2008
DOI: 10.1111/j.1551-2916.2008.02294.x
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New Approach to the β→α Polymorphic Transformation in Magnesium‐Substituted Tricalcium Phosphate and its Practical Implications

Abstract: The transformation β→α in Mg‐substituted Ca3(PO4)2 was studied. The results obtained showed that, contrary to common belief, there is, in the system Mg3(PO4)2–Ca3(PO4)2, a binary phase field where β+α‐Ca3(PO4)2 solid solutions coexist. This binary field lies between the single‐phase fields of β‐ and α‐Ca3(PO4)2 solid solution in the Ca3(PO4)2‐rich zone of the mentioned system. In the light of the results and the Palatnik–Landau's Contact Rule of Phase Regions, a corrected phase equilibrium diagram has been pro… Show more

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Cited by 103 publications
(86 citation statements)
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“…(1250 °C). Based on results reported on the literature [22][23][24] depending on the Magnesium content in the precursors employed the temperature at which pure α-TCP can be synthesized could be raised up to 1500 °C, however, if the material is sintered at the right temperature and for enough time to guarantee the total β → α conversion it is possible to obtain pure α-TCP no matter how high is the Mg contamination. Then, if the powders synthesized on this…”
Section: Discussionmentioning
confidence: 99%
“…(1250 °C). Based on results reported on the literature [22][23][24] depending on the Magnesium content in the precursors employed the temperature at which pure α-TCP can be synthesized could be raised up to 1500 °C, however, if the material is sintered at the right temperature and for enough time to guarantee the total β → α conversion it is possible to obtain pure α-TCP no matter how high is the Mg contamination. Then, if the powders synthesized on this…”
Section: Discussionmentioning
confidence: 99%
“…In these reports the boundary between the field of the low temperature β-TCPss and the high temperature α-TCPss is a line (one-dimension), which contradicts Palatnik-Landau's Contact Rule of Phase Regions (CRPR), lately reformulated as the Boundary Theory (BT) (53)(54)(55)(56)(57). As stated by the CRPR and the BT a phase boundary line (one-dimension) cannot separate two mono-phase fields in a binary phase equilibrium diagram at constant pressure (47).…”
Section: Glassmentioning
confidence: 89%
“…Due to the differences in solubility of β-TCPss and α-TCPss the coexistence of both phases in equilibrium becomes evident. Besides, neutron and X-ray diffraction experiments confirmed the reconstructive character of the α↔β transition, which requires to surpass a large activation energy barrier to proceed and indicates that quenching is not required to retain the pure α-TCP phase, but it is only needed to reach a temperature inside the primary field of α-TCP ss and to keep it for a period of time enough to complete the β→α transformation (47).…”
Section: Glassmentioning
confidence: 97%
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