Elsevier

Thin Solid Films

Volume 735, 1 October 2021, 138869
Thin Solid Films

Multilayers for efficient thermal energy conversion in high vacuum flat solar thermal panels

https://doi.org/10.1016/j.tsf.2021.138869Get rights and content

Highlights

  • Selective Solar absorbers designed to work in high vacuum flat panels were realized.

  • The refractive index of the single layers was assessed by ellipsometry measurements.

  • Solar to Thermal energy conversion efficiency of 60% at 250 °C was obtained.

  • Stagnation temperature of 380 °C for 1000 W/m2 illuminating power density was achieved.

  • Thermal stability of SSA was demonstrated at 400 °C under high vacuum for four hours.

Abstract

Multilayer absorbers based on Cr2O3 and Cr, designed to improve the solar-to-thermal conversion efficiency at mid temperatures in high vacuum flat thermal panel, are fabricated via sputtering deposition on bulk copper substrates and characterized by thermal and optical analysis. The refractive index of the single layers has been measured and used to estimate absorber thermal efficiency at the operating temperatures. Multilayers have been produced via sputtering deposition on bulk copper substrates. The absorber multilayers can be 10% more efficient than the commercial alternative at 250 °C operating temperatures, reaching 380 °C stagnation temperature without sun concentration. The thermal stability has been checked at temperature of 400 °C in vacuum for four hours. High vacuum flat thermal collectors, equipped with the produced selective solar absorbers can obtain unprecedented performances and can give important contribution to the energy transition from fossil fuels to renewable energy for efficient heat production.

Introduction

The energy transition from fossil fuels to renewable energy is an important goal of our society and solar energy can play a key role in such transition [1]. Almost one third of the energy resources in the developed countries is nowadays used for heating and cooling [2,3], and a large fraction of this energy can be provided by highly efficient solar thermal collectors. The most efficient solar thermal collector in the low temperature range is the High Vacuum solar thermal Flat Panel (HVFP) [4] produced by TVPSolar SA [5]. The Selective Solar Absorber (SSA) is the key component in determining the efficiency in HVFP. The SSA idea was introduced at the end of 1950, and thenceforward several works have been devoted to SSA optimization. To fabricate an SSA with an emissivity curve close to the ideal one, different designs have been analyzed by several authors in the past years both for concentrated and unconcentrated applications [6,[7], [8]], such as nanomultilayers[8], ceramic and metal structrures (cermet) [9], nanocermet and self-doped nanocermet [10], multilayers [11], photonic designs [12], multilayered cermets [13]. In particular, its thermal emittance determines the radiation losses, that represent the main loss source thanks to the presence of high vacuum. As explained by Cao [9] at temperature higher than 100 °C without concentration, the thermal emittance gains importance over the thermal absorption. However, all absorbers available in commerce [14,15] and most of the absorbers present in literature [16,17] have been developed to work for concentrated solar applications [18] or for low temperature (< 100 °C) applications: in both conditions, to obtain high efficiency, the absorptance is more important than thermal emittance.

As pointed out by Moss and coworkers [19], HVFPs can be the most efficient collectors also at temperature up to 250 °C if they were equipped with an optimized SSA with thermal emittance of 0.04. Unfortunately, commercially available absorbers have such low emittance value only at room temperature. Their emittance increases to 0.1 or more at temperatures higher than 200 °C resulting in an increase of radiative power losses, with a consequent decrease in efficiency. Very few scientific studies have been performed on SSAs for unconcentrated applications. The only SSAs developed to work in unconcentrated environment and temperature higher than 100 °C, are reported in [20,21]. The SSA based on semiconductor multilayer developed in [20] only reaches 220 °C as maximum temperature and authors claim that it could optimized to reach 300 °C maximum temperature. A SSA based on metal/dielectric multilayer, reported in [21], was deposited by electron beam evaporation technique (e-beam) on a glass/metal substrate. The glass substrate was chosen to perform ellipsometric characterization avoiding the roughness contribution to the optical response. Results were very promising: a very selective emissivity curve was obtained opening the route to high efficiencies in the temperature range (150-300) °C without concentration. However, the produced samples could not be measured in operating conditions [21] and preliminary results on copper bulk substrates indicated that the temperature stability is not adequate to mid temperature applications.

Nowadays, a commercially available SSA (Mirotherm from Alanod) is mounted in HVFPs, providing very good efficiency up to 150 °C operating temperatures. In the present study we present SSAs based on metal (Cr) and dielectric (Cr2O3) multilayer deposited on Cu industrial substrate via DC magnetron sputtering, designed to work at temperatures higher than 150 °C. They have been characterized in operating conditions by absorptance and thermal emittance measurements. SSA thermal stability was also verified at 400 °C under vacuum for 4 hours.

Section snippets

Experimental and theoretical details

The most important properties of a SSA are the spectrally averaged absorptivity α¯ (also referred to as solar absorptance) and the spectrally averaged emissivity ε¯(T) (also referred to as thermal emittance). They are defined and calculated according to the following Eqs. [22]:α¯=0μmμmα(λ)S(λ)dλ0μmμmS(λ)dλε¯(T)=0ε(λ)Ebb(λ,T)dλ0Ebb(λ,T)dλwhere S(λ) (Wm−2μm−1) is the solar radiation spectrum and Ebb(λ, T) (Wm−2μm−1) is the blackbody radiation spectrum depending on the radiation wavelength

Results and discussions

Using the refractive indices reported in the Section 2.2, it is possible to predict the reflectivity of multilayer as function of the layer thicknesses. Then, using Eqs. (3), (1) and (2) is possible to calculate the spectrally average emissivity and absorptivity. In Fig. 4 a) we report the result for two coatings designed to work at Operating Temperatures (OT) higher than 150 °C (coating A: OT = 200 °C and coating B: OT = 300 °C). The reported thermal emittance is extremely low. To obtain such

Conclusions

The use of Cr based multilayers to produce selective solar absorbers paves the route to the application of high vacuum flat panels as very efficient thermal solar collectors at temperature up to 250-300 °C. The multilayers are fabricated via sputtering deposition techniques and their fabrication process can be easily transferred to industrial deposition systems.

The presented selective solar absorbers have a very low emittance preserving a large absorptance and reaching stagnation temperature

Credit author statement

Davide De Maio: Investigation, Data Curation, Software, Writing - Original Draft Carmine D'Alessandro: Investigation, Data Curation Antonio Caldarelli: Investigation, Daniela De Luca: Data Curation, Visualization Emiliano Di Gennaro: Writing - Review & Editing, Supervision Maurizio Casalino: Methodology, Software Mario Iodice: Methodology, Formal analysis, Writing - Review & Editing , Mariano Gioffr`e: Resources, Validation Roberto Russo: Writing - Review & Editing, Supervision, Funding

Declaration of competing interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

The Ph.D. grant of two of the authors (DDL, AC) is funded by the PON2014-2020 “Dottorati innovativi con caratterizzazione industriale, XXXIV ciclo” program. The Ph.D. grant of one of the authors (DDM) is funded by the CNR-Confindustria “Dottorati di Ricerca Industriali” program XXXIV ciclo.

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