, recycle evaporated process water (cooling towers) and could condense potable water from the air in arid areas and serve for disaster relief when electricity is not available. Coupling it with a heat exchanger and fluid storage, it could be used to supplement and improve the efficiency of HVAC systems, or deep-freezer units by providing a low temperature heat sink for rejecting heat.
The apparatus, systems, and methods are susceptible to modifications and alternative forms. Specific embodiments are shown by way of example. It is to be understood that the apparatus, systems, and methods are not limited to the particular forms disclosed. The apparatus, systems, and methods cover all modifications, equivalents, and alternatives falling within the spirit and scope of the application as defined by the claims.
According to one embodiment, an apparatus for cooling a surface includes a composite that includes a porous infrared (IR) transparent material having at least one substance that is transparent to infrared radiation having a wavelength in a range of 8 to 13 μm. In addition, the composite includes a support frame having an opening for exposing a sky-facing surface of the porous IR transparent material and an encapsulant. The encapsulant is positioned on the sky-facing surface of the porous IR transparent material. The composite is configured to be optically reflective to sunlight and is thermally insulating for reducing heating of a surface from surrounding air.
According to another embodiment, a method of forming an apparatus for cooling a surface includes forming a porous infrared (IR) transparent material having at least one substance that is transparent to infrared radiation having a wavelength in a range of 8 to 13 μm. The method includes coupling the porous IR transparent material to a support frame structure, where the porous IR transparent material is coated with an IR transparent encapsulant.
The accompanying drawings, which are incorporated into and constitute a part of the specification, illustrate specific embodiments of the apparatus, systems, and methods and, together with the general description given above, and the detailed description of the specific embodiments, serves to explain the principles of the apparatus, systems, and methods.
Part (a) of
Part (b) of
The following description is made for the purpose of illustrating the general principles of the present invention and is not meant to limit the inventive concepts claimed herein. Further, particular features described herein can be used in combination with other described features in each of the various possible combinations and permutations.
Unless otherwise specifically defined herein, all terms are to be given their broadest possible interpretation including meanings implied from the specification as well as meanings understood by those skilled in the art and/or as defined in dictionaries, treatises, etc.
It must also be noted that, as used in the specification and the appended claims, the singular forms “a,” “an” and “the” include plural referents unless otherwise specified.
As also used herein, the term “about” denotes an interval of accuracy that ensures the technical effect of the feature in question. In various approaches, the term “about” when combined with a value refers to plus and minus 10% of the reference value. For example, a length of about 100 nm refers to a length of 100 nm+10 nm, a temperature of about 50° ° C. refers to a temperature of 50° C.±5° C., etc.
As further used herein, the term “fluid” may refer to a liquid or a gas.
Further, as used herein, all percentage values are to be understood as percentage by weight (wt. %), unless otherwise noted. Moreover, all percentages by weight are to be understood as disclosed in an amount relative to the bulk weight of an organic plastic scintillator material, in various approaches.
Unless expressly defined otherwise herein, each component listed in a particular approach may be present in an effective amount. An effective amount of a component means that enough of the component is present to result in a discernable change in a target characteristic of the ink, printed structure, and/or final product in which the component is present, and preferably results in a change of the characteristic to within a desired range. One skilled in the art, now armed with the teachings herein, would be able to readily determine an effective amount of a particular component without having to resort to undue experimentation.
The following description includes embodiments of apparatus of an infrared transparent porous material composite for deep sub-ambient cooling of virtually any surface and/or related systems and methods.
In accordance with one general embodiment, an apparatus for cooling a surface includes a composite that includes a porous infrared (IR) transparent material having at least one substance that is transparent to infrared radiation having a wavelength in a range of 8 to 13 μm. In addition, the composite includes a support frame having an opening for exposing a sky-facing surface of the porous IR transparent material and an encapsulant. The encapsulant is positioned on the sky-facing surface of the porous IR transparent material. The composite is configured to be optically reflective to sunlight and is thermally insulating for reducing heating of a surface from surrounding air.
In accordance with another general embodiment, a method of forming an apparatus for cooling a surface includes forming a porous infrared (IR) transparent material having at least one substance that is transparent to infrared radiation having a wavelength in a range of 8 to 13 μm. The method includes coupling the porous IR transparent material to a support frame structure, where the porous IR transparent material is coated with an IR transparent encapsulant.
A list of acronyms used in the description is provided below.
Referring to the drawings, to the following detailed description, and to incorporated materials, detailed information about the apparatus, systems, and methods is provided including the description of specific embodiments. The detailed description serves to explain the principles of the apparatus, systems, and methods. The apparatus, systems, and methods are susceptible to modifications and alternative forms. The application is not limited to the particular forms disclosed. The application covers all modifications, equivalents, and alternatives falling within the spirit and scope of the apparatus, systems, and methods as defined by the claims.
