2019
DOI: 10.1039/c8ta05333b
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Efficient cycling utilization of solar-thermal energy for thermochromic displays with controllable heat output

Abstract: Photo-thermal energy cycles for thermochromic displays with control of heat output.

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Cited by 91 publications
(60 citation statements)
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“…For ideal solar heating, it is expected the material has high absorption in 200-2500 nm and low emissivity in >2500 nm 7 . Prior research efforts for both solar heating [8][9][10][11] and radiative cooling [12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29] have yielded both high technological performance and deep scientific understanding, which spans from a variety of fields, including materials science, photonics and plasmonics, and heat transfer. However, they are mostly static or quasi-dynamic devices, which cannot completely solve the dynamic heating and cooling demand problem effectively, especially in the daytime [12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29] .…”
mentioning
confidence: 99%
“…For ideal solar heating, it is expected the material has high absorption in 200-2500 nm and low emissivity in >2500 nm 7 . Prior research efforts for both solar heating [8][9][10][11] and radiative cooling [12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29] have yielded both high technological performance and deep scientific understanding, which spans from a variety of fields, including materials science, photonics and plasmonics, and heat transfer. However, they are mostly static or quasi-dynamic devices, which cannot completely solve the dynamic heating and cooling demand problem effectively, especially in the daytime [12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29] .…”
mentioning
confidence: 99%
“…The broad exothermic peak in a heating curve arose from the thermally induced cis→trans isomerization in the melt, which revealed ΔHisom of 160-190 J/g (consistent with the molar enthalpy of 52 kJ/mol), falling in the range of the attainable energy density by azobenzene compounds (< 200 J/g). [5a,6a,18] Little exothermicity was observed below 80 o C and the exothermic peak temperatures were as high as ~135 o C, manifesting the very high storage stability of our molecular materials compared to that of the reported solar thermal batteries, including small-molecule azobenzenes, [18] azopolymers, [19][20][21][22] nanocarbon-templated azobenzene hybrids, [23] and phase-changeable ionic azo materials. [16] The sharp exothermic peak in a cooling curve represents the rapid transition from trans-liquid to trans-crystal, and it provides ΔHcryst of about 140-210 J/g.…”
Section: Resultsmentioning
confidence: 93%
“…The solar energy storage of the composite in this study is driven by azobenzene‐based isomerization and phase change. Compared with the pure azobenzene derivatives as solar thermal fuel, this energy density is higher [13b,c,14,25] (Figure 4b). The approaches to improve the energy density by grafting and polymerization increase the energy barrier of isomerization, as a result decreasing the isomerization extent (Δ ξ ) and isomerization speed (release speed).…”
Section: Resultsmentioning
confidence: 99%
“…a) Energy release obtained by DSC and calculated on the charged C 14 OH@C 14 Azo with various mole ratios in the exothermic and endothermic process, including of phase change and isomerization. b) A comparison of the energy density from the latest reports: ○ , Azo‐based hybrid; [10b,c,11b,13a] □ , mono‐Azo‐based material; [13b,c,14,25a] ▽ , composites of Azo and PCM; [5a,6a] ☆ , this paper. c) Possible energy storage mechanism.…”
Section: Resultsmentioning
confidence: 99%
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