Selective surface: Difference between revisions
m ce, mainly punctuation |
→Selective materials: added more detailed information about the types of selective surfaces. |
||
| Line 7: | Line 7: | ||
* Thermal infrared radiation, from materials with temperatures approximately in the interval -40 to 100 °C, covers approximately the wavelengths 4000 nm to 40,000 nm = 4 um to 40 um; The thermal infrared radiation interval being named or covered by: [[Mid-infrared|MIR]], [[LWIR]] or [[IR-C]]. |
* Thermal infrared radiation, from materials with temperatures approximately in the interval -40 to 100 °C, covers approximately the wavelengths 4000 nm to 40,000 nm = 4 um to 40 um; The thermal infrared radiation interval being named or covered by: [[Mid-infrared|MIR]], [[LWIR]] or [[IR-C]]. |
||
== Selective |
== Selective Surface Designs == |
||
Normally, a combination of materials is used. One of the first selective surfaces investigated was a semiconductor-metal tandem<ref name=":0">{{Cite web|url=https://www.nrel.gov/docs/fy02osti/31267.pdf|title=Review of Mid- to High-Temperature Solar Selective Absorber Materials|last=Kennedy|first=Cheryl|date=2002|website=NREL|access-date=2018}}</ref> - simply [[copper]] with a layer of black [[cupric oxide]]. Silicon on metal is also another example.<ref name=":0" /> A different design has ceramic-metal composites (cermets) on metal substrates.<ref name=":0" /><ref>{{Cite journal|last=Tesfamichael|first=Tuquabo|last2=Wäckelgård|first2=Ewa|date=1999-07-01|title=Angular solar absorptance of absorbers used in solar thermal collectors|url=https://www.osapublishing.org/abstract.cfm?uri=ao-38-19-4189|journal=Applied Optics|language=EN|volume=38|issue=19|pages=4189–4197|doi=10.1364/AO.38.004189|issn=2155-3165}}</ref> For example, [[Black]] [[chromium]] ("black chrome") and [[nickel]]-plated anodized aluminum is another selective surface that is very durable, highly resistant to [[humidity]] or [[oxidizing]] atmospheres and extreme [[temperature]]s while being able to retain its selective properties, but expensive. One of the more popular designs - a multi-layer broadband solar absorber - consists of a metal substrate coated with multiple layers of metal and dielectric materials. While those have to be vacuum-deposited, they have been widely adopted due to their suitability for vacuum tubes.<ref>{{Cite web|url=http://www.almecogroup.com/en/pagina/53-tinox-energy-cu|title=TiNOX energy|last=|first=|date=2018|website=Alemco|access-date=2018}}</ref><ref name=":0" /> Recently, plasmonic nanoparticle-coated metal sheets made by a simple dip-and-dry method have been proposed as selective surfaces,<ref>{{Cite journal|last=Mandal|first=Jyotirmoy|last2=Wang|first2=Derek|last3=Overvig|first3=Adam C.|last4=Shi|first4=Norman N.|last5=Paley|first5=Daniel|last6=Zangiabadi|first6=Amirali|last7=Cheng|first7=Qian|last8=Barmak|first8=Katayun|last9=Yu|first9=Nanfang|date=2017-11-01|title=Scalable, “Dip-and-Dry” Fabrication of a Wide-Angle Plasmonic Selective Absorber for High-Efficiency Solar–Thermal Energy Conversion|url=http://onlinelibrary.wiley.com/doi/10.1002/adma.201702156/abstract|journal=Advanced Materials|language=en|volume=29|issue=41|pages=n/a–n/a|doi=10.1002/adma.201702156|issn=1521-4095}}</ref> but they are yet to be commercially used. |
|||
Normally, a combination of materials is used. One of the first selective surfaces investigated was simply [[copper]] with a layer of black [[cupric oxide]]. [[Black]] [[chromium]] ("black chrome") [[nickel]]-plated [[copper]] is another selective surface that is very durable, highly resistant to [[humidity]] or [[oxidizing]] atmospheres and extreme [[temperature]]s while being able to retain its selective properties, but expensive. Another combination consists of [[steel]] plated with [[gold]], [[silicon]], and [[silicon dioxide]]. |
|||
Although ordinary black paint has high solar absorption, it also has high thermal emissivity, and thus it is not a selective surface. |
Although ordinary black paint has high solar absorption, it also has high thermal emissivity, and thus it is not a selective surface. |
||
Revision as of 00:05, 21 February 2018
 |
In solar thermal collectors, a selective surface or selective absorber is a means of increasing its operation temperature and/or efficiency. The selectivity is defined as the ratio of solar radiation absorption (αsol) to thermal infrared radiation emission (εtherm).
