G. Zhong et al. / Journal of Alloys and Compounds 492 (2010) 482–487
485
ꢀ
ꢀ
from C0 to C0 , boundary layer thickness decreased from Xb to Xb
.
The degree of constitutional undercooling also decreased as shown
in Fig. 4 that the constitutional undercooling zone reduced from
the area surrounded by curve T –TL and straight line GL to that
i
ꢀ
ꢀ
ꢀ
surrounded by curve T –TL and straight line GL . All of these are
i
because of the lower level of solute concentration in solidifica-
tion front, which caused by the acoustic streaming and micro-flow
stirring in the melt.
Strong convection caused in the melt for the introduction of USV
◦
at about 715 C, homogenized the solute distribution field and the
temperature field of the melt. When the USV finished, the melt
◦
temperature was about 690 C, and the semi-solid slurry with some
pre-formed phases was obtained. The start-freezing temperature of

phase decreased in subsequent solidification process, for lower
concentration degree of Fe atoms in the melt with USV. Moreover,
◦
−1
a cooling rate about 10 C s higher than that of traditional casting
could be obtained because the forming temperature of semi-solid
◦
processing was about 130 C lower than that of traditional cast-
ing. As a result, the start-freezing temperature of  phase further
declined due to the higher cooling rate. Therefore, Fe-containing
intermetallic compounds of the alloy with USV continue to form in
the form of ␦ phase rather than acicular  phase.
The longer time USV imposing on the melt, the more uniform
solute distribution, and the more difficult to form acicular  phase
in the solidification process. As can be seen from Fig. 3, the needle-
like  phases decreased remarkably (Fig. 3b) and a large number of
block ␦ phases emerged in the matrix with the application of USV.
The  phases kept on decreasing with the increasing time of USV,
and there were only a small amount of  phases with USV treat-
ment for 180 s (Fig. 3d). It can also be seen from Fig. 3, with USV
time prolonged, the block ␦ phase, which was larger than 100 m
without USV as shown in Fig. 1, was refined to about 40–60 m
with the effect of USV for 60 s (Fig. 3b), and further refined to about
30 m for 120 s (Fig. 3c). But coarse ␦ phase of larger than 50 m
acquired with the effect of USV for 180 s (Fig. 3d). The evenly dis-
tributed fields of temperature and solute of the melt generated by
the effect of acoustic cavitation and acoustic streaming, not only
promoted the formation of ␦ phase, but also inhibited the rapid
growth of ␦ phase in a single direction bringing the refinement
of particles. A part of refined needle-like  phase coexisted with
coarse ␦ phase in the F0 alloy with USV 60 s, due to the influence
of USV was not strong enough. And for 120 s, the effect of USV was
sufficient for restricting the forming of  phase, the finest ␦ phase
and only a small amount of  phase were obtained. Whereas, the
␦ phase grew and coarsened gradually for too long holding time
under the USV for 180 s, though the acicular  phase continued to
decrease for the further homogenous solute distribution.
Fig. 4. Effect of USV on the solute and temperature distributions in front of a crystal.
the plate ␦ phase of F0 alloy without USV. So, the conclusion could
be drawn that the forming of long needle-like  phase was sup-
pressed, which was benefit to the formation of ␦ phase with the
effect of USV on the alloy F0.
In the solidification process of this alloy, Fe atoms aggregate in
the solidification front due to the large difference of solubility of Fe
between liquid and solid Al, even a small amount of Fe in the alloy
will cause harmful acicular  phase to form. It was verified [16]
that the start-freezing temperature of  phase was variable, which
decreased with decreasing iron content, increasing cooling rate,
and increasing melt superheat temperature until it merges with the
temperature of Al–Si eutectic reaction eventually. Among which,
the Fe content has the greatest impact on the start-freezing tem-
perature of  phase, which ascends sharply with the increasing iron
content. And longer growth time is obtained because of enlarged
forming temperature range, causing much coarser  phase. The
same result could be observed through simulation of the  phase’s
start-freezing temperature of the alloys Al–20Si–xFe (x = 1, 2, 5)
◦
using JMatPro software, and the simulated results are 587.7 C,
◦
◦
6
21 C, 670 C respectively.
3.3. Combined effects of ultrasonic vibration and Mn addition on
the Fe-containing intermetallic compounds of high silicon
aluminum alloy with 2% Fe
Acoustic cavitation and streaming whose velocity is about
3
1
0–10 times of that of the fluid thermal convection, will be
produced by USV imposing on the metal melt [3,10–12,17,18].
A maximum speed of acoustic streaming about 1.37 m/s can be
reached by this device for USV, based on theoretical calculations.
And it plays an important role in homogenizing the solute distri-
bution field and the temperature field of the melt, accelerating the
heat and mass transfer, as well as dispersing the primary nuclei. The
convection which speeds up uniform distribution of melt tempera-
ture, is strengthened by the combination of micro-flows generated
by the broken of cavitation bubbles and macro-flows of molten melt
induced by acoustic streaming. It is favorable to form homogenous
solute distribution field and temperature field in the melt, with
the application of USV on the melt before solidification, namely
near the liquidus temperature. The effects of USV on the solute and
temperature distribution of crystallization front are shown in Fig. 4.
As can be seen, the solute concentration of crystal front decreased
Fig. 5 shows the typical optical microstructures of F1 alloy con-
taining 0.5% Mn with and without USV in as-cast state. As can be
seen from Fig. 5a, that the intermetallic compounds of F1 alloy
without USV were mainly composed of needle-like  phase and
plate compound A (light gray). With the effect of USV for 120 s, the
 phase basically eliminated and a large number of fine particles
(such as the light gray compound B directed by the arrow) emerged
with uniform distribution in the matrix, as shown in Fig. 5b. An
EDS analysis shows that the plate compound A and the particles B
contain the same elements Al, Si, Fe and Mn atoms, and the compo-
sitions contents of A and B are listed in Table 4. Based on the ratio
of compositions, compound A is close to the formula Al (Fe,Mn)Si ,
4
2
and two kinds of compounds with the similar morphologies as B are
close to the formula Al (Fe,Mn)Si2 and Al5(Fe,Mn)Si respectively.
4