| CONDENSED MATTER: STRUCTURAL, MECHANICAL, AND THERMAL PROPERTIES |
Prev
Next
|
|
|
Influence of hydration on the thermal transport properties of yttria-doped barium zirconate |
| Jianqun Gao(高健群)1, Zhaoyang Wang(王朝阳)2,†, Yuhang Jing(荆宇航)3, and Yufei Gao(高宇飞)4 |
1 School of Electrical and Electronic Engineering, University of Sheffield, Sheffield S1 3JD, England; 2 School of Intelligent Manufacturing, Nanyang Institute of Technology, Nanyang 473000, China; 3 Department of Astronautical Science and Mechanics, Harbin Institute of Technology, Harbin 150001, China; 4 School of Energy and Power Engineering, Dalian University of Technology, Dalian 116024, China |
|
|
|
|
Abstract Perovskites exhibit excellent protonic conductivity in the mid-temperature range, and among them, yttria-doped barium zirconate (BZY) is considered one of the most promising perovskite proton conductors. Molecular simulations provide an efficient approach to investigating the thermal transport behavior of nanocrystalline materials. The effect of doping concentration on the thermal transport properties of BZY structures was investigated using the equilibrium molecular dynamics (EMD) method combined with phonon spectral energy density (SED) analysis. The results show that the thermal transport properties gradually decrease with increasing doping concentration, and for structures with dopants only and without oxygen vacancies, the thermal conductivity exhibits a similar decreasing trend but remains higher than that of structures containing both dopants and oxygen vacancies. Comparison of phonon lifetime and group velocity reveals that oxygen vacancy defects enhance phonon scattering, thereby leading to a reduction in thermal transport properties, while doping reduces the thermal transport properties by weakening lattice harmonicity. The effect of different hydration levels on the thermal transport properties of BZY was also investigated, and the results indicate that the thermal conductivity fluctuates in structures with low hydration levels and continues to decrease as the proton defect concentration increases with hydration. Further analysis of phonon lifetime and group velocity demonstrates that proton defects reduce the thermal transport properties through both enhanced phonon diffusion and weakened harmonicity.
|
Received: 01 July 2025
Revised: 25 August 2025
Accepted manuscript online: 08 September 2025
|
|
PACS:
|
66.70.-f
|
(Nonelectronic thermal conduction and heat-pulse propagation in solids;thermal waves)
|
| |
02.70.Ns
|
(Molecular dynamics and particle methods)
|
| |
63.20.-e
|
(Phonons in crystal lattices)
|
| |
61.72.S-
|
(Impurities in crystals)
|
|
| Fund: Project supported by the National Natural Science Foundation of China (Grant No. 12172112) and the National Natural Science Foundation of China (Joint Fund for Corporate Innovation and Development-Key Program) (Grant No. U22B2082). |
Cite this article:
Jianqun Gao(高健群), Zhaoyang Wang(王朝阳), Yuhang Jing(荆宇航), and Yufei Gao(高宇飞) Influence of hydration on the thermal transport properties of yttria-doped barium zirconate 2026 Chin. Phys. B 35 026601
|
[1] Fabbri E, Pergolesi D and Traversa E 2010 Chem. Soc. Rev. 39 4355 [2] Liu Y, Fu M, Zhang Y, Liu J, Liu K and Tao Z 2024 J. Electroanal. Chem. 961 118204 [3] Loganathan S, Biswas S, Kaur G and Giddey S 2024 Processes 12 2278 [4] Kindelmann M, Escolastico S, Almar L, Vayyala A, Jennings D, Deibert W, Meulenberg W, Rheinheimer W, Bram M, Serra J, Mayer J and Guillon O 2024 J. Mater. Chem. A 12 3977 [5] Duan C, Huang J, Sullivan N and O’Hayre R 2020 Appl. Phys. Rev. 7 011314 [6] Meng Y, Gao J, Zhao Z, Amoroso J, Tong J and Brinkman K S 2019 J. Mater. Sci. 54 9291 [7] Hou J, Miao L, Hui J, Bi L, Liu W and Irvine J T 2018 J. Mater. Chem. A 6 10411 [8] Rehman J, Hanif M B, Khan M Z, Ullah M, Starostina I A, Muhammad M T and Li Z 2024 Energy Fuels 38 22637 [9] Mikami Y, Sekitani Y, Yamauchi K, Kuroha T and Okuyama Y 2024 ACS Appl. Energy Mater. 