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    Materials Science and Engineering A326 (2002) 370381

    Mechanical stir casting of aluminium alloys from the mushy state:

    process, microstructure and mechanical properties

    D. Brabazon, D.J. Browne *, A.J. Carr

    Department of Mechanical Engineering, Uniersity College Dublin, Belfield, Dublin 4, Ireland

    Received 2 April 2001; received in revised form 29 August 2001

    Abstract

    A comprehensive study was carried out to establish the effects of controlled stirring during solidification on the microstructure

    and mechanical properties of aluminium alloys, in comparison to conventionally gravity chill cast material. A novel device

    comprising a grooved reaction bonded silicon nitride rod rotating in a tube-like crucible was used to process aluminium alloys in

    the mushy state. The stir casting device was specially designed to also enable rheometric study of the alloys in this condition. A

    factorial design of experiments was used to determine the effect of the process variables shear rate ( ), shear time (ts), and volume

    fraction solid during shear (fs) on microstructure and both static and dynamic mechanical properties of the stir cast alloy.

    Investigation of the microstructure consisted of computer-aided image analysis of the primary phase morphology. A more

    globular primary phase was achieved at low values of fs, but this was not the optimum morphology for mechanical properties.

    In all cases, improved mechanical properties and reduced porosity were obtained in the stir cast condition in comparison with

    conventional casting and in comparison with previous work on stir casting. Comparison with alloy commercially rheocast via

    electromagnetic stirring, however, showed that the latter had superior mechanical properties. It is proposed that the mechanical

    stir casting process be considered as an alternative to gravity die casting in cases where very simple and thick walled shapes are

    required. 2002 Elsevier Science B.V. All rights reserved.

    Keywords: Stir casting; Aluminium alloys; Image analysis; Microstructure; Mechanical properties; Rheocasting

    www.elsevier.com/locate/msea

    1. Introduction

    In conventional casting processes, liquid metal is

    poured into a mould and solidifies as heat is extracted

    via the mould walls. The morphology of the growing

    solidliquid interface is typically dendritic. The natural

    progression of filling followed by solidification often

    leads to internal structural defects, such as entrained

    oxide or shrinkage porosity, which combine to yield acasting of relatively poor mechanical properties.

    Research at the MIT in the 1970s into the rheology

    of alloys in the mushy state, as reported in [1], generally

    involved use of a rotational viscometer which acted to

    fragment the dendritic solid morphology in a time-de-

    pendent fashion, revealing the thixotropic nature of

    metallic materials in this state. This work inspired three

    decades of subsequent research into the processing and

    properties of alloys in this so-called semi-solid state, the

    results of which are reported at the biennial interna-

    tional conference on the subject [24]. It is beyond the

    scope of this paper to present a comprehensive review

    of the field, but it should be noted that the semi-solid

    processing (SSP) of alloys is utilised in a number of

    manufacturing routes today for high quality aluminium

    and magnesium castings, with reduced levels of castingdefects.

    Over the years, a number of devices have been con-

    structed to either investigate the rheological behaviour

    of semi-solid metals, or to produce billets with a non-

    dendritic microstructure. Rheological characterisation

    has typically been carried out by an active mechanical

    shearing method, normally using augers or impellers

    mounted on a central rotating shaft (e.g. [58]). Elec-

    tromagnetic stirring (EMS), on the other hand, due in

    part to its high production rate, has become the main

    method of producing SSP billet commercially. EMS

    * Corresponding author. Tel: +353-1-716-1901; fax: +353-1-283-

    0534.

    E-mail address: [email protected] (D.J. Browne).

    0921-5093/02/$ - see front matter 2002 Elsevier Science B.V. All rights reserved.

    PII: S 0 9 2 1 - 5 0 9 3 ( 0 1 ) 0 1 8 3 2 - 9

    mailto:[email protected]
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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381 371

    also avoids contact of molten metal with stirrers, and in

    some cases the crucible, and may be easier to imple-

    ment for high temperature alloys [912].

