Water heaters use solar selective coatings to convert solar energy into thermal energy. These coatings must meet three criteria to be helpful: showing high absorption, α, in the spectral range from 0.4 to 2.5 μm, having a low emission, ε, in the infrared range from 2.5 to 50 μm, and demonstrating high selectivity, α/ε, at 100 °C. The ideal selective coating shows reflection with R = 0 in the visible region and R = 1 in the infrared, i.e., the black body spectra. Tabor produced the first commercially valuable absorbent coating by electro-galvanization 1995
[66]. Chrome has become the typical product in the marketplace
[67]. Today’s commercial absorbent layers are produced with vacuum deposition techniques with excellent results. Alanod launched on the market various commercial products such as mirotherm Control
®, mirotherm
®, eta plus
®, and mirosol
® with α
s and ε
T up to 97% and 4% (
b/
w = 24.25), with the PVD technique
[68]. In recent years, scientists have manufactured solar absorbent coatings with the sol-gel process to reduce the cost of the production facilities of these returns with great success
[69]. Based on CoCuMnO
x spinels with SiO
x coatings, coatings CuO@SiO
2 were prepared with values α
s = 0.85–0.91 and ε
T below 0.036 (α/ε = 17–18)
[70][71]. In coatings with CuCoMnO
x produced on an aluminum substrate, CuO@SiO
2 micro-containers were incorporated into these coatings of 980 μm ± 30 nm. CuO micro-containers 715 μm ± 15 nm in size were first prepared. The TEM measurement demonstrates that the CuO micro-containers are internally empty
[9]. CuO micro-containers are coated with SiO
2 to produce CuO@SiO
2 double-shell micro-containers
[9]. The concentration of CuO@SiO
2 micro-containers in the spinel coatings varied from 0 to 1 wt.%. The resulting α/ε ratio was measured in these samples
[9].
10. Electricity Generation
In a past study, it was shown that light could be trapped in ZnO micro-containers. These ZnO-type hollow light traps are beautiful as photovoltaic sun solar cells due to their high surface area for absorbing incident light, high electron mobility, and low production costs. In one study, the ZnO spheres exhibited a 400–500 nm diameter, with a power conversion efficiency of 4.33% and a short-circuit current density of 9.56 mAcm
−2 [72]. To improve the coefficient of efficiency of ZnO microspheres, multi-shell spheres with well-defined structures were produced with a defined number of inner shells and controlled distances between them through the production process. This research showed that hollow ZnO microspheres with different shell structures exhibit various energy conversion efficiency factors. The quadruple shell microstructure is one in which sunlight reflects internally multiple times, losing its energy internally, raising its performance to 5.6%
[73]. The corresponding spectrum of U.V./vis diffuse reflectance behaves accordingly. The multi-shelled ZnO hollow microspheres (M.S. ZnO HMS) were decorated with TiO
2 nano-tree (N.T.)
[74]. The TiO
2 decoration significantly enhances light scattering and increases the specific area of ZnO HMS. The I–V tests show a significant enhancement of short-circuit current density (Jsc) by controlling M.S. Combining ZnO HMS shell numbers and M.S. ZnO HMS with TiO
2 NT reaches a power conversion efficiency (PCE) of 7.40%
[74]. In addition, combining T.S. ZnO HMS with TiO
2 NT increases light-collecting efficiency and extends electron lifetime. Another approach was made using CdS and CdSe quantum dots to decorate the surface of the ZnO core/shell hollow microspheres to increase the light scattering of the ZnO hollow structure
[75]. The new system improved power conversion efficiency by 76.22% and 21.74%, higher than in ZnO N.P.s and ZnO HMS
[75].