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Reflection spectra of various ITO-coated glass substrates (the “Geomatec” sample used a thicker substrate).

Reflection spectra of various ITO-coated glass substrates (the “Geomatec” sample used a thicker substrate).

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Solar thermal collectors are radiative heat exchangers. Their efficacy is dictated predominantly by their absorption of short wavelength solar radiation and, importantly, by their emission of long wavelength thermal radiation. In conventional collector designs, the receiver is coated with a selectively absorbing surface (Black Chrome, TiNO x , etc....

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... A comprehensive comparison of selective transmitters was reported in [25], concluding that ZnS/Ag/Zns and ITO perform best at low cost for the latter. ITO was also reported as an antireflection coating for silicon solar cells [26], while filters with appropriate cut-off at 1200 nm, suitable for silicon solar cells, were reported in [27]. ...
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... The outer surface of the inner glass tube is coated with a copper-aluminum alloy coating that absorbs solar radiation. This material has gained widespread usage due to its low cost and high heat absorption efficiency [43]. To determine if there were significant differences in the cooling of each vacuum tube, three T-shaped thermocouples (−200~350 • C) were installed on the outer surface of the vacuum tubes facing the ground and sky, respectively, along the length of the vacuum tube array at the 1st, 6th, 11th, and 15th vacuum tubes from the left. ...
... Energies 2023, 16, x FOR PEER REVIEW 11 of 2 meant that it had little obstruction to the outward heat radiation during cooling at nigh The outer surface of the inner glass tube is coated with a copper-aluminum alloy coatin that absorbs solar radiation. This material has gained widespread usage due to its low cos and high heat absorption efficiency [43]. To determine if there were significant difference in the cooling of each vacuum tube, three T-shaped thermocouples (−200~350 °C) wer installed on the outer surface of the vacuum tubes facing the ground and sky, respectively along the length of the vacuum tube array at the 1st, 6th, 11th, and 15th vacuum tube from the left. ...
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... By stacking combinations of these quarter wavelength designs together, the resulting dichroic mirror can be designed to create a simple edge-pass/edge-stop filter or a band-stop/band-pass optical element (such as the one used in Green et al. [421]). Several companies offer stock and custom designs of these materials [422][423][424], but they are typically orders of magnitude too expensive (e.g., 1 × 10 5 to 1 × 10 6 USD/m 2 ) for PV-T collectors [425]. Ignoring their cost, nearly ideal optical properties can be achieved through careful design. ...
... With these so-called 'low-emissivity' windows, modern buildings can reduce their solar heat gain (and indoor heat loss) without reducing the amount of natural daylight they receive. This feature is enabled by spectral splitting dichroic coatings deposited on the inner pane of a double or triple-glazed frame (which reflects all solar wavelengths except the visible light) [425]. Given their ubiquitous use in high-efficiency buildings, dichroic-coated glass might also be mass-produced for PV-T products in the future. ...
... Given their ubiquitous use in high-efficiency buildings, dichroic-coated glass might also be mass-produced for PV-T products in the future. This would require two fundamental changes from today's architectural glazing manufacturing processes: (a) broadening of the transmitted spectrum (perhaps requiring different materials and layer thicknesses) to shift the transmission window from about 450 to 750 nm to, say, 700-1100 nm band for Silicon cells [425]; and (b) use of low-iron or 'solar glass' substrates (rather than typical window glass), which is less absorbing of these longer wavelengths. ...
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... In recent years, thin films have attracted great attention for various applications such as solar cells [1], supercapacitor, counter electrode, thermal sensors [2], catalysts, solar selective coatings [3], diluted magnetic materials [4] and anode materials. Because of these semiconductor materials showed unique physical properties [5], optical [6] and electrical behaviors. ...