7 1136 [10] Chen G, Gao P, Kang J, Li B, Ali W, Qin Z, Lu X and Li C 2017 J. Alloys Compd. 726 403 [11] Løken A, Saeed S W, Getz M N, Liu X and Bjørheim T S 2016 J. Mater. Chem. A 4 9229 [12] Lindman A, Helgee E E and Wahnstrom G 2017 Chem. Mater. 29 7931 [13] Wang B, Bi L and Zhao X S 2018 J. Power Sources 399 207 [14] Anjaneya K C, Nayaka G P, Manjanna J, Kumar V A, Govindaraj G and Ganesha K N 2014 J. Alloys Compd. 598 33 [15] Yadav D, Nirala G, Yadav S, Kumar U, Upadhyay S and Kumar S 2021 Appl. Phys. A 127 964 [16] Radenahmad N, Afroze S, Afif A, Azad A T, Shin J S, Park J Y, Zaini J H and Azad A K 2020 Ionics 26 1297 [17] Sammes N, Phillips R and Smirnova A 2004 J. Power Sources 134 153 [18] Medvedev D A, Lyagaeva J G, Gorbova E V, Demin A K and Tsiakaras P 2016 Prog. Mater. Sci. 75 38 [19] Bi L, Daas E H and Shafi S P 2017 Electrochem. Commun. 80 20 [20] Chen G, Luo Y, Sun W, Liu H, Ding Y, Li Y, Geng S, Yu K and Liu G 2018 Int. J. Hydrog. Energy 43 12765 [21] Zajac W, Rusinek D, Zheng K and Molenda J 2013 Open Chem. 11 471 [22] Alford N M, Templeton A and Penn S J 1998 Supercond. Sci. Technol. 11 703 [23] Kamitani A, Wakana H, Adachi S and Tanabe K 2004 Phys. C Supercond. 412 1414 [24] He D, Feng Q, Fu Y, Zhang M, Chen G, Gao P and Li C 2024 J. Mater. Res. Technol. 33 9726 [25] Shen Y, Hong D, Sun T, Hou R, Zheng G, Niu Y and Chen G 2025 J. Asian Ceram. Soc. 13 89 [26] Dierickx D, Houben I, Lapin J, Delannay F and Van Der Biest O 1996 J. Mater. Sci. Lett. 15 1573 [27] Grammatika N, McLachlan D S and Sonnenberg N 1993 Supercond. Sci. Technol. 6 469 [28] Koopman M, Duncan S, Chawla K K and Coffin C 2001 Compos. Part Appl. Sci. Manuf. 32 1039 [29] Chen Z C, Tamachi T, Kulkarni R, Chawla K K and Koopman M 2008 J. Eur. Ceram. Soc. 28 1149 [30] Yamanaka S, Hamaguchi T, Oyama T, Matsuda T, Kobayashi S and Kurosaki K 2003 J. Alloys Compd. 359 1 [31] Goh W F, Khan S A and Yoon T L 2013 Model. Simul. Mater. Sci. Eng. 21 045001 [32] Liu Y, Zhang W, Wang B, Sun L, Li F, Xue Z, Zhou G, Liu B and Nian H 2018 Ceram. Int. 44 16475 [33] Qiao Z, Li S, Li Y, Xu N and Xiang K 2022 Ceram. Int. 48 12529 [34] Zeraati M, Oganov A R, Fan T and Solodovnikov S F 2024 Phys. Rev. Mater. 8 033601 [35] Stokes S J and Islam M S 2010 J. Mater. Chem. 20 6258 [36] Raiteri P, Gale J D and Bussi G 2011 J. Phys. Condens. Matter 23 334213 [37] Volz S G and Chen G 2000 Phys. Rev. B 61 2651 [38] Schelling P K, Phillpot S R and Keblinski P 2002 Phys. Rev. B 65 144306 [39] Schelling P K and Phillpot S R 2001 J. Am. Ceram. Soc. 84 2997 [40] Gao Y, Ning W, Zhang X, Liu Y, Zhou Y and Tang D 2021 Nano Energy 82 105747 [41] Bao H, Chen J, Gu X and Cao B 2018 ES Energy Environ. 1 16 [42] Wang Z, Feng T and Ruan X 2015 J. Appl. Phys. 117 084317 [43] Zhang X, Bao H and Hu M 2015 Nanoscale 7 6014 [44] Wang F, Sun Y, Zou Y, Xu B and Fu B 2023 Chin. Phys. B 32 096301 [45] Xu L and Huang J 2020 Chin. Phys. Lett. 37 080502 [46] Li Y, Qiao Z, Li S, Liu F and Tan J 2024 Ceram. Int. 50 18750 |
| No Suggested Reading articles found! |
|
|
Viewed |
|
|
|
Full text
|
|
|
|
|
Abstract
|
|
|
|
|
Cited |
|
|
|
|
Altmetric
|
|
blogs
Facebook pages
Wikipedia page
Google+ users
|
Online attention
Altmetric calculates a score based on the online attention an article receives. Each coloured thread in the circle represents a different type of online attention. The number in the centre is the Altmetric score. Social media and mainstream news media are the main sources that calculate the score. Reference managers such as Mendeley are also tracked but do not contribute to the score. Older articles often score higher because they have had more time to get noticed. To account for this, Altmetric has included the context data for other articles of a similar age.
View more on Altmetrics
|
|
|