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dc.contributor.authorDidato, N.
dc.contributor.authorAngel, R.
dc.contributor.authorRademacher, M.
dc.date.accessioned2024-03-22T01:47:32Z
dc.date.available2024-03-22T01:47:32Z
dc.date.issued2023-10-04
dc.identifier.citationN. Didato, R. Angel, M. Rademacher, "Shape-adjustable heliostats: designs for individuals and fields for > 3000 concentration," Proc. SPIE 12671, Advances in Solar Energy: Heliostat Systems Design, Implementation, and Operation, 126710D (4 October 2023); https://doi.org/10.1117/12.2681483
dc.identifier.isbn978-151066556-9
dc.identifier.issn0277-786X
dc.identifier.doi10.1117/12.2681483
dc.identifier.urihttp://hdl.handle.net/10150/671517
dc.description.abstractShape-adjustable heliostats can maintain a focused image of the solar disc on a receiver target throughout the day, as the angle of incidence (AOI) changes on the reflector. This requires the heliostat reflector to be deformed into a unique biconic concave shape dependent on AOI. The reflector comprises a single rectangular sheet of silvered float glass mounted to a steel frame. Its shape is set initially, by adjusting the height of mounting points, to the biconic shape required for imaging at 60 degrees AOI. Shapes for other AOIs are obtained by twisting the frame from its four corners and center. A finite element model was made of a heliostat designed to form a disc image on a 130 m distant receiver using a single sheet glass reflector, 1/8” thick x 130” x 96”, supported by 58 points on a rectangular tube frame structure weighing 120 kg. Analysis shows an overall RMS slope error <1 mrad for all AOI from 0 to 70 degrees. Without twisting, the RMS slope error would be ~3.5 mrad at 0° and 70° AOI. Preliminary results from analysis of slope error maps generated from the FE model indicate encircled energies within the ideal solar disc radius of >85% are achievable. Models of fields of closely packed heliostats of this type, on target axis mounts, demonstrate a geometrical throughput into the receiver of >73% of the total mirror area, after accounting for blocking, shadowing, and cosine loss. In one model, with 450 heliostats powering five compound parabolic concentrators at a receiver, a concentration of > 3,000 was obtained at powers > 1 MW, through much of the day. © 2023 SPIE.
dc.language.isoen
dc.publisherSPIE
dc.rights© 2023 SPIE.
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/
dc.subjectAdjustable
dc.subjectAngle of incidence
dc.subjectEncircled energy
dc.subjectFocus
dc.subjectHeliostat
dc.subjectSlope error
dc.subjectTwisting
dc.titleShape-adjustable heliostats – designs for individuals and fields for > 3000 concentration
dc.typeProceedings
dc.typetext
dc.contributor.departmentDepartment of Astronomy, Steward Observatory, University of Arizona
dc.identifier.journalProceedings of SPIE - The International Society for Optical Engineering
dc.description.noteImmediate access
dc.description.collectioninformationThis item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.
dc.eprint.versionFinal Published Version
dc.source.journaltitleProceedings of SPIE - The International Society for Optical Engineering
refterms.dateFOA2024-03-22T01:47:32Z


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