According to various embodiments, an apparatus, a system, and methods have been developed that allow virtually any underlying surface to be cooled to sub-ambient temperatures using materials that are inexpensive, scalable, and robust to sunlight. The essential properties of the apparatus described herein include, 1) materials are highly reflective to solar radiation to reduce heating from sunlight in the 300 nm to 2500 nm range (solar spectrum) (minimizing heat gain during the day), 2) materials are highly thermally insulating to avoid heating from surrounding air (minimizing heat gain, around the clock), and 3) materials are transparent to the 8-13 μm band, allowing radiation to escape to space and effectively cool the surface. These three properties allow the current invention to be placed atop virtually any surface, thereby allowing the surface to cool to sub-ambient temperature.
As illustrated in
Improved cooling has been shown to occur by limiting the radiative exchange with the sky to the most transparent regions (45° to the zenith). This angular selectivity effectively reduces radiative exchange with the warmer parts of the sky (angles toward the horizon) and improves the net cooling power from an emitting surface. This is usually accomplished with geometrically placed reflecting materials that surround the emitting surface, such as a conical reflector, but can be accomplished by other means such as photonic-crystal, where the surface emission does not follow the typical Lambert's cosine law.
According to various embodiments, an apparatus, systems, and methods use solution-processed, freeze-dried aerogels/foams from common salts to produce an insulating material that is optically reflective, thermally insulating, and infrared transparent. The utility of using common salts to produce these materials is three-fold, 1) they are inexpensive materials and the methods described herein make the materials inexpensive to produce, 2) the materials are robust to UV light and long-term exposure to UV does not degrade their performance, and 3) they can be packaged into mechanical frames that can further improve cooling performance through angular selectivity of the frame (i.e. geometrical reflectors built into the frame).
Sodium chloride, potassium chloride, etc. are very highly transparent to the IR, in addition to being stable under UV. If they are sitting out in sunlight, they will not be degraded from sunlight. The reason for that choice is a lot of work with polyethylene (plastic bags) degrades rapidly in sunlight unless it has some sort of UV stabilizer. IR transparent aerogel are typically made from polyethylene and polyethylene is not stable and if ever directly rained on, it would collapse. The liquid tension in the polyethylene aerogel would collapse during exposure to water (e.g., rain). Aerogels are light, fluffy solids that are dried by removing the solvent by conversion from a solid to a gas, from a non-liquid state without surface tension, resulting in a dense network (e.g., super critical CO2 drying). Freeze-drying does the same process. NaCl and KCl may be used as thick window for IR optics, a vacuum chamber with a KCl chamber, etc. NaCl and KCl have not been used in an aerogel.
Referring now to
According to one embodiment, the following description includes steps of an apparatus, systems, and methods. According to one embodiment, fabricating an electricity-free, around-the-clock, deep sub-ambient radiative cooling is described. In one approach, a thermally insulating material, e.g., a salt foam panel, an IR transparent aerogel, foam, etc. is packaged into panels. In a one approach, the thermally insulating material is an aerogel. Aerogels are the optimal size to scatter visible light (solar reflective), but small enough not to scatter infrared radiation (IR transparent). Aerogels are also the most thermally insulating solid currently known. Superhydrophobic coatings are commonly applied to some types of aerogels and can provide stability against moisture and rain. Additional encapsulation with a suitable IR transparent material can provide additional protection against moisture.
As illustrated in
Referring now to
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One of the goals for a practical radiative cooler is to achieve 20 to 25° C. below ambient for a highly emissive surface. Preferably, the cooling apparatus achieves 60 W/m2 at 10° C. below ambient temperature. For example, a radiative cooler may keep at 10′ by 12′ insulated building 10° C. below ambient temperature with 2 to 3 people inside. Preferably, the practical radiative cooler is capable of cooling any surface.
Method 1000 begins with operation 1002 of forming a porous infrared (IR) transparent material that includes at last one substance that is transparent to infrared radiation having a wavelength in a range of 8 to 13 μm. In one approach, the substance may be a common salt. In another approach, the substance may be an element known to be transparent to IR radiation. In yet another approach, the substance may be a compound that is transparent to IR radiation.
According to one embodiment, an IR transparent material is a porous solid having low density, reflective to sunlight, and is thermal insulating for reducing heating of a surface. The IR transparent material is at least 70% to 90% transparent to IR between 8 to 13 μm. In preferred approaches, the IR transparent material has a density in a range of 0.5% to 2.0% of a maximum theoretical density. In one approach, the porous IR transparent material has a porosity in a range of 98% to 99% porosity. In one approach, density is calculated according to the mass of the material divided by the volume of the material. Preferably, the IR transparent material is porous and low density for favorable insulating properties.
