Elsevier

Applied Thermal Engineering

Volume 77, 25 February 2015, Pages 42-56
Applied Thermal Engineering

Research paper
Multi-objective and thermodynamic optimisation of a parabolic trough receiver with perforated plate inserts

https://doi.org/10.1016/j.applthermaleng.2014.12.018Get rights and content

Highlights

  • The study focuses on the use of perforated plate inserts in a parabolic trough receiver.

  • Multi-objective and thermodynamic optimisation of the receiver is investigated.

  • Influence of Reynolds numbers, fluid temperature and insert geometry is presented.

  • Pareto optimal solutions and optimal insert configurations are presented.

  • Optimal Reynolds at which entropy generation is a minimum is obtained and presented.

Abstract

In this paper, multi-objective and thermodynamic optimisation procedures are used to investigate the performance of a parabolic trough receiver with perforated plate inserts. Three dimensionless perforated plate geometrical parameters considered in the optimisation include the dimensionless orientation angle, the dimensionless plate diameter and the plate spacing per unit meter. The Reynolds number varies in the range 1.02 × 104 ≤ Re ≤ 1.36 × 106 depending on the fluid temperature. The multi-objective optimisation was realised through the combined use of computational fluid dynamics, design of experiments, response surface methodology and the Non-dominated Sorted Genetic Algorithm-II. For thermodynamic optimisation, the entropy generation minimisation method was used to determine configurations with minimum entropy generation rates.

Introduction

Heat transfer enhancement in heat exchangers and in other thermal applications is of significant importance. Not only does it result in energy savings but has other benefits depending on the application under consideration such as heat exchanger weight and size reduction, reduction in device temperatures and reduction in the temperature difference between process fluids.

In parabolic trough receivers, heat transfer enhancement has potential to reduce absorber tube circumferential temperature gradients [1], [2] and also reduce absorber tube temperatures thus lower receiver thermal loss and improved receiver thermal performance [3], [4], [5]. Moreover, as parabolic trough systems with high optical efficiencies and high concentration ratios become feasible [6], [7], high heat fluxes and high absorber tube temperature gradients will result. As such, improved heat transfer performance will be essential to minimise absorber tube temperature gradients as well as improve the performance and reliability of the receiver at these high concentration ratios. More still, an increase in concentration ratios leads to increased entropy generation rates due to the increased finite temperature differences as concentration ratios increase [8], [9]. As such, heat transfer enhancement can also act to minimise the entropy generation in the receiver. For these reasons, heat transfer enhancement in parabolic trough receivers has received considerable attention in the last few decades.

Passive heat transfer enhancement techniques are widely researched and applied in many industrial applications since they require no direct power input as compared to active techniques. Several researchers have applied some of the passive heat transfer enhancement techniques to improve the performance of parabolic trough receivers. Reddy et al. [10] numerically analysed a receiver with various porous and longitudinal fin geometries. Ravi Kumar and Reddy [11] investigated the performance of the receiver with a porous disc. Different angles of orientation, porous disc heights and distances between the consecutive discs were considered. Muñoz and Abánades [2] analysed an internally helically finned absorber tube to improve the thermal performance of the receiver and minimise the temperature gradients in the receiver's absorber tube. Recently Cheng et al. [12] analysed the heat transfer enhancement of parabolic trough receivers using unilateral longitudinal vortex generators. In these studies, the potential for improved heat transfer performance in receivers with heat transfer enhancement is demonstrated.

Most heat transfer fluids used in parabolic trough receivers decompose rapidly at temperatures above 400 °C [13], [14], leading hydrogen permeation in the receiver's annulus space which exacerbates receiver heat loss. Therefore, heat transfer enhancement mechanism in the receiver's absorber tube should avoid any hot spots and absorber tube surface modification should be done while taking into account likely thermal stresses. Therefore, use of tube inserts appears to be a sure way of avoiding temperature hotspots and thermal stress in the absorber tube. Porous media or perforated inserts present several benefits when compared with solid inserts such as lightweight, low fluid friction and potential for forcing uniform flow distribution [15]. In this study, the use of perforated plate inserts for heat transfer enhancement in a parabolic trough receiver is investigated.

