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Optimization of a trapezoidal cavity absorber for the Linear Fresnel Reflector

M.A. Moghimi, +2 more
- 01 Sep 2015 - 
- Vol. 119, pp 343-361
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TLDR
In this article, a trapezoidal cavity absorber of an LFR (Linear Fresnel Reflector), also called a Linear Fresnel Collector (LFC), is optimized for a concentrated solar power (CSP) plant.
About
This article is published in Solar Energy.The article was published on 2015-09-01 and is currently open access. It has received 79 citations till now. The article focuses on the topics: Optimal design & Concentrated solar power.

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Citations
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Journal ArticleDOI

A review of concentrating solar thermal collectors with and without nanofluids

TL;DR: In this article, the authors reviewed the recent trends in the solar concentrating collectors and gave the emphasis on the performance enhancement methods which applied to the concentrating technologies, and concluded that the most effective enhancement methods in the concentrating solar collectors, as well as the future fields that have to be investigated.
Journal ArticleDOI

Parametric investigation of thermal characteristic in trapezoidal cavity receiver for a linear Fresnel solar collector concentrator

TL;DR: In this paper, the authors analyzed the heat transfer rate and heat loss in a trapezoidal cavity of the linear Fresnel reflector in a steady state, laminar model in which temperature-dependent density is assumed for the air inside the cavity.
Journal ArticleDOI

Progress in the design and the applications of linear Fresnel reflectors – A critical review

TL;DR: In this article, the Linear Fresnel reflector (LFR) is one of the major concentrating solar systems for producing useful heat in medium and high-temperature levels (i.e.
Journal ArticleDOI

A novel computational approach to combine the optical and thermal modelling of Linear Fresnel Collectors using the finite volume method

TL;DR: A novel 2-D:3-D phased approach to conduct the ray tracing required to quantify the optical performance of a line concentration Concentrated Solar Power (CSP) receiver, as well as the conjugate heat transfer modelling required to estimate the thermal efficiency of such a receiver.
Journal ArticleDOI

A linear Fresnel reflector as a solar system for heating water: Theoretical and experimental study

TL;DR: In this article, the authors validate the experimental work carried out in the winter of 2015 on the concentrator in the city of Algerian city "Blida" by a numerical simulation, where the tap water used as a heat carrier fluid.
References
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Book

Fundamentals of Heat and Mass Transfer

TL;DR: This paper introduced the physical effects underlying heat and mass transfer phenomena and developed methodologies for solving a variety of real-world problems, such as energy minimization, mass transfer, and energy maximization.
Book

Radiative heat transfer

TL;DR: In this article, the Monte Carlo method for thermal radiation was used to estimate the radiative properties of one-dimensional Gray Media, and the method of Spherical Harmonics (PN-Approximation) was used for the same purpose.
Book

A heat transfer textbook

Journal ArticleDOI

Relation between Surface Roughness and Specular Reflectance at Normal Incidence

TL;DR: In this paper, the roughness of a plane surface is related to its specular reflectance at normal incidence, and expressions for the case when the root mean square surface roughness is small compared to the wavelength of light are presented.
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Frequently Asked Questions (12)
Q1. What are the contributions in "Optimization of a trapezoidal cavity absorber for the linear fresnel reflector" ?

This paper focuses on applying an integrated optimization technology to a solar thermal application, more specifically for the optimization of a trapezoidal cavity absorber of an LFR ( Linear Fresnel Reflector ), also called a Linear Fresnel Collector ( LFC ), CSP plant. This paper uses a commercial tool to find an optimal design for a set of operating conditions. In this paper the effect of absorbed irradiation is introduced in the form of an outer surface of pipe temperature. 

Due to the assumption of external forced convection provided by an approaching wind, a constant convective surface heat transfer coefficient was chosen. 

The requirement for accuracy when modeling naturally convective flow is that the pressure variation should be insignificant when compared to temperature variation. 

The main types of CSP plants that exist or are in various stages of development and research are: Parabolic Trough Collector (PTC), Parabolic Dish Reflector (PDR), Heliostat Field Collector (HFC), and Linear Fresnel Reflector (LFR). 

radiation remains the dominant heat transfer mechanism in the whole cavity and therefore also the main heat loss contributor. 

At the wall, the boundary intensity for all outgoing directions in a specific band λ∆ is given byλ∆π λ λ ,out0 q The author= 16It should be considered that for a non-gray diffuse semi-transparent wall, the heat flux on the two sides of a medium is calculated using equations 14 and 15 for each medium, while the incident intensity Iin is calculated from a complicated mathematical equation (omitted for brevity), which is related to the refractive indices for the media. 

The spatial discretization of the equations for pressure, momentum, energy and discrete ordinates was chosen as PRESTO, second-order upwind, second-order upwind, and first-order upwind, respectively. 

In addition, the aperture size is held fixed at 1231.3mm to satisfy the condition of a given optical system having almost constant intercept factors and a fixed overall output in the optical domain. 

The RTE was solved every 10 iterations of the coupled mass, momentum and energy equation set in order to allow the adjusted radiation heat source to influence the flow in the domain. 

if the root mean square (RMS) surface roughness is less than incident radiation wavelength, then the surface acts as specular (Bennett and Porteus, 1961), else it acts as diffuse. 

The external shape directly influences the wind load (according to Bhaduri and Murphy (1985), the projected area (Figure 4) is directly proportional to the wind load on low-height structures with a height-dependent velocity coefficient also playing a role. 

As mentioned by Modest (2013), from a physical viewpoint, the net loss of radiative energy from a control volume is equal to emittance of energy from that volume minus the absorbed incident radiation to it.