According to one approach, an IR transparent material may be an IR transparent foam. According to another approach, an IR transparent material is an IR transparent aerogel. In one approach, the IR transparent material is in the form of an aerogel powder. In another approach, the IR transparent material is in the form of an aerogel monolith.
In various approaches, the substance transparent to IR radiation may include a salt. In one approach, the substance may be a common salt. In one approach, the IR transparent material may be formed with a solution of a salt and a solvent. The solution may be an aqueous solution. The solution may include an organic solvent, e.g., TBA. In various approaches, common salts may include sodium chloride (NaCl), potassium chloride (KCl), sodium bromide (NaBr), potassium bromide (KBr), cesium iodide (CsI), etc.
In some approaches, the substance transparent to IR radiation may include one or more of the following: germanium (Ge), zinc selenide (ZnSe), zinc sulfide (ZnS), barium fluoride (BaF2), etc.
In one approach, a process of forming an IR transparent material may include spraying a solution of salt and solvent to form droplets. The solution may include at least one salt that is transparent to infrared radiation having a wavelength in the range of 8 to 13 μm. One approach of the process of the method is illustrated in part (a) of
The solubility of the salts with water and the phase diagram of the salt mixtures strongly controls the feature sizes of the resulting aerogel/foam when the ice is freezing. In some approaches, smaller structures may be formed during freeze drying salts, so a mixture of salts may be preferable and may behave differently than single salts.
According to one embodiment, the structure of the IR transparent material (e.g., aerogel, foam, etc.) is responsible for the cooling properties of the material. In various approaches, the concentration of the substance may be tuned to result in predefined sizes of finer features of the IR transparent material. For example, lower concentrations of a precursor salt result in finer features of the porous material. The feature sizes provide an IR transparent material favorable optical and IR properties, while the low density and porosity provide the favorable thermal properties.
Moreover, controlling the freezing conditions of the salt solution and the salt composition, the features size of the structure of the IR transparent material (e.g., aerogel, foam, etc.) may be controlled. In some approaches, scattering calculations reveal that features smaller than approximately 500 nm achieve a desired IR transmission for effective PDRC (˜70% transmission over atmospheric IR window).
In some approaches, a porous IR transparent material may be formed with at least one substance that is transparent to IR radiation using methods for forming aerogel, foam, etc. In one approach, a porous IR transparent material may be formed using gelation techniques for forming an aerogel. In another approach, a porous IR transparent material may be formed using a freeze-drying process that uses super critical drying. In another approach, a porous IR transparent material may be formed by plasma spraying.
In exemplary approaches, an IR transparent material may be formed having predefined small fine features for optimal reflection of sunlight, transparency to IR radiation, and optimal insulating properties. A material having features larger than a micron may strongly reflect, e.g., scatter solar light, strongly, as well as scatter IR thereby reducing the transmission of IR radiation. It is generally well understood that finer the features, then the higher the IR transmission increases with a material having finer features. In some approaches, an average diameter of the features of the IR transparent material (e.g., foam, aerogel, etc.) is in a range of greater than 10 nm to about 500 nm. In preferred approaches, an average diameter of the features of the IR transparent material (e.g., foam, aerogel, etc.) is in a range of greater than 20 nm to about 300 nm. In one approach, an insulating material has fine features having a size that scatters optical sunlight and is transparent to IR radiation. In one approach, the IR transparent material is effective at scattering optical light having a wavelength less than one micron. In a preferred approach, the IR transparent material is optically reflective to sunlight.
In some approaches, a concentration of the precursor salt at about 3 M to 6 M forms a material having features with an average diameter in a range of greater than 0.7 μm to greater than 1 μm. Preferably, a concentration of the precursor salt is in a range of 0.01 M up to about 2 M for forming a material with features having an average diameter in a range of less than 100 nm up to 500 nm. In preferred approaches, a mixture of precursor salts forms a material with features having an average diameter in a range of around 50 nm to 200 nm. Preferably, a concentration of the at least one salt is in a range of 0.1 M to about 0.4 M. For a solution having a combination of salts, each salt has a concentration in a range of 0.1 M to about 0.4 M. In one approach, the concentration of each salt is the same in a solution having a combination of salts.
A total salt concentration may affect the overall feature size as well as the material density. The eutectic composition is known to result in finer feature sizes due to eutectic-mode solidification. In the NaCl and H2O solution, hypereutectic concentrations (>5.1 M) resulted in larger feature sizes than hypoeutectic concentrations (<5.1 M). For hypereutectic concentrations, the salt crystals freeze first, and the eutectic structure follows, leaving large proeutectic salt crystals. For hypoeutectic concentrations, H2O crystals form first, followed by the eutectic structure, leaving only the finely formed eutectic salt crystals. Since the H2O is removed upon freeze drying, this leaves a highly porous network from the missing large proeutectic ice crystals making hypoeutectic solutions more favorable for these lower density materials.