However, besides improving heat transfer performance, heat transfer enhancement techniques also result in an increase in fluid friction. Therefore, to optimise the performance a particular heat transfer enhancement technique, increasing the heat transfer and reducing fluid friction should be considered at the same time. This presents a multi-objective optimisation problem, in which the heat transfer performance is to be maximised and the fluid friction is to be minimised. In this case, the two objectives are conflicting with each other such that as the heat transfer performance increases the fluid friction also increases. There is no single design that is “best” for all the objectives when both objectives are of the same importance.

In such a case, a set of best solutions often called non-dominated solutions or Pareto optimal solutions [16], [17] is sought, such that selecting any one solution in place of another sacrifices quality of one of the objectives while improving the other objective. Genetic algorithms are suited for optimisation of these classes of problems in many applications including fluid flow and heat transfer problems [18]. Detailed description of genetic algorithms and their suitability for use in optimisation of multi-objective problems is provided in Refs. [17], [18]. Researchers who have used genetic algorithms for multi-objective optimisation of heat transfer and fluid flow problems include Kim et al. [19], Ndao et al. [20], Cortes-Quiroz et al. [21], [22] and Karathanassis et al. [23]. Other authors have applied multi-objective optimisation to thermal systems such as refrigeration systems [24] and energy storage systems [25], [26], [27].

Most investigations on heat transfer enhancement use the first law of thermodynamics to characterise the resulting thermo-hydraulic performance. Studies that use the second law of thermodynamics to investigate both the thermo-hydraulic and thermodynamic performance of heat transfer enhancement techniques are not wide spread. The second law of thermodynamics provides a means of specifying the quality of the available energy. In this investigation, we use both multi-objective optimisation and thermodynamic optimisation to optimise the heat transfer, fluid friction and thermodynamic performance of a parabolic trough receiver with perforated plate inserts.

Section snippets

Physical model and computational domain

The physical model of the receiver with perforated plates under consideration in this study is shown in Fig. 1(a) and (b). Similar to the conventional parabolic trough receivers, the space between the absorber tube and the glass cover is considered evacuated. Thus, only the radiation heat loss takes place between the absorber tube and the glass cover.

From Fig. 1(a), three geometrical parameters of the perforated plate are defined: the spacing between the two consecutive perforated plates (p),

Governing equations

Due to the high heat fluxes on the receiver's absorber tube, high flow rates are usually used for better heat transfer performance. Therefore, we considered the flow inside the absorber tube to be steady-state and fully developed turbulent. As such, the governing equations are:

Continuity equation(ρui)xi=0

Momentum equationxjρuiuj=Pxi+xjμuixj+ujxi23μuixiδijρuiuj¯+Sm

Energy equationxjρujcpT=xjλTxj+μtσh,tcpTxj+ujPxj+μuixj+ujxi23μuixiδij-ρuiuj¯uixjwhere -ρuiuj

Multi-objective optimisation

In its general form, a multi-objective optimisation problem can be written as [17]:Minimise/maximisefm(x),m=1,2,,M;Subjecttogj(x)0j=1,2,,J;hk(x)=0k=1,2,,K;xi(L)xixi(U)i=1,2,,n.where fm(x) is the objective function, M is the number of functions to be optimised. A solution x is a vector of n decision variables such that x = (x1, x2, … , xn)T. gj(x) and hk(x) are constraint functions with J representing the inequality constraints and K the equality constraints. The last set

Validation of numerical results

Our numerical model was validated in a number of steps. First, we have compared our results with experimental data from Dudley et al. [28] for temperature gain and collector efficiency to validate that our receiver model is accurate. Good agreement was achieved for both the temperature gain and the collector efficiency with a maximum deviation of less than 8% as shown in Table 3.

The perforated plate model was validated using data from Gan and Riffat [43]. The variation of the pressure

Conclusion

In the present study, the use of multi-objective optimisation and thermodynamic optimisation in arriving at optimal solutions for a receiver with perforated plate inserts was presented. In the multi-objective optimisation part, the NSGA-II algorithm was used to obtain Pareto optimal solutions for the Nusselt number and pressure drop. Using a goal-based, weighted, aggregation-based decision ranking method, representative design candidates were obtained and presented.

In the thermodynamic

Acknowledgements

The funding received from NRF, TESP, and Stellenbosch University/University of Pretoria, SANERI/SANEDI, CSIR, EEDSM Hub and NAC is duly acknowledged and appreciated.

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