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... The downside of using nanofluid-based DASCs should be considered. Firstly, as indicated by Hewakuruppu et al. [18] and Taylor et al. [19], rather than using a low-emissivity selective surface, thermal emission emanates the basefluids of DASCs, so: Q radiation loss ¼ A surface s ε basefluid T 4 basefluid , where ε basefluid $ 1. This can become a major source of energy loss as T basefluid increases much above ambient temperatures. ...
... This can become a major source of energy loss as T basefluid increases much above ambient temperatures. This means most of the DASC proposed in the literature would be inefficient and uncompetitive at temperatures >100 C. To address this issue, transparent solar selective surfaces (SSS) have been proposed as a cover for DASCs [19]. Another issue for nanofluid-based DASCs is that nanofluids intrinsically increase the pumping power (over pure fluids) [20] because they usually exhibit higher viscosity than their basefluids. ...
... As mentioned earlier, a transparent substrate coated with a layer of ITO was selected as the best available SSS for solar thermal application. As this ITO was custom-made, the modeled refractive indices were kindly provided by a fellow researcher [19]. These constants were plugged into OpenFilters [26], then transmission and reflection spectra were given to an ITO manufacturer and a sample with~250 nm thick ITO (corresponding to the optimised thickness for 400 C in Ref. [19]) on quartz was fabricated via magnetron sputtering by Geomatec, Japan (see Fig. 1h). ...
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... Solar selective surfaces are well-developed and they have been commonly realized using cermets, metal oxides, metals coated with thin-films comprising dielectric/metal/dielectric sandwich structures or semiconductors, and metal surfaces textured on the micron scale [2][3][4][5][6][7]. While a wide range of selective surfaces that absorb solar energy are available for different applications, their transparent counterparts are underdeveloped [8]. Transparent selective surfaces, or "transparent heat mirrors", are technologically desirable for the advancement of concentrated solar technologies that employ volumetric receivers [9][10][11][12][13]. ...
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... Nanofluids-water, oils, gases containing nanoparticles-have been proven to provide heat transfer enhancements [2][3][4] and control over the optical properties [5][6][7] of their base fluid. However, these benefits (e.g., increased convective heat coefficients) are often largely cancelled out by the increased viscosity resulting from the addition of nanoparticles [8]. ...
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Solar energy can be converted into useful energy via photovoltaic cells or with a photothermal absorber. While these technologies are well-developed and commercially viable, significant benefits can be realised by pulling these two technologies together in photovoltaic/thermal (PV/T) systems which can provide both heat and electricity from a single collector. Emerging configurations in the PV/T field aim to incorporate micro and/or nanotechnology to boost total solar utilisation even further. One example of this is the nanofluid-based PV/T collector. This type of solar collector utilises nanofluids—suspensions of nanoparticles in traditional heat transfer fluids—as both an optical filter and as a thermal absorber. This concept seeks to harvest the whole solar spectrum at its highest thermodynamic potential through specially engineered nanofluids which transmit the portion of solar spectrum corresponding to the PV response curve while absorbing the rest as heat. Depending on the nanoparticle concentration, employing nanofluids in a flowing system may come with a price—an efficiency penalty in the form of increased pumping power (due to increased viscosity). Similarly, microchannel-based heat exchangers have been shown to increase heat transfer, but they may also pay the price of high pumping power due to additional wall-shear-related pressure drop (i.e., more no-slip boundary area). To develop a novel PV/T configuration which pulls together the advantages of these micro and nanotechnologies with minimal pumping power requirements, the present study experimentally investigated the use of nanofluids in patterned hydrophobic microchannels. It was found that slip with the walls reduced the impact of the increased viscosity of nanofluids by reducing the pressure drop on average 17% relative to a smooth channel. In addition, flowing a selective Ag/SiO2 core–shell nanofluid over a silicon surface (simulating a PV cell underneath the fluid) provided a 20% increase in solar thermal conversion efficiency and ~3% higher stagnation temperature than using pure water. This demonstrates the potential of this proposed system for extracting more useful energy from the same incident flux. Although no electrical energy was extracted from the underlying patterned silicon, this study highlights potential a new development path for micro and nanotechnology to be integrated into next-generation PV/T solar collectors.