A mixture of salts in solution may also result in smaller feature sizes since ternary eutectics can form very fine features (e.g., NaCl+KCl+H2O is a ternary eutectic forming mixture). Similar to the case with NaCl+H2O, the hypoeutectic concentration forced proeutectic H2O crystals to form first, followed by NaCl+KCl in the eutectic ratio.
In some approaches, combining two different precursor salts results in an IR transparent material having finer features. For example, a combination of NaCl+KCl with each having a concentration of 0.3 M, the features of the resulting a material may be finer than a material formed with each precursor salt at the same concentration (0.3 M). In preferred approaches, features are smaller 250 nm. In some approaches, an optimized NaCl+KCl particle may be created by changing the salt concentration within the solution, mixing different salts, and adding a cosolvent such as TBA. The size of fine features of the aerogels, foams, etc. (SEM histograms of the materials) may have a bimodal range, where a plurality of features have an average diameter of about 50 nm and then a plurality of features have an average diameter of about 300 nm. In a preferred approach, a mixture of NaCl and KCl in a particular ratio which forms a ternary eutectic may form the finest structures.
In some approaches, an addition of a cosolvent such as TBA into the salt solution may cause further refinement and even distribution of the features of the material. In some reports, TBA may be included in the solution for freeze-casting to refine microstructures in freeze-cast materials. The eutectic freezing of ice and TBA causes small domains of TBA, and H2O ice to freeze, distributing small liquid domains of liquid H2O (with dissolved salt) around the freezing droplet. This is the aforementioned proeutectic freezing of H2O and drives the concentration of salt up to the eutectic point in the liquid H2O regions. Subsequently, eutectic freezing of H2O/salt and any remaining liquid TBA occurs, leaving the fine structures seen in the image of part (a),
In another approach, the porous material (e.g., salt aerogel, salt foam) having desired fine features, may be sintered to form a monolith structure having particles immobilized within the monolith structure. Approaches for sintering the porous material may include application of heat, exposure to a predefined humidity (e.g., a high moisture content of a humidity chamber).
Moreover, the composite preferably includes a coating to protect the salt-based material from humidity. In some approaches, a coating is included in addition to the encapsulant, such that a coating is added onto the encapsulant. In one example, a coating may be added to the surface of PE film that encapsulates the composite.
NaCl and KCl are both hygroscopic materials that can easily be recrystallized by ambient humidity resulting in macroscopic shrinkage of the material and microscopic coarsening of the crystallites. Structural changes induced by humidity may reduce the ability of the material to insulate and may drastically reduce IR transmission, rendering the IR transparent material ineffective at cooling. Even with encapsulant PE sheets, humidity may easily penetrate the SFP and interact with the IR transparent material since PE has a high water vapor transmission rate. With recent PDRC works demonstrating continued optimal performance of emitter materials in outdoors environments, longevity of IR transparent material (e.g., aerogel, foam, etc.) is desired.
In some approaches, an anti-caking agent may be included in the forming of an IR transparent material to prevent the small features in the salt from growing larger in ambient humidity. Examples of an anti-caking agent include a surfactant, ferrocyanide, CTAB, a common surfactant cation, etc. which may be included with the salt during formation of the material. Being hygroscopic, the salt components such as NaCl and KCl, have a net positive charge that attracts atmospheric water. The relative humidity in the air will absorb the surface of the porous material (e.g., aerogel, foam, etc.). The absorption of water will cause the salt to diffuse along the water at the surface and form crystalline bridges, growing the salt crystals and coarsening features. Preferably, the composite includes a means of protecting the porous IR transparent material from the absorption of water to prevent the formation of undesirable coarsened features that reduces IR transparency of the material. In one approach, a surfactant such as cetyltrimethylammonium bromide (CTAB) may be used as a hydrophobic coating on the porous material to mitigate water uptake and improve lifetime of the porous material.
In one approach, addition of known anti-caking agents might protect the porous material from humidity induced damage. Anti-caking agents include surfactants, surface tension modifies, etc. In one example, sodium ferrocyanide Na4Fe(CN)6 is a well-known anti-caking agent known to stop coarsening of salts from ambient moisture. In one approach, adding the anti-caking component ferrous cyanide (Na4Fe(CN)6) to the salt components may adhere to the surface of salt to prevent movement of the salt on the surface of the porous material, and thereby prevent crystallization of the salt-based porous material. In preferred approaches, the presence of ferrocyanide in the salt-based porous material allows the salt in the material to resist forming crystal structures during exposure to very high humidity. Another preferred approach is to use a process of coating the porous material (e.g., aerogel, foam, etc.) using vacuum evaporation of PDMS. This process coats the aerogel surface and does not allow moisture to attach to the surface. A combination of approaches is also possible to minimize moisture uptake and coarsening.