    A more recently developed method of SSP has been

    termed liquidus casting or the New RheoCasting pro-

    cess (NRC) [1315]. This involves pouring the alloy

    with a low superheat into a chilling environment to

    nucleate many small grains. Once held for a short

    period of time at semi-solid forming temperature these

    grains ripen and develop a non-dendritic morphology.

    NRC is beginning to be used commercially for slurry

    on demand SSP whereby the production of non-den-

    dritic alloy and subsequent forming via die casting are

    integrated into one operation.

    For the commercial production of industrial compo-

    nents via the SSP route, the final step is often that of

    high pressure die casting of mushy alloy with non-den-

    dritic or globular morphology; a process known as

    thixocasting. And the process by which the requisite

    starting globular structure is attained has become

    known as rheocasting.The thixocasting step produces near net shape prod-

    ucts, and adds significant value to the alloy. For these

    reasons there have been many studies of the effects of

    thixocasting process variables on microstructure and

    properties of the product. There have also been studies

    carried out on the mechanical properties of rheocast

    materials, but these have not been comprehensive. To

    the knowledge of the authors, there has been no de-

    tailed quantitative study on the effects of rheocasting

    variables on the microstructure and both static and

    dynamic mechanical properties of the rheocast material.

    This was an oversight, because it is possible that suffi-cient improvements in quality and mechanical proper-

    ties of alloys could be produced via rheocasting such

    that, in certain cases, the additional cost of thixocasting

    would not be justified. For example, in cases where thin

    walls and fine detail are not a feature of a part,

    rheocasting could be considered as an alternative to

    gravity die casting. For this reason, in addition to

    scientific interest, such a study was undertaken by the

    authors.

    It was decided that use of mechanical stirring was the

    most direct and cost effective way of altering shear rate,

    and because of this, in addition to enabling rheometry,a mechanical rheocaster was designed and built. The

    design brief was to produce materials with a range of

    microstructures, from fully dendritic to fully globular.

    At this point a note on terminology is appropriate. The

    most common SSP route today is rheocasting to pro-

    duce a solid billet, and later reheat of this billet fol-

    lowed by thixocasting. However, in cases where there is

    no intermediate billet solidification stage, the process of

    die casting a rheocast slurry has also been referred to as

    rheocasting [1]. As the current work is not directly

    concerned with the production of feedstock for thixo-

    casting, and also to avoid confusion with the latter

    definition of rheocasting, stir casting [16] has been

    adopted to describe the current process. The principal

    interest here is the difference between conventional

    gravity die casting and the casting of sheared semi-solid

    alloy into a metal mould.

    The distinguishing features of the new mechanical

    stir caster were to include:

    1. a capability for semi-continuous stir casting of alu-

    minium alloys;

    2. top feeding with liquid, and semi-solid poured in a

    continuous laminar stream from the bottom;

    3. a well-defined shear zone in which process parame-

    ters could be closely controlled;

    4. shear zone design to avoid porosity-inducing vortex

    formation;

    5. dual purpose i.e. to act also as a rheometer;

    6. use of unique rotor and crucible materials to enable

    continuous clean operation.

    Some of these features are shared with other devices,

    but this stir caster is unique in its design and in that ithas allof these attributes. The authors have established

    that at least 30 mechanical stirring systems have been

    constructed over the past three decades, and it is practi-

    cal to cite only some examples here. The devices have

    been used either for rheological [58] or stircasting

    [1618] investigations, but rarely for both. Most previ-

    ous systems are also much smaller than the one pre-

    sented here.

    This study involved a Taguchi designed test pro-

    gramme to reveal microstructural features and deter-

    mine mechanical properties, including toughness and

    fatigue performance, of stir cast materials, in compari-son to conventionally cast material. In this way, the

    properties of the processed alloys could be related to

    the microstructure, and conclusions drawn regarding

    not only optimum microstructures, but also optimum

    processing conditions. Image analysis techniques were

    used to supply quantitative data on the microstructure.

