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contributor authorSchenk, Heiko
contributor authorHirsch, Tobias
contributor authorFabian Feldhoff, Jan
contributor authorWittmann, Michael
date accessioned2017-05-09T01:12:33Z
date available2017-05-09T01:12:33Z
date issued2014
identifier issn0199-6231
identifier othersol_136_04_041015.pdf
identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/156322
description abstractIn recent years, linear Fresnel (LF) collector systems have been developed as a technical alternative to parabolic trough (PT) collector systems. While in the past, LF systems focused on lowand mediumtemperature applications, today, LF systems are equipped with vacuum receivers and, therefore, can be operated with similar operating parameters as PT systems. Papers about the technical and economical comparison of specific PT and LF systems have already been published (Dersch et al., 2009, "Comparison of Linear Fresnel and Parabolic Trough Collecor Systems—System Analysis to Determine BreakEven Costs of Linear Fresnel Collectors," Proceedings of the 15th International SolarPACES Symposium, Berlin; Giostri et al. 2011, "Comparison of Two Linear Collectors in Solar Thermal Plants: Parabolic Trough vs. Fresnel," ASME 2011 5th International Conference on Energy Sustainability, Washington, DC; and Morin et al., 2012, "Comparison of Linear Fresnel and Parabolic Trough Collector Power Plants," Sol. Energy, 86(1), pp. 1–12). However, the present paper focuses on the systematic differences in optical and thermodynamic performance and the impact on the economic figures. In a first step the optical performance of typical PT and LF solar fields (SFs) has been examined, showing the differences during the course of the day and annually. Furthermore, the thermodynamic performance, depending on the operating temperature, has been compared. In a second step, the annual electricity yield of typical PT and LF plants has been examined. Solar Salt has been chosen as the heat transfer fluid. Both systems utilize the same power block (PB) and storage type. Solar field size, storage capacity, and PB electrical power are variable, while all examined configurations achieve the same annual electricity yield. As expected for molten salt systems, both systems are the most costeffective with large storage capacities. The lower thermodynamic performance of the LF system requires a larger SF and lower specific SF costs in order to be competitive. Assuming specific PT field costs of 300 €/m2 aperture, the breakeven costs of the LF system with Solar Salt range between 202 and 235 €/m2, depending on the site and storage capacity. In order to confirm the major statements, within a sensitivity analysis, it is shown that a variation of SF and storage costs does not have a significant impact on the relative breakeven costs of the LF system.
publisherThe American Society of Mechanical Engineers (ASME)
titleEnergetic Comparison of Linear Fresnel and Parabolic Trough Collector Systems
typeJournal Paper
journal volume136
journal issue4
journal titleJournal of Solar Energy Engineering
identifier doi10.1115/1.4027766
journal fristpage41015
journal lastpage41015
identifier eissn1528-8986
treeJournal of Solar Energy Engineering:;2014:;volume( 136 ):;issue: 004
contenttypeFulltext


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