In one example, an IR transparent composite (e.g., salt foam panel) may be fabricated in part from an aqueous solution containing NaCl, KCl, sodium ferrocyanide (Na4Fe(CN)6) and tert-butyl alcohol (TBA) sprayed directly into a bath of liquid nitrogen to flash-freeze the solution. The frozen droplets may be freeze dried overnight, yielding highly porous powder particles with nanoscale features. The rapid solidification using liquid nitrogen may be necessary to achieve the desired small feature size. The solvent TBA may be included to refine the features of the porous material and the Na4Fe(CN)6 may be added to minimize coarsening from moisture.
According to one approach, the features of a porous material may be optimized by improving the flash freeze process. As described in part (a) of
Looking back to method 1000 of
As described herein, in one approach, the process may fabricate batches of 5 to 10 grams of foam at once (enough material for one or two cooling panels), and the process may be completed within 24 hours. In one approach, the production metho may be scaled to kg quantities of foam. In sharp contrast, supercritical CO2 drying may take up to 3 days for the necessary solvent exchanges and drying processes to complete.
Referring now to
In one approach, part (a) of
According to some approaches, the support frame includes a plurality of sections (e.g., compartments) for containing the IR transparent material. The support frame has an opening for exposing the sky facing surface of the IR transparent material to its surroundings, and preferably the sky so as to maximize radiative transmission of heat. Preferably, the support frame has an opening for exposing the entirety of the sky-facing surface of the IR transparent material.
The support frame provides a confined sections, space, compartments, etc. for particles of the IR transparent material to be immobilized. Without a support frame, material that is composed of particle spheres having an average diameter of 10 to 20 μm would tumble, rock, shift, etc. in response to environmental factors, and this movement results in a compaction of the particles and material. Preferably each compartment 1105 of the support frame 1104 is filled with the material 1102 so that the particles do not move and collapse.
One example of a mechanical support frame may have dimensions of 110 mm w×110 mm/x 10 mm h, with each compartment having dimensions of about 35 mm×35 mm×10 mm. As illustrated in part (a), arrows indicate the mechanical support frame 1104 and the material 1102 are in the same plane, each compartment 1105 of the support frame 1104 is filled with the material 1102. The support frame may function as an optomechanical frame, where the frame holds the material on the surface to be cooled and aligns the material in the direction of the IR radiation from the sky.
The composite includes an encapsulant to protect the IR transparent material (e.g., aerogel, foam, etc.) from humidity of the environment. In one approach, the composite may include a coating for inhibiting water vapor transmission to the IR transparent material. In one approach, the coating may be applied to the encapsulant. As illustrated in part (a), the encapsulant 1016a is positioned on the sky-facing surface of the IR transparent material 1102. The encapsulant 1016a, 1016b may cover the composite. In one approach, the encapsulant may be in the form of a transparent film. In one approach, the composite is encapsulated by a thin sheet of polyethylene (PE). As shown in part (a), in one example, the IR transparent material 1102/mechanical support frame 1014 may be encapsulated with thin polyethylene (PE) sheets 1016a, 1016b to prevent the porous material being blown away by wind currents. The encapsulant may be a commercially available film that is transparent to IR radiation in a range of 8 to 13 μm. The thickness of the encapsulant (measured from the surface of the porous IR transparent material to the outer surface of the encapsulant) may be a thickness that maintains an IR transparency of the encapsulant. For example, a thickness of the encapsulant, e.g., PE sheets, may be about 12.5 μm. In another approach, a portion of an IR transparent material in the shape of a compartment of the support frame is encapsulated with PE film thereby forming packets of the IR transparent material that are placed in each compartment of the support frame to immobilize the encapsulated IR transparent material.
Part (b) of
In a preferred approach, the composite is thermally insulating for reducing heating of a surface from surrounding air. The composite may function as an insulation layer without sacrificing IR transmission or optical reflectance. In some approaches, a thickness of the IR transparent composite (e.g., salt foam panel, aerogel composite, etc.) may contribute to increased solar reflectance. The configuration of the dimensions of the composite includes considerations of adding more material to gain reflectance that may result in reduced IR transmission where the particles are not completely transparent and scatter IR radiation. There are considerations of the interplay between thickness for insulation, optical reflectance, and IR transmission to determine the optical feature size of the IR transparent material (e.g., foam, aerogel, etc.).