    This follows the previous work on microstructural

    characterisation of EMS [19] and mechanically [20]

    rheocast alloys.

    2. Experimental

    2.1. Stir caster design

    A mechanical stir caster/rheometer as illustrated in

    Fig. 1, was designed and built to produce the various

    cast morphologies. The semi-solid alloy was sheared in

    a heated tubular zone between a grooved rotor and a

    crucible. An independent in-line torque meter was posi-

    tioned between the stirring rotor and the drive motor to

    enable rheological measurements. The caster furnace

    was heated by means of four resistance heating ele-

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381372

    ments. One element around the wide reservoir at the

    top of the crucible and three along the lower narrow

    section were used to control the temperature in the

    semi-solid range of the alloy. This configuration en-

    abled a maximum temperature of 850 C and control

    of the temperature gradient within the narrow section

    of the crucible, where the shearing occurred. A linear

    drive provided lift to the rotor, enabling evacuation of

    the stir caster after the desired period of shear. Duringshear, with the rotor in the lower position, the device

    also acted as a rheometer.

    The rotor and crucible (Fig. 2) were both, uniquely,

    of Reaction Bonded Silicon Nitride (RSBN), which

    enabled these two parts to be easily lapped together

    during operation of the stir caster. RBSN has good

    thermal shock resistance, good high temperature

    strength, does not contaminate the melt, and has a low

    coefficient of thermal expansion and moment of inertia.

    An additional external immersion heating element

    was needed in the reservoir to provide sufficient molten

    alloy there for an adequate metallostatic head for stir

    casting at higher fractions solid. A batch casting trolley,

    which also held a plug against the crucible outlet, was

    used to carry the chill moulds into which the stir cast

    material poured. Control of stirring speed, stirring time,

    stirrer height, and the temperature profile of the fur-

    nace, was implemented on a PC by means of LABVIEW

    control software, and data input and output control

    boards. The software also displayed and logged the

    stirring speed, height of the stirrer, temperatures in the

    furnace, and the torque experienced by the stirrer, on a

    real time basis. Apparent viscosity, shear rate, and

    shear stress were also calculated and logged against

    time by the program. Detailed design, construction and

    operation of this stir caster have been previously de-

    scribed [21].

    2.2. Operation of the stir caster

    When setting up the stir caster before an experiment

    the rotor was first lowered into the crucible, Fig. 1. Its

    height was accurately adjusted to form a partial seal at

    the exit such that it was held concentrically duringstirring. Only a partial sealing of the outlet was allowed

    to ensure that torque pick-up from the rotor-crucible

    interaction was negligible. An external plug attached to

    the batch casting trolley provided a full seal at the exit.

    After the caster set-up, metal melted in an induction

    furnace was transferred to a resistance holding furnace

    where it was stabilised at a temperature 20 C above

    the liquidus temperature. The melt was then poured

    into the stir caster furnace which had been preheated to

    570 C for A356 and to 595 C for Al4%Si. Once the

    temperature of the semi-solid melt (Tss) was stabilised,

    giving the desired fs, via the element controllers, rota-tion of the stirrer was started. After shearing the alloy

    at the specified shear rate and for the specified length of

    time, the rotor was raised, the plug on the batch casting

    trolley was released and the alloy allowed to flow into

    a 35 mm diameter cylindrical steel mould, of height

    90 mm.

    Conventional gravity chill castings, poured from

    20 C above the liquidus, were also made in these

    moulds, for comparison purposes.

    The resultant bars were examined radiographically.

    Quality indicator wire showed that a resolution of

    about 0.1 mm could be obtained from the procedure.

    2.3. Thermal analysis

    The slope of the Tssfs curves close to the eutectic

    temperature affects fs control. With too small an abso-

    lute slope here, accurate fs control becomes difficult

    [17]. The upper limit of fs at which stir casting is

    possible depends on the stir casting device. For exam-

    ple, local solidification may occur due to a lack of

    accurate temperature control, or insufficient motor

    torque may be available to stir the more solid structure.

