S. Ghosh et al. / Thermochimica Acta 505 (2010) 69–72
71
Fig. 6. Phase diagram of CaCl2–CaBr2 system.
Fig. 4. XRD pattern of samples equilibrated at 923 K.
The phase diagram consists of the following four regions:
Complete solid solution of CaCl2 and CaBr2
Solid solution rich in CaCl2 + liquid
Solid solution rich in CaBr2 + liquid
Liquid
binary system with no significant mutual solubility between the
pure components, one expects a sharp endothermic peak for the
eutectic reaction at eutectic temperature (an isothermal event) for a
range of compositions. Further, this isothermal endothermic peak is
expected to be followed by a broad tailing that retraces the base line
at liquidus temperature for each composition. The absence of such
a DTA pattern with isothermal peak indicates the CaBr –CaCl sys-
The minimum in the liquidus curve shown in Fig. 6 is at
56.5 mol% CaBr2 and at 971 K where it would meet the solidus
curve. It is noted here that the DTA curves of samples of this
system showed a width of 6 and 4 K even for the endothermic
2
2
tem does not exhibit a simple eutectic reaction. On the other hand
the observation of a monotonic variation of onset temperature of
endothermic peaks with change in composition indicates that the
components of the system exhibit mutual and complete solid solu-
bility at high temperatures if not from room temperature onwards.
The solid solution region is essentially a single-phase region and
the degree of freedom in this region is two. This means that both
temperature and composition can be changed in this region with-
out appearance of another phase. On heating a solid solution of a
known composition, liquid phase appears at a temperature which
is characteristic of that composition and falls on the solidus curve
as the degree of freedom is one. On further heating, more of liquid is
formed due to preferential dissolution of either CaCl or CaBr solid
peaks of the melting of pure CaCl2 and CaBr , respectively. Hence
2
at compositions near the minimum of liquidus temperatures, the
experimentally measured liquidus points are found to be outside
the liquidus curve shown as dotted line. Further, on decreasing
sample size to ∼4 mg the width did not come down both for the
pure compounds and compositions. The fact that the liquidus curve
shows a minimum at 56.5 mol% CaBr2 instead of a continuous
monotonic increase from pure CaBr2 to pure CaCl , indicates that
2
this system may exhibit a region where two limited solid solu-
tions co-exist, probably at lower temperatures. Evidence of this
possibility could not be obtained from the DTA results as DTA
curves of all the compositions showed a single endothermic peak
between 298 and 1073 K. Also, XRD results obtained for 100% CaBr2,
100% CaCl2 and for the phases obtained after long-term equilibra-
tion of compositions 90, 75, 60, 45, 30 and 15 mol% CaBr2 at 923
and 673 K, qualitatively agreed with the DTA results. The samples
are moisture sensitive in nature and the equilibrated phases were
taken in Lindemann capillary tubes and sealed gas tight with wax
inside argon glove box. Due to the small sample size, the XRD
pattern obtained could be used only to characterize the phases
as the signal to noise ratio of many XRD peaks are moderate. It
could be seen from Figs. 4 and 5 that the XRD pattern is nearly
the same for different compositions and only shifting of major
XRD peaks are observed with compositional change. From the X-
ray data of the most intense peak obtained for 1 1 1 plane, which
showed high signal to noise ratio, we calculated the d111 values
and are given in Table 2. These values are plotted against com-
position of CaBr2 in Fig. 7 and the fitted curve is found to vary
2
2
into the liquid phase. The two-phase region would end ultimately
at the liquidus temperature when the solid phase completely dis-
appears. From all these observations made on DTA results, phase
diagram ofCaBr –CaCl system is constructedandis shownin Fig. 6.
2
2
linearly from pure CaCl2 to pure CaBr . The fact that both phases
2
CaCl2 and CaBr2 belong to the same crystal structure namely,
−
−
orthorhombic and the ionic radii of Cl and Br are very close
1.81 and 1.96 Å, respectively [12]), satisfy the condition needed
(
for complete solid solution formation of these two phases. Fig. 7
indicates that when the bulkier bromide ions substitute for the
smaller chloride ions with increasing composition of CaBr , the
2
lattice probably experiences isotropic expansion. More detailed
analysis of X-ray data is not possible with these X-ray data and
Fig. 5. XRD pattern of samples equilibrated at 673 K.