As illustrated in part (b), a diagram of one example of an outdoor testing apparatus 1110 including the composite 1101 (e.g., salt foam panel (SFP)). The cooling ability of the SFP was demonstrated by outdoor testing on a hot, clear day. Emitters 1114 were affixed to polished Cu substrates 1116 with thermocouples 1118 attached to the bottom of the substrates 1116. Since the cooling performance of an emitter is greatly affected by non-radiative (conductive and convective) heat gains from the surroundings, the bottom of emitters 1114 were insulated by polystyrene foam 1112.
As illustrated in parts (c) and (d), several emitting surfaces may be tested for comparative thermal performance; (1) white reflective TiO2 paint, (2) 3M Enhanced Specular Reflector (ESR) film, and (3) black paint, etc. As illustrated in part (b), the composite 1101 may be placed on top of black paint 1114a. In part (c), two emitting surfaces include a composite 1101 (SFP) placed on top of black paint (4) and (5) to serve as a worst-case scenario, where any sunlight transmitted through the IR composite would be absorbed and heat the emitter. The two black painted substrates+SFP represent two salt aerogel panels formed with different Na4Fe(CN)6 concentrations. (4) black paint+SFP with higher Na4Fe(CN)6 concentration, and (5) black paint+SFP with higher Na4Fe(CN)6 concentration.
In one example, a testing was performed on 2022 September 8-9 near Livermore, California (peak solar irradiance of 872 W m−2) with the ambient temperature peaking at 42° ° C. (one of the hottest days of the year). A full 24 hour cycle was measured to demonstrate the uninterrupted cooling capabilities of the SFP. Conditions on the testing day included high wind speeds of up to 10 m s−1, which increases parasitic heating, and high downwelling atmospheric radiation with an average of 381 W m−2.
Part (c) depicts an optical image of the emitting surfaces tested for comparative thermal performance. Part (d) depicts an IR thermal image of the emitting surfaces. Sample (4) SFP with the higher Na4Fe(CN)6 concentration demonstrates the lowest thermal energy compared to sample (3) black paint (only) that demonstrates the brightest IR thermal image. Sample (2), the metal-backed 3M ESR film, which has been reported as a sub-ambient cooling film in multiple publications, did not remain sub-ambient in these adverse conditions, and demonstrates a similar IR thermal image to white paint (1). The difference in temperature can be clearly seen in the IR thermal images of the emitters during outdoor test.
Graphs of the cooling performance of the emitters are illustrated in
The SFP (▪) also outperformed highly reflective TiO2 white paint (●, and the state-of-the-art 3M ESR film (□) which has been commercially used for radiative cooling applications. Compared to the 3M ESR film (□), the SFP (▪) demonstrated 2.1° ° C. cooler at solar noon and an average temperature drop below ambient of 5.5° C. throughout the day while the average temperature drop for 3M ESR film (□) was 1.7° C.
According to one embodiment, performance advantages of SFP may be attributed to a reduction of parasitic heating from the environment. Although the presence of the SFP decreases the overall IR transmission from the emitter surface, at low temperatures the insulating properties may outweigh transmission losses. Part (c) of
In one example, part (d) of
NaCl (ACS, 99.0%) was purchased from Alfa Aesar, Thermo Fisher Scientific, and KCl (ACS) was supplied by LabChem. TBA was obtained from Millipore-Sigma. Sodium ferrocyanide decahydrate (Na4Fe(CN)610H2O) was also supplied by Millipore-Sigma.
To prepare the salt aerogels, an aqueous solution of salt was made with 20.83 g of NaCl to 9.19 g KCl, to 1069.80 g of deionized H2O (added 1000 g H2O to ternary eutectic composition). Other additives such as Na4Fe(CN)6 (1 mM, H2O basis) or TBA (18 wt % with respect to H2O) were also added at this point and the solutions were mixed well for several minutes. Next, the solution was pumped through an ultrasonic spray head vibrating at 180 kHz (4.5 W) via a Sono-Tek syringe pump to disperse the solution into 5-50 mm droplets. The droplets were sprayed directly into a bath of liquid nitrogen to rapidly freeze. A feed rate of 8 mL min−1 was used to minimize build-up of salt on the liquid nitrogen surface. The resulting ice was then kept at −196.2° C. (77 K) until it was transferred into a freeze drier and was lyophilized in a Harvest Right Scientific Freeze dryer with a temperature profile set to −23.2° C. (250 K) for 8 hours, −18.2° C. (255 K) for 6 hours, −9.2° C. (264 K) for 4 hours and −1.2° ° C. (272 K) for 2 hours and lastly to room temperature until the sample was removed. This profile ensured that the ice was removed while frozen, avoiding any local melting of the salt. Every freeze-dried batch consisted of several containers full of frozen droplets, 25 mL of solution per container was used to ensure that the layer of frozen droplets was thin enough to completely dry in the 20-hour lyophilization cycle.