Selective surfaces take advantage of the differing wavelengths of incident solar radiation and the emissive radiation from the absorbing surface:
- Solar radiation covers approximately the wavelengths 350 nm to 4000 nm; UV-A, visible and near infrared (NIR, or IR-A plus IR-B).
- Thermal infrared radiation, from materials with temperatures approximately in the interval -40 to 100 °C, covers approximately the wavelengths 4000 nm to 40,000 nm = 4 um to 40 um; The thermal infrared radiation interval being named or covered by: MIR, LWIR or IR-C.
Selective Surface Designs
Normally, a combination of materials is used. One of the first selective surfaces investigated was a semiconductor-metal tandem[1] - simply copper with a layer of black cupric oxide. Silicon on metal is also another example.[1] A different design has ceramic-metal composites (cermets) on metal substrates.[1][2] For example, Black chromium ("black chrome") and nickel-plated anodized aluminum is another selective surface that is very durable, highly resistant to humidity or oxidizing atmospheres and extreme temperatures while being able to retain its selective properties, but expensive. One of the more popular designs - a multi-layer broadband solar absorber - consists of a metal substrate coated with multiple layers of metal and dielectric materials. While those have to be vacuum-deposited, they have been widely adopted due to their suitability for vacuum tubes.[3][1] Recently, plasmonic nanoparticle-coated metal sheets made by a simple dip-and-dry method have been proposed as selective surfaces,[4] but they are yet to be commercially used.
Although ordinary black paint has high solar absorption, it also has high thermal emissivity, and thus it is not a selective surface.
Typical values for a selective surface might be 0.90 solar absorption and 0.10 thermal emissivity, but can range from 0.8/0.3 for paints on metal to 0.96/0.05 for commercial surfaces. Thermal emissivities as low as 0.02 have been obtained in laboratories.
Other selective surfaces
There exists other selective surfaces that are not normally used on solar thermal collector surfaces, such as low emissivity surfaces used in window glasses, which reflect thermal radiation and have high transmittance factors (being transparent) for visible sunlight.
See also
External links
- Selective Surface for efficient Solar Thermal Conversion
- Table of absorption and emissivity for various materials
- ^ a b c d Kennedy, Cheryl (2002). "Review of Mid- to High-Temperature Solar Selective Absorber Materials" (PDF). NREL. Retrieved 2018.
{{cite web}}: Check date values in:|access-date=(help) - ^ Tesfamichael, Tuquabo; Wäckelgård, Ewa (1999-07-01). "Angular solar absorptance of absorbers used in solar thermal collectors". Applied Optics. 38 (19): 4189–4197. doi:10.1364/AO.38.004189. ISSN 2155-3165.
- ^ "TiNOX energy". Alemco. 2018. Retrieved 2018.
{{cite web}}: Check date values in:|access-date=(help) - ^ Mandal, Jyotirmoy; Wang, Derek; Overvig, Adam C.; Shi, Norman N.; Paley, Daniel; Zangiabadi, Amirali; Cheng, Qian; Barmak, Katayun; Yu, Nanfang (2017-11-01). "Scalable, "Dip-and-Dry" Fabrication of a Wide-Angle Plasmonic Selective Absorber for High-Efficiency Solar–Thermal Energy Conversion". Advanced Materials. 29 (41): n/a–n/a. doi:10.1002/adma.201702156. ISSN 1521-4095.