... Another noted improvement is the potential for reduced life cycle energy because of the elimination of the absorber surface [44], but it should also be noted that operating a DASC has some inherent limitations. A seminal work by Hewakuruppu et al. identified and studied the limitations of DASC as it relates to selectivity [45], and based on earlier studies by Taylor et al. [46]. This limitation shows up in considering the parameter a 2 in equation (2), the non-linear loss term associated with radiation (and to a lesser degree in term a 1 ). ...
... Taylor et al. identified an inherent problem in the DASC, especially for temperatures operating above 100 C, in that the base fluids have inherently high emissivity in the infrared [46]. A typical solar thermal absorber operating at high temperatures is designed to be solar selective with a high solar absorptance and low thermal emittance with an ideal cutoff wavelength defined by the operating temperature [47]. ...
Article
Over the last 100 plus years, solar thermal energy has been used for residential heating applications, industrial process heating, electricity generation, and thermochemical reactions. Because of the vast number of applications, numerous designs have been developed to improve the efficiency of converting incoming solar energy into useful heat and to lower the cost. Conventional solar thermal collectors required a solid surface to absorb and convert incoming solar energy to useful thermal energy. Developments in materials science have enabled a new type of absorber—a volumetric absorber—which utilizes nanoparticles suspended in a fluid to absorb sunlight. Since most working fluids only weakly absorb sunlight, well-engineered ‘nanofluids’ are attractive because only a low volume fraction of nanoparticles is needed to obtain a large shift in the optical properties. This review, on the 10-year anniversary of the first appearance of nanofluid-based direct absorption solar thermal collectors, provides a forward-looking perspective on the challenges and opportunities associated with nanofluids as direct absorbers. Through a critical comparison of design considerations, as well as the most recent experimental results of less well explored areas like hybrid photovoltaic/thermal systems and direct steam generation, this review aims to provide discourse on the next steps for development.
... Some of these are already commercialized [19]. Very recent research on multilayer [9,20] or composite SSCs [21] addressed even temperatures in the range up to 1000 K. Textured surfaces [22] and selective transmitters [23] can also provide solar selectivity. The application of transparent conductive oxides (TCOs) for low emissivity glasses was studied intensively as shown in the work of Granqvist [4], but only a few studies using TCOs on an absorbing substrate were published. ...
... The stack was thermally stable at 973 K in vacuum for up to 10 h when prepared with a SiO 2 interlayer between metal substrate and TCO [26]. Taylor et al. studied a wide range of TCOs including F-, Sb-and Cd-doped SnO 2 (FTO, ATO, CTO), Sn doped In 2 O 3 (ITO) and B-, Al-, Ga-and F-doped ZnO (BZO, AZO, GZO, FZO) [23]. In that theoretical study, ITO and FTO showed the best solar selectivity in the temperature range up to 873 K. ...
Article
The transparent conductive oxide (TCO) SnO 2 :Ta is developed as a selectively solar-transmitting coating for concentrated solar power (CSP) absorbers. Upon covering with an antireflective layer, a calculated absorptivity of 95% and an emissivity of 30% are achieved for the model configuration of SnO 2 :Ta on top of a perfect black body (BB). High-temperature stability of the developed TCO up to 1073 K is shown in situ by spectroscopic ellipsometry and Rutherford backscattering spectrometry. The universality of the concept is demonstrated by transforming silicon and glassy carbon from non-selective into solar-selective absorbers by depositing the TCO on top of them. Finally, the energy conversion efficiencies of SnO 2 :Ta on top of a BB and an ideal non-selective BB absorber are extensively compared as a function of solar concentration factor C and absorber temperature T H. Equal CSP efficiencies can be achieved by the TCO on BB configuration with approximately 50% lower solar concentration. This improvement could be used to reduce the number of mirrors in a solar plant, and thus, the levelized costs of electricity for CSP technology.