    Fig. 1. Schematic of stir casting device.

    Fig. 2. RBSN ceramic crucible reservoir and rotor.

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381 373

    Table 1

    Chemical composition of A356 and Al4%Si alloys (in wt.%)

    Si Cu Mg Fe Mn Ti Ni Zn Pb Sn Al

    7.14A356 0.1 0.4 0.31 0.12 0.14 0.013 0.056 0.07 0.007 Bal

    0.004 0.01 0.173 0.005 0.007 0.0054.02 0.013Al4%Si 0.004 0.006 Bal

    Table 2

    Stir casting parameters used for producing test bars

    (s1) fsMaterial Ts ( C)Material type ts (s)

    1 Al4Si chill cast

    54.93 0.36Al4Si stir cast 6302 60

    112.843 0.36Al4Si stir cast 630 60

    A356 chill cast 4

    54.93 0.35 601A356 stir cast 60

    112.84 0.3A356 stir cast 6016 60

    7 54.93A356 stir cast 0.3 601 300

    112.84 0.3A356 stir cast 6018 300

    54.93 0.259 605A356 stir cast 60

    112.84 0.25A356 stir cast 60510 60

    54.93 0.25 605 30011 A356 stir cast112.84 0.25A356 stir cast 60512 300

    13 EMS rheocast

    Higher fractions solid may be stir cast by using a

    relatively large liquid metal head, to provide a pressure

    on the semi-solid material during stir casting, and/or by

    keeping the caster exit well insulated to avoid local

    solidification. The Tssfs relationship and coherency

    points for the alloys under investigation, A356 and

    Al4%Si, were determined using thermal analysis fol-

    lowing the methodology of Backerud et al. [22]. Such

    thermal analysis of A356 has been carried out previ-

    ously [22,23] but at faster cooling rates. A slow cooling

    rate of 0.06 C s1 (the slope of the cooling curve after

    solidification) was used in this work in order to match

    the stabilised temperatures in the experiments. The

    chemical compositions of the alloys used are shown in

    Table 1.

    2.4. Design of experiments

    Process parameters used for the stir casting experi-

    ments may be seen in Table 2. Those listed for A356follow a Taguchi factorial design [24] with three factors

    (, fs, ts) and two levels (23). Conventional chill cast

    specimens (materials 1 and 4), poured from 20 C

    above the liquidus temperatures, were tested and the

    results compared with those obtained for the stir cast-

    ings. An upper fraction solid of 0.3 was used for A356

    to ensure fluid castings and a lower fraction solid of

    0.25 was used to ensure that the alloy was above the

    coherency point (the fraction solid at which equiaxed

    dendritic grains start to impinge upon one another

    under normal solidification conditions). The levels of

    shear rate were chosen with the lower value about half

    of the upper one. Previous work (e.g. [8,25]) has shown

    that particle size diminishes early on during shear due

    to morphological disintegration, but begins to increase

    at extended shear times due to primary phase coarsen-

    ing and coalescence. In order to avoid the latter effect,

    shear times were restricted to 5 min. Material 13 is

    commercial EMS rheocast A356 alloy from a European

    supplier.

    2.5. Metallography and image analysis

    Samples cut from the stir cast bars were prepared for

    metallographic examination. A final hand polish was

    performed on Selvyt cloth with Brasso metal polish

    [26]. This final polishing stage also served to etch the

    Al4%Si microstructure. A356 was etched with Kellers

    reagent.

    Particle size, distribution, and shape were investi-

    gated by image analysis techniques. Analysis was per-formed on a PC using the IMAGETOOL program

    (developed at the University of Texas Health Science

    Centre, San Antonio). The primary phase particles and

    agglomerates that do not connect with neighbouring

    primary phase were analysed as isolated particles [27].

