Fundamentals of Materials Science and Engineering: An Integrated Approach, 3e

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GTBL042-10 GTBL042-Callister-v2 August 13, 2007 18:16


368 • Chapter 10 / Phase Diagrams

+ L
 + L

C 4
Composition (wt % Sn)

Temperature (

°C)

L

(Pb) (Sn)
18.3 61.9 97.8

100

0

200

300

PRQ



Figure 10.18 The lead–tin
phase diagram used in
computations for relative
amounts of primaryαand
eutectic microconstituents
for an alloy of composition
C′ 4.

composition of 61.9 wt% Sn. Hence, the lever rule is applied using a tie line between
theα−(α+β) phase boundary (18.3 wt% Sn) and the eutectic composition. For
example, consider the alloy of compositionC′ 4 in Figure 10.18. The fraction of the
eutectic microconstituentWeis just the same as the fraction of liquidWLfrom which
it transforms, or

We=WL=

P


P+Q


=


C 4 ′− 18. 3


61. 9 − 18. 3


=


C 4 ′− 18. 3


43. 6


(10.10)


Lever rule expression
for computation of
eutectic
microconstituent and
liquid phase mass
fractions
(compositionC′ 4 ,
Figure 10.18) Furthermore, the fraction of primaryα,Wα′, is just the fraction of theαphase
that existed prior to the eutectic transformation or, from Figure 10.18,

Wα′=

Q


P+Q


=


61. 9 −C 4 ′


61. 9 − 18. 3


=


61. 9 −C 4 ′


43. 6


(10.11)


Lever rule expression
for computation of
primaryαphase
mass fraction

The fractions oftotalα,Wα(both eutectic and primary), and also of totalβ,Wβ,
are determined by use of the lever rule and a tie line that extendsentirely across the
α+βphase field. Again, for an alloy having compositionC′ 4 ,

Wα=

Q+R


P+Q+R


=


97. 8 −C 4 ′


97. 8 − 18. 3


=


97. 8 −C 4 ′


79. 5


(10.12)


Lever rule
expression for
computation of total
αphase mass fraction
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