Abstract

Molybdenum-doped zirconium tungstate (ZrW2−xMoxO8) has been widely studied because of its large isotropic coefficient of negative thermal expansion (NTE). However, low density and poor sinterability limit its production and application. In this study, relative density greater than 90% single-phase ZrW2−xMoxO8 (0.0 ≤ x ≤ 1.0) sintered bodies were fabricated by spark plasma sintering (500–600 °C for 10 min) using ZrW2−xMoxO7(OH)2·2H2O precursor powders as the starting material. High-temperature X-ray diffraction and thermomechanical analysis were used to investigate the change in the order–disorder phase transition temperature of the sintered materials; it gradually dropped from 170 °C at x = 0.0 to 78 °C at x = 0.5, and then to below room temperature at x ≥ 0.7. In addition, all sintered bodies exhibited NTE behavior. The NTE coefficient was controllable by changing the x value as follows: from −7.85 × 10−6 °C−1 (x = 0) to −9.01 × 10−6 °C−1 (x = 0.6) and from −3.22 × 10−6 °C−1 (x = 0) to −2.50 × 10−6 °C−1 (x = 1.0) before and after the phase transition, respectively. Rietveld structure refinement results indicate that the change in the NTE coefficient can be straightforwardly traced to the thermodynamic instability of the terminal oxygen atoms, which only have one coordination.

Highlights

  • Negative thermal expansion (NTE) materials, which exhibit volume contraction upon warming, have been extensively investigated because of their potential utility in many fields, especially in those requiring precisely controllable negative, positive, or near-zero coefficients of thermal expansion composites [1,2,3,4,5,6]

  • We describe the fabrication of dense, pure ZrW2−x Mox O8 (0.0 ≤ x ≤ 1.0) sintered bodies and the effect of Mo substitution for W on the phase transition temperature and NTE coefficients

  • Single-phase ZrW2−xMoxO8 (0 ≤ x ≤ 1) sintered bodies with a relative density greater than 90%

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Summary

Introduction

Negative thermal expansion (NTE) materials, which exhibit volume contraction upon warming, have been extensively investigated because of their potential utility in many fields, especially in those requiring precisely controllable negative, positive, or near-zero coefficients of thermal expansion composites [1,2,3,4,5,6]. A series of NTE materials, including the AM2 O7 , AM2 O8 , and A2 M3 O12 families have been investigated [7,8,9,10,11,12,13,14,15,16,17,18,19]. The basic model for the NTE mechanism is based on the idea that the rotation of linked polyhedra pull them in toward each other. This motion is seen more locally as the flexing of the Zr–O–W linkage through transverse motions of the O atoms without significant stretching of the Zr–O and W–O bonds

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