    The equivalent average diameter (D) of the isolated

    particles was calculated from their average area (A)

    according to Eq. (1):

    D=4A

    1/2(1)

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381374

    The frequency of occurrence of these particles within

    various size ranges was also computed. The number of

    isolated particles per square millimetre was calculated

    for all the material types. An edge detect image process-

    ing filter was used to approximate the total number of

    primary particles. This included all particles within

    agglomerates or rosettes that were only lightly attached

    to their neighbouring primary phase particles. Dividing

    this by the number of isolated particles detected pro-

    vided a means of approximating the average number of

    particles within an agglomerate. The form factor (F)

    and aspect ratio (R) were calculated for the isolated

    particles (including agglomerates) according to Eq. (2)

    and Eq. (3), respectively, in which P represents the

    particle perimeter,Ljis the length of the major axis, and

    Ln is the length of the minor one.

    F=4A

    P2

    (2)

    R=

    Lj

    Ln (3)

    F has a value between zero and one. A value of one

    represents a perfectly circular particle morphology. As

    this value decreases from one the particle morphology

    becomes less circular. So the form factor can also be

    regarded as sphericity or roundness. A circular mor-

    phology yields a value of one forR, but as the morphol-

    ogy of the particles becomes more elongated the value

    of the aspect ratio increases.

    The microstructure of the eutectic phase in the A356

    samples was also studied by optical microscopy.

    2.6. Mechanical testing

    A minimum of three castings was performed for each

    set of experimental parameters. Four tensile, fatigue, or

    Charpy samples could be produced from each cast bar.

    Where possible, specimens for a given test were taken

    from different stir castings. Tensile, hardness, and

    toughness tests were also performed on commercial

    rheocast EMS A356 billet (64 mm diameter) for com-

    parison with the mechanically stir cast material. A

    minimum of three results was obtained for each prop-erty reading.

    2.6.1. Tensile, hardness and fatigue testing

    Tensile tests were conducted according to ASTM

    B577M for tension testing of cast aluminium alloys. A

    Mitutoyo AVK-C2 hardness tester with a 10 N load was

    used to obtain Vickers hardness values for the castings

    in accordance with BS 427 Part 1. A Wohler fatigue

    machine was used to perform the fatigue tests. These

    were performed at a constant speed of 53 Hz, in

    accordance with ISO 1143 and BS 3518 Part 2.

    2.6.2. Toughness testing

    Plane strain fracture toughness tests were carried out

    on the commercially produced A356 EMS rheocast

    billet. A more detailed discussion of the testing proce-

    dure used has been described previously [28].

    Charpy V-notch (Type A), keyhole (Type B) and

    powder metallurgy type (PM) test pieces were made

    from the cast materials, and tested according to ASTM

    standard E23. Standard dimensions (101055 mm)

    were used for all Charpy specimens. Type A samples

    had a centrally located 2 mm deep 45notch with a root

    radius of 0.1 mm. Type B specimens contained a

    through 2 mm hole centrally located in the specimen

    with a through thickness narrow slot leading to it from

    the specimen surface. PM specimens contained no stress

    raiser.

    2.7. Porosity assessment

    Comparisons between porosity levels for chill cast

    and stir cast material were made from density measure-ments using Archimedes principle. Porosity levels, be-

    ing too low for assessment using ISO 10040:1992, were

    also evaluated by microscopic examination (15) on a

    subjective scale, with 10 indicating the most sound

    sample and 1 indicating a sample with relatiely high

    levels of porosity.

    2.8. Analysis methodsdesign of experiments

    Due to the factorial design of the A356 stir casting

    experiments the results could be examined in detail for

    their dependency on the stir casting parameters [24].Average effect graphs were plotted to examine the effect

    of processing parameters on the microstructural features

    and material properties. On these plots the number one

    on the x-axis represents the average effect of a higher

    parameter setting and minus one indicates the average

    effect of a lower parameter setting. The difference

    between these two averages represents what is termed

    the main effect of the parameter on the property.

