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9.12  Development of Microstructure in Eutectic Alloys  •  321

                                                                                  Figure 9.12  Schematic
                                                                                  representations of the equi-
                                                   x                              librium microstructures for a
                                                                       L
                                                  d        L                      lead–tin alloy of composition
                                                        (C  wt% Sn)               C 2  as it is cooled from the
                                                         2
                                                                                  liquid-phase region.
                                    300
                                                                   L
                                                  e


                                                                       + L
                                  Temperature (°C)  200     f       C  wt% Sn

                                                                     2


                                         Solvus
                                          line
                                                  g

                                    100

                                                                    +



                                                   x
                                       0      10      20      30      40      50
                                                  C 2
                                                    Composition (wt% Sn)

                                 cooling, these particles grow in size because the mass fraction of the b phase increases
                                 slightly with decreasing temperature.
                                    The third case involves solidification of the eutectic composition, 61.9 wt% Sn (C 3  in
                                 Figure 9.13). Consider an alloy having this composition that is cooled from a temperature
                                 within the liquid-phase region (e.g., 250 C) down the vertical line yy¿ in Figure 9.13. As
                                 the temperature is lowered, no changes occur until we reach the eutectic temperature,
                          : VMSE  183 C. Upon crossing the eutectic isotherm, the liquid transforms into the two a and b
                   Eutectic (Pb-Sn)
                                 phases. This transformation may be represented by the reaction
                                                         cooling
                                           L(61.9 wt% Sn) m a(18.3 wt% Sn) + b(97.8 wt% Sn)          (9.9)
                                                         heating
                                 in which the a- and b-phase compositions are dictated by the eutectic isotherm end points.
                                    During this transformation, there must be a redistribution of the lead and tin com-
                                 ponents because the a  and b  phases have different compositions, neither of which is
                                 the same as that of the liquid (as indicated in Equation 9.9). This redistribution is ac-
                                 complished by atomic diffusion. The microstructure of the solid that results from this
                                 transformation consists of alternating layers (sometimes called lamellae) of the a and
                                 b phases that form simultaneously during the transformation. This microstructure, rep-
              eutectic structure  resented schematically in Figure 9.13, point i, is called a eutectic structure and is char-
                                 acteristic of this reaction. A photomicrograph of this structure for the lead–tin eutectic
                                 is shown in Figure 9.14. Subsequent cooling of the alloy from just below the eutectic to
                                 room temperature results in only minor microstructural alterations.
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