Effect of microcracking on ionic conductivity in LATP

被引:171
作者
Jackman, Spencer D. [1 ]
Cutler, Raymond A. [1 ]
机构
[1] Univ Utah, Dept Mat Sci & Engn, Salt Lake City, UT 84112 USA
关键词
LATP; Ionic conductivity; Microcracking; Strength; Fracture toughness; THERMAL-EXPANSION BEHAVIOR; IMPEDANCE SPECTROSCOPY; CERAMICS; NA; CHEMISTRY; ZIRCONIA; M=LI; ZR;
D O I
10.1016/j.jpowsour.2012.06.081
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Because of high thermal expansion anisotropy, lithium aluminum titanium phosphate (LATP) is prone to microcrack generation. While much attention has been given to the role of grain boundary phases on the ionic conductivity of LATP, the effect of microcracking is also expected to lower conductivity. While all LATP materials characterized had grains larger than the critical size for microcracking, fine-grained (1.7 +/- 0.7 mu m) Li1.3Al0.3Ti1.7(PO4)(3) had twice the ionic conductivity of the same purity of coarse-grained (4.8 +/- 1.9 mu m) LATP at 323 K due to less extensive cracking at grain boundaries. While the increase in Young's modulus (81-115 GPa) and biaxial strength (26 +/- 2 MPa to 123 +/- 17 MPa) is consistent with the reduction in grain size, the increase in conductivity is a strong driving force for avoiding large LATP grains. Lower purity degraded ionic conductivity for similar grain sizes, as expected. Single-edged precracked beam fracture toughness measurements showed that the fine-grained, high-purity IATP has a K-1c value of 1.1 +/- 0.3 MPa root m. Flexural strength measurements (147 +/- 14 MPa) indicated that the critical flaw size was on the order of 30 mu m, with processing flaws still limiting strength. It is expected that as grain size is further reduced, strength and ionic conductivity will continue to improve in tandem until microcracking is eliminated. (C) 2012 Elsevier B.V. All rights reserved.
引用
收藏
页码:65 / 72
页数:8
相关论文
共 38 条
[1]  
[Anonymous], 2009, ASTMC149909
[2]  
[Anonymous], 2010, 142110 ASTM
[3]   IONIC-CONDUCTIVITY OF THE LITHIUM TITANIUM PHOSPHATE (LI1+XALXTI2-X(PO4)3), (LI1+XSCXTI2-X(PO4)3), (LI1+XYXTI2-X(PO4)3), (LI1+XLAXTI2-X(PO4)3 SYSTEMS [J].
AONO, H ;
SUGIMOTO, E ;
SADAOKA, Y ;
IMANAKA, N ;
ADACHI, GY .
JOURNAL OF THE ELECTROCHEMICAL SOCIETY, 1989, 136 (02) :590-591
[4]   Lithium mobility in titanium based Nasicon Li1+xTi2-xAlx(PO4)3 and LiTi2-xZrx(PO4)3 materials followed by NMR and impedance spectroscopy [J].
Arbi, K. ;
Rojo, J. M. ;
Sanz, J. .
JOURNAL OF THE EUROPEAN CERAMIC SOCIETY, 2007, 27 (13-15) :4215-4218
[5]  
ASTM, 2008, ASTM Designation: C 1161-02c
[6]  
Balapanov M.K., 2006, B RUSS ACAD SCI PHYS, V70, P1064
[7]  
Best A. S., 1998, Journal of the Australasian Ceramic Society, V34, P236
[8]  
Bradt RC., 1995, CERAM T, V52, P5
[9]  
Ceilings P.J., 1996, CRC HDB SOLID STATE, P10
[10]   GRAIN SIZE MICROCRACKING RELATIONS FOR PSEUDO-BROOKITE OXIDES [J].
CLEVELAND, JJ ;
BRADT, RC .
JOURNAL OF THE AMERICAN CERAMIC SOCIETY, 1978, 61 (11-1) :478-481