    3. Results

    3.1. Thermal analysis

    Temperature versus fraction solid graphs, as deter-

    mined for the two alloys, may be seen in Fig. 3.

    Processing should occur between the coherency point

    and the eutectic point in order for the dendritic structure

    to be modified by the shearing action. Using the co-

    herency point determined by the two thermocouple

    method [22], processing temperature ranges of 54 C

    and 37 C for Al4%Si and A356, respectively, were

    found.

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381 375

    3.2. Metallography and image analysis

    Chill and stir cast microstructures for Al4%Si and

    A356 are presented in Fig. 4. A range of dendritic to

    globular microstructures was developed by the chosen

    conditions. The results from the primary phase image

    analysis of the variously produced microstructures are

    shown in Table 3. Stir cast A356, which was not

    chemically modified, had a course coupled eutectic

    structure with acicular Si particles with average length

    of the order of tens of microns. The EMS material,

    which had been modified by Sr additions of about

    0.03%, had a divorced eutectic structure with rounded

    Si particles with average diameter of the order of a few

    microns.

    3.3. Mechanical properties

    Average material property results determined are pre-

    sented in Table 4 and are related to Table 2 by means

    of the material number. Material 13 is EMS alloy froma European supplier. Samples obtained from a different

    supplier had practically identical properties.

    3.3.1. Fatigue

    Chill cast A356 and Al4%Si were initially tested

    with a range of stress amplitudes in order to determine

    those which gave a fatigue life of the order of 1105

    cycles to failure for each alloy. These values were then

    used for the test programme. A356 was seen to have a

    higher fatigue strength during these initial tests. A

    stress amplitude of 134 MPa was determined and used

    for the A356 rotating fatigue tests and 104 MPa for

    Al4%Si.

    3.3.2. Toughness

    Plane strain conditions were not achieved in any of

    the tested specimens of commercially rheocast material.

    Due to the size and ductility of the castings prepared

    in-house, the tests to determine fracture toughness were

    inapplicable. Similar difficulty in obtaining valid tough-

    ness results using such testing methods for a higher

    strength wrought alloy has recently been observed [29].

    The impact toughness of the castings was, therefore,

    evaluated by means of the Charpy test. Details of the

    difficulty in obtaining toughness results and the final

    choice of the Charpy test for the current work have

    been presented earlier [28]. Conventional Type A speci-

    mens were used for Al4%Si toughness determination.

    Values in the range of only 33.5 J were obtained usingthis type of specimen for the A356 samples, indicating

    its lack of toughness compared with Al4%Si. Type B

    specimens did not produce higher toughness values for

    the A356 samples. Un-notched specimens, as specified

    for powder metallurgical materials were, therefore, used

    for the A356 samples in order to obtain sufficiently

    large values. Un-notched Al4%Si samples bent and

    were pushed through the anvil on testing, and so could

    not be used for comparison with A356. Lateral expan-

    sion was also measured on all specimens.

    3.4. Porosity

    X-radiography indicated that the castings were

    sound. Sectioned castings confirmed the results ob-

    served in the developed X-ray films. Estimates of the

    relative soundness of the materials are included in

    Table 4. Density and porosity levels, determined using

    Archimedes principle, for the main material condi-

    tions, are presented in Table 5. A large degree of scatter

    was noticeable in the porosity observations.

    3.5. Summary

    The main effects plots, which relate microstructural

    features to process conditions for A356 are shown in

    Fig. 5. The main effects plots relating mechanical prop-

    erties to process conditions are shown in Fig. 6.

    4. Discussion

    Here the links between the stir casting process vari-

    ables and the resultant microstructure are investigated.

    This is followed by a study of the effects of microstruc-Fig. 3. Temperature vs. fraction solid for (a) A356; and (b) Al 4%Si,

    at a cooling rate, after solidification, of 0.06 C s1.

