Systems and Methods of Using Phase Change Material in Power Plants
US-2015204612-A1 · Jul 23, 2015 · US
US11041680B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11041680-B2 |
| Application number | US-201716306693-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jun 2, 2017 |
| Priority date | Jun 3, 2016 |
| Publication date | Jun 22, 2021 |
| Grant date | Jun 22, 2021 |
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Latent heat storage devices are disclosed, such as latent heat storage devices comprising a phase change material encapsulated in sufficiently conductive tubes, wherein the tubes are arrayed in a hexagonal-packed pattern. The devices herein can be used, for example, in residential and/or commercial HVAC systems.
Opening claim text (preview).
What is claimed is: 1. A latent heat storage device comprising: a containment tank; a plurality of cylindrical encapsulation tubes having a hollow interior, wherein the cylindrical encapsulation tubes are arrayed in a hexagonal-packed pattern, are comprised of a sufficiently conductive material, and are contained within the containment tank; a phase change material, contained within the hollow interior of the cylindrical encapsulation tubes; and a means for connecting the containment tank in fluid communication with a first source of heat transfer fluid to allow a heat transfer fluid to flow through a heat transfer fluid space to exchange heat with the phase change material; wherein the latent heat storage device has a first resistance ratio of less than about 0.1, wherein the first resistance ratio is defined by the equation: R t R c = π 3 72 ( 2 3 - π ) ( r o + r i ) / 2 ( r o - r i ) Nu k f k t wherein: R t is the resistance of conduction around the encapsulation tube [° K/W]; R c is the resistance of convection between the heat transfer fluid (HTF) and the encapsulation tube [° K/W]; r o is the outside radius of the encapsulation tube [m]; r i is the inside radius of the encapsulation tubing [m]; k f is the conductivity of the heat transfer fluid [W/(m·° K)]; k t is the conductivity of the encapsulation tube material [W/(m·° K)]; and Nu is the Nusselt number. 2. The device of claim 1 , wherein the sufficiently conductive tubes are comprised of a metal. 3. The device of claim 2 , wherein the sufficiently conductive tubes are comprised of copper. 4. The device of claim 2 , wherein the sufficiently conductive tubes are comprised of aluminum. 5. The device of claim 1 , wherein the phase change material is selected from water (ice), a salt hydrate, a fatty acids, or a paraffin hydrocarbon. 6. The device of claim 5 , wherein the phase change material is a paraffin hydrocarbon. 7. The device of claim 6 , wherein the phase change material comprises tetradecane. 8. The device of claim 7 , wherein the phase change material comprises at least 99% tetradecane. 9. The device of claim 1 , wherein the phase change material has a phase change temperature in a range between 5° C. and 12° C. 10. The device of claim 1 , wherein the heat transfer fluid comprises an aqueous solution of ethylene glycol, propylene glycol, glycerol, or combinations thereof. 11. The device of claim 10 , wherein the heat transfer fluid comprises an aqueous solution containing about 35% by volume propylene glycol. 12. The device of claim 1 , wherein the latent heat storage device has a resistance ratio of less than about 0.05. 13. A latent heat storage device comprising: a containment tank; a plurality of cylindrical encapsulation tubes having a hollow interior, wherein the cylindrical encapsulation tubes are arrayed in a hexagonal-packed pattern, are comprised of a sufficiently conductive material, and are contained within the containment tank; a phase change material, contained within the hollow interior of the cylindrical encapsulation tubes; and a means for connecting the containment tank in fluid communication with a first source of heat transfer fluid to allow a heat transfer fluid to flow through a heat transfer fluid space to exchange heat with the phase change material; wherein the latent heat storage device has a resistance ratio of less than about 0.1, wherein the resistance ratio is defined by the equation: R t R p = π 2 18 ( r o + r i ) / 2 ( r 0 - r i ) k p k t wherein: R t is the resistance of conduction around the encapsulation tube [° K/W]; R p is the resistance of conduction between the PCM and the encapsulation
with assemblies of stacked elements · CPC title
the heat storage material being enclosed in loose or stacked elements · CPC title
Thermal energy storage · CPC title
using latent heat · CPC title
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