The SFPs fabricated consisted of 3D printed frames of 3×3 squares (each square was 35 mm×35 mm×10 mm) printed with acrylonitrile butadiene styrene (ABS) and painted with barium sulfate (BaSO4) to minimize solar absorption. The frame was filled with salt aerogel powder (0.350 g per square, 1.4% relative density) and encapsulated in a thin clear PE sheet (food wrap, 12.5 mm thick) to prevent wind blowing the aerogel away. The PE sheets were sealed with a heat sealer to make the devices were air-tight. The SFPs were fabricated in a N2-filled glove box to minimize any initial moisture exposure.
The emitters were mounted in 75 mm polystyrene aerogel covered with aluminum coated mylar to minimize solar absorption (part (b),
Parasitic heat transfer coefficients were calculated using a National Instruments 9210 Temperature input module with type-K thermocouples (to monitor temperature) and a USB controlled power supply with a proportional-integral-derivative (PID) controller implemented in LabView to control heater power. 10 cm×10 cm silicone encapsulated surface heaters were attached to the bottom of aluminum heat spreader substrates. 3M ESR emitters were affixed to the top of the Al heat spreaders. The test was conducted at night with minimal wind (<0.5 m s−1) using identical 3M SR films and identical SFPs.
The aerogel microstructure was investigated by SEM in an Apreo S Lo Vac at an accelerating voltage of 2 kV. Fourier Transform Infrared (FTIR) spectroscopy was performed in a Bruker's VERTEX 70 spectrometer equipped with a PIKE Technologies mid-IR integrating sphere. UV-Vis-NIR reflectance/transmittance was measured with a PerkinElmer Lambda 950 with an integrating sphere. Thermal conductivity of an encapsulated support frame without aerogel, and a SFP packaged with aerogel at varying relative density was measured in a Hot Disk TPS 3500 Thermal Constants Analyzer (ThermTest Inc). TEM images were collected in a Thermo Fisher Scientific Titan equipped with a SuperX x-ray energy dispersive spectrometer. Particle sizes histograms from SEM images were analyzed by manual measurements in ImageJ.
Miniature SFPs (1.5% density) were placed in a Memmert AtmoCONTROL climate chamber. Two SFPs (coated and uncoated aerogel samples) were held in succession at 55%, 65%, and 75% RH for 30 minutes each and photographed after each exposure. SEM imaging was performed before and after the final moisture exposure.
To test how density affects thermal conductivity, miniature SFPs at two different densities were measured using the hot-disk method. As shown in Table 1, the thermal conductivity exhibited a minimum value of 0.037 W m−1 K−1 at 1.5% relative density. This conductivity value is similar to other commonly used insulating materials, such as cotton and fiberglass. The measurements suggest that increasing density further may increase the thermal conductivity. Therefore, SFPs packed at low density between 1.4-1.5% relative density (0.03 g cm−3) minimizes the thermal conductivity, maximizes the IR transmission, and fills any voids after packing the SFP (1% was the lowest self-supporting density possible, but typically results in unfilled regions).
aEmpty support frame (air)
aSFP at 1.5% relative density
aSFP at 2.5% relative density
bCotton
bFiberglass insulation
aError values shown are the standard deviation in the hot-disk measurement value.
bRange of values
Part (a) of
Part (b) shows a histogram of feature sizes measured via SEM from different aerogels. The insets depict SEM images of each aerogel having a scale bar of 500 nm: NaCl+KCl (top)(solid line), 0.3 M KCl (middle)(∘), and 0.3 M NaCl (bottom) (●). The distribution of feature sizes in each aerogel, with a bimodal distribution, may be centered around 50 and 300 nm. The inset SEM images illustrate the features of the particles from the aerogels made from only hypoeutectic NaCl solutions (●) bottom inset, or hypoeutectic KCl solutions (∘) middle inset. These aerogels did not result in sufficiently small features (e.g., 500 and 300 nm average features, respectively) whereas the mixed salt formed much finer features (solid line, top inset). The molar ratio of salt to water was around 1%, resulting in approximately 1% dense aerogel particles as the final density of the loose powder with no packing was approximately 0.02 g cm−3.
Parts (c) and (d) depict images of transmission electron microscope (TEM) energy dispersive spectroscopy (EDS) map of a crushed NaCl+KCl particle (made with TBA and 1 mM Na4Fe(CN)6). The images reveal the mixture of NaCl and KCl resulted in small crystallites of each component. Chemical mapping showed larger NaCl features measuring approximately 400 nm and mixture of small KCl features <100 nm. This is consistent with proeutectic H2O crystals forming first, followed by ternary eutectic formation.
To quantify the reduction in the parasitic heating rate, the parasitic heat transfer coefficients were measured with and without the SFP. In this method, the cooling power at ambient temperature and the maximum temperature drop are measured simultaneously with two identical devices. The uncovered 3M ESR surface was found to have a parasitic heat transfer coefficient of h=8.1 Wm−2 K−1. Covering the 3M ESR film with the SFP reduced the parasitic heat transfer rate by more than 50%, to h=3.6 W m−2 K−1.
