4.7 Article

A DSC analysis of thermodynamic properties and solidification characteristics for binary Cu-Sn alloys

期刊

ACTA MATERIALIA
卷 60, 期 19, 页码 6518-6527

出版社

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.actamat.2012.08.013

关键词

Differential scanning calorimetry (DSC); Enthalpy of fusion; Undercooling; Peritectic solidification; Metatectic transformation

资金

  1. National Natural Science Foundation of China [50971105, 51201136, 51101123]
  2. Fundamental Research Funds of Northwestern Polytechnical University [JC20110280, JC20120245]

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The liquidus temperatures and enthalpies of fusion for Cu-Sn alloys are systematically measured across the whole composition range by differential scanning calorimetry (DSC). The liquidus slope vs. Sn content is derived on the basis of the measured results. The measured enthalpy of fusion is related to the Sn content by polynomial functions, which exhibit one maximum value at 55 wt.% Sn and two minimum values around 28.9 wt.% Sn and 90 wt.% Sn, respectively. The undercoolability of those liquid alloys solidifying with primary a (Cu) solid solution phase is stronger and can be further enhanced by increasing the cooling rate. However, other alloys with the preferential nucleation of intermetallic compounds display smaller undercoolings and are not influenced by cooling rate. Microstructural observations reveal that peritectic reactions can rarely be completed. With the increase in undercooling, the primary alpha (Cu) dendrites are refined in the peritectic Cu-22 wt.% Sn alloy. For the hyperperitectic Cu-70 wt.% Sn alloy, typical peritectic cells are formed in which the peritectic eta(Cu6Sn5) phase has wrapped the primary epsilon(Cu3Sn) phase. The DSC curves of metatectic-type Cu-Sn alloys indicate that the metatectic transformation gamma -> epsilon + L upon cooling is an exothermic event, and a large undercooling of 70 K is required to initiate this transformation in metatectic Cu-42.5 wt.% Sn alloy. The metatectic microstructures are characterized by (epsilon + eta) composite structures. The eta phase is mainly distributed at the grain boundaries of the coarse epsilon phase, but are also dispersed as small particles inside epsilon grains. The volume fraction of the eta phase increases with the Sn content. (c) 2012 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.

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