Film growing method
US-2015368779-A1 · Dec 24, 2015 · US
US9267207B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9267207-B2 |
| Application number | US-201013499384-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 14, 2010 |
| Priority date | Sep 30, 2009 |
| Publication date | Feb 23, 2016 |
| Grant date | Feb 23, 2016 |
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A central tube for linear concentrating solar thermal power plants, has an absorber layer. The absorber layer is generated by cold gas sputtering, wherein suitable method parameters can in particular generate an increased surface roughness by means of pores in the surface region of the absorber layer. An absorber layer can thus be advantageously produced, having a quadratic roughness of no more than 1 μm, measured in a close range of no more than 50 μm diameter, and preferably being made of a corrosion-proof hard alloy comprising tungsten carbide, in particular WC—CoCr, WC—Co, WC—FeCo, WC—FeC, WC—FeNi, WC—Ni or WC—NiCr.
Opening claim text (preview).
The invention claimed is: 1. A method comprising: providing a solar-thermal-power-plant-linear-concentrating central tube; and depositing a corrosion-resistant tungsten-carbide-based cemented carbide by cold gas spraying to thereby apply an absorber layer onto the central tube, the absorber layer applied to have a surface with a roughness, a surface profile of which can be described by a two-dimensional Fourier spectrum of a location-dependent height position H of the surface, and the two-dimensional Fourier spectrum defined such that within spatial frequencies which correspond to spatial periods of greater than 6 μm and less than 50 μm, the amplitudes are not greater than a maximum amplitude within spatial frequencies which correspond to spatial periods of less than 6 μm. 2. The method as claimed in claim 1 , wherein the cemented carbide is selected from the group consisting of WC—CoCr, WC—Co, WC—FeCo, WC—FeC, WC—FeNi, WC—Ni and WC—NiCr. 3. The method as claimed in claim 1 , wherein the absorber layer is produced to have a surface with a root-mean-squared roughness of at most 1 μm, measured in a near range of at most 50 μm in diameter. 4. The method as claimed in claim 1 , wherein the absorber layer is applied as a gradient layer, which has properties that change across a surface thereof. 5. The method as claimed in claim 1 , wherein the absorber layer is layered on to form a multi-ply layer. 6. The method as claimed in claim 1 , wherein the absorber layer is layered on to form a multi-ply layer having a plurality of plies, and at least one ply of the multi-ply layer is a gradient ply having properties that change across a surface thereof. 7. The method as claimed in claim 1 , wherein the central tube serves as a substrate for the absorber layer, the absorber layer has a base region near the substrate and a surface region, and the base region is formed by controlling method parameters such that a substantially pore-free layer construction results. 8. The method as claimed in claim 1 , wherein the cemented carbide is deposited by coating particles, and the method further comprises varying method parameters and/or a particle concentration in a circumferential direction and/or in a longitudinal direction of the central tube such that the properties of the absorber layer change across a surface thereof. 9. A device to linearly concentrate solar thermal energy, comprising: a central tube; and an absorber layer formed on the central tube, the absorber layer being formed of a corrosion-resistant tungsten-carbide-based cemented carbide and having a roughness of 0.5 to 6 μm, the absorber layer having a surface with a roughness, a surface profile of which can be described by a two-dimensional Fourier spectrum of a location-dependent height position H of the surface, and the two-dimensional Fourier spectrum defined such that within spatial frequencies which correspond to spatial periods of greater than 6 μm and less than 50 μm, the amplitudes are not greater than a maximum amplitude within spatial frequencies which correspond to spatial periods of less than 6 μm. 10. The device as claimed in claim 9 , wherein the absorber layer is formed of at least one material selected from the group consisting of WC—CoCr, WC—Co, WC—FeCo, WC—FeC, WC—FeNi, WC—Ni and WC—NiCr. 11. The device as claimed in claim 9 , wherein the absorber layer has a surface with a root-mean-squared roughness of at most 1 μm, measured in a near range of at most 50 μm in diameter. 12. The device as claimed in claim 9 , wherein the device has a solar absorptivity α>0.85 and a thermal emissivity ε<0.15 at temperatures of at least 400° C. 13. The device as claimed in claim 9 , wherein the absorber layer is formed from a material and/or with a structural design that changes in a circumferential direction and/or in a longitudinal direction of the central tube. 14. The device as claimed in claim 13 , wherein the absorber layer has different absorption and emission characteristics across a circumferential direction and/or across a longitudinal direction of the central tube.
Solar heat collectors for receiving concentrated solar energy, e.g. receivers for solar power plants · CPC title
Impact or kinetic deposition of particles · CPC title
Preventing corrosion; Protecting against dirt or contamination · CPC title
Cross-Sectional Technologies · mapped topic
Mechanical Engineering · mapped topic
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