An aerogel with large average feature sizes (B1 mm) may scatter optical light (i.e., sunlight), and may also scatter IR light (due to Mie scattering) leading to low IR transmission. An optimized salt aerogel with its small feature sizes (B100 nm) may be able to scatter optical light while minimizing IR scattering. In one example, reflectance and transmission of the salt aerogels were measured by packing the aerogel into a holder at 2.0% relative density to ensure no gaps. The hemispherical transmittance and reflectance of the aerogels are shown in part (a) of
Additionally, the IR transmission of the NaCl and KCl do not possess any absorption peaks within the atmospheric transmission window. The peak near 3 mm corresponds to the —OH absorption of water that is present on the surface of the NaCl and KCl. As the measurements were done in ambient air, moisture was present on the surface of the salt.
Part (b) of
In one approach, Na4Fe(CN)6 may be included in salt aerogels to mitigate coarsening. A desired concentration of Na4Fe(CN)6 may be added to the salt solution before spray freezing. In one example, aerogel samples were prepared as uncoated SFP samples and “Na4Fe(CN)6-coated” SFP samples and placed in a humidity chamber for 30 minutes, removed, photographed, then exposed to the next humidity step.
Addition of 1 mM Na4Fe(CN)6 to the SFP aerogel samples reduced the propensity of the coated aerogels to coarsen from exposure to moisture at RH as high as 75% compared to no humidity (lower row,
Therefore, it will be appreciated that the scope of the present application fully encompasses other embodiments which may become obvious to those skilled in the art. In the claims, reference to an element in the singular is not intended to mean “one and only one” unless explicitly so stated, but rather “one or more.” All structural and functional equivalents to the elements of the above-described preferred embodiment that are known to those of ordinary skill in the art are expressly incorporated herein by reference and are intended to be encompassed by the present claims. Moreover, it is not necessary for a device to address each and every problem sought to be solved by the present apparatus, systems, and methods, for it to be encompassed by the present claims. Furthermore, no element or component in the present disclosure is intended to be dedicated to the public regardless of whether the element or component is explicitly recited in the claims. No claim element herein is to be construed under the provisions of 35 U.S.C. 112, sixth paragraph, unless the element is expressly recited using the phrase “means for.”
While the apparatus, systems, and methods may be susceptible to various modifications and alternative forms, specific embodiments have been shown by way of example in the drawings and have been described in detail herein. However, it should be understood that the application is not intended to be limited to the particular forms disclosed. Rather, the application is to cover all modifications, equivalents, and alternatives falling within the spirit and scope of the application as defined by the following appended claims.
Moreover, any of the structures and/or steps may be implemented using known materials and/or techniques, as would become apparent to one skilled in the art upon reading the present specification.
Various embodiments may be used to cool virtually any surface for such uses as electricity-free air conditioning, remote refrigeration, potable water collection, etc. One embodiment may be used to cool buildings or vehicles directly, recycle evaporated process water (cooling towers) and could condense potable water from the air in arid areas and serve for disaster relief when electricity is not available. In one approach, coupling the apparatus with a heat exchanger and fluid storage may be useful to supplement and improve the efficiency of HVAC systems, deep-freezer units, etc. by providing a low temperature heat sink for rejecting heat.
The inventive concepts disclosed herein have been presented by way of example to illustrate the myriad features thereof in a plurality of illustrative scenarios, aspects, and/or implementations. It should be appreciated that the concepts generally disclosed are to be considered as modular, and may be implemented in any combination, permutation, or synthesis thereof. In addition, any modification, alteration, or equivalent of the presently disclosed features, functions, and concepts that would be appreciated by a person having ordinary skill in the art upon reading the instant descriptions should also be considered within the scope of this disclosure.
While various aspects have been described above, it should be understood that they have been presented by way of example only, and not limitation. Thus, the breadth and scope of an aspect of the present invention should not be limited by any of the above-described exemplary aspects but should be defined only in accordance with the following claims and their equivalents.
This application is a Continuation in Part of U.S. patent application Ser. No. 17/935,396, filed on Sep. 26, 2022, which claims priority to U.S. Provisional Patent Application No. 63/261,788 filed Sep. 29, 2021, each of which are herein incorporated by reference.
This invention was made with Government support under Contract No. DE-AC52-07NA27344 awarded by the United States Department of Energy. The Government has certain rights in the invention.
Number | Date | Country | |
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63261788 | Sep 2021 | US |
Number | Date | Country | |
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Parent | 17935396 | Sep 2022 | US |
Child | 18600120 | US |