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381376

    Fig. 4. Microstructures of (a) material 1, chill cast Al4%Si; (b) material 3, Al4%Si stir cast at 112.84 s1, 0.36 fs, for a period of 60 s; (c)

    material 4, chill cast A356; (d) material 5, A356 stir cast at 54.93 s1, 0.3 fs, for a period of 60 s; (e) material 12, A356 stir cast at 112.84 s1,

    0.25 fs, for a period of 300 s; and (f) commercially produced EMS A356.

    ture on the mechanical properties of the specimens.

    This finally enables the identification of the optimum

    process settings to (a) produce a certain type of mi-

    crostructure and (b) to induce good mechanical proper-

    ties in the castings.

    4.1. Structureprocessing relationships

    Here the microstructural features (Table 3) are re-

    lated to the process variables (Table 2). For both

    Al4%Si and A356, with the exception of material 3, a

    smaller primary phase particle size is evident in the stir

    cast materials versus the conventional chill castings

    (Table 3). For Al4%Si, there is an increased particle

    density and a reduced number of particles per agglom-

    erate, both indicating primary phase fragmentation, in

    the stir cast condition. Unexpectedly, there is a higher

    aspect ratio for stir cast material 3 than for the chill

    cast material 1 (compare Fig. 4(b) with (a)), and a

    slightly lower form factor. For A356, the particle den-

    sity and the number of particles per agglomerate seem

    to depend on the fraction solid at which shearing took

    place. For high fs (materials 58) there is an averagereduction in the density in comparison to the chill cast

    material 4, and a relatively high number of particles per

    agglomerate, whereas for low fs the opposite is true

    (materials 912). This would indicate that a greaterdegree of structural fragmentation has occurred in the

    material which has been sheared at a fraction solid of

    0.25 (e.g. compare Fig. 4(e) with (d)). This is supported

    by all the average effects charts of Fig. 5. At low fs the

    average form factor is higher and the aspect ratio

    lower. It should be borne in mind that even under

    conventional conditions primary solid is less dendritic

    at the earlier stages of solidification.

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381 377

    Fig. 4. (Continued)

    Table 3Image analysis results describing particle size and morphology for chill cast and stir cast Al4%Si and A356 alloys

    Average Average number of particlesIsolated particle densityFlagMaterial Form factor Aspect Ratio

    diameter (m) per agglomerate(mm2)

    90 97 4 0.341 1.42CAS

    79 173 2SAS 0.432 1.74

    SAS3 98 130 3 0.32 2.13

    CA34 117 91 2 0.27 1.93

    94 59 6SA3H 0.335 1.99

    88 68 66 0.32SA3H 1.70

    71 97 5SA3H 0.327 1.90

    SA3H8 68 107 4 0.42 1.86

    SA3L9 58 128 3 0.39 1.8760 131 3SA3L 0.3610 2.05

    64 16911 1SA3L 0.36 1.80

    58 128 3SA3L 0.5712 1.39

    EMS13 94 127 4 0.36 1.51

    The material number relates to the processing parameters outlined in Table 2. The Flag code contains summary information about the material;

    CAS, conventional chill cast Al4%Si; SAS, stir cast Al4%Si; CA3, conventional chill cast A356; SA3, stir cast A356, with final letter H, high

    fs; or L, low fs; EMS, commercial electromagnetically stirred material.

    As expected (Fig. 5) the main effects of increasing are to increase sphericity and reduce aspect ratio. This

    trend towards a more globular primary phase agrees

    with the findings of other workers [6,18]. The effect of

    shear time on particle size and density, sphericity and

    aspect ratio, show that experiments were carried out

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    Table 4

    Average material property observations for the given casting conditions

    Material y (MPa)TS (MPa) f (%) Impact energy Lateral expansion Soundness ratingFatigue life Hv (HV10)

    (cycles103)(mm)(J)

    561 10.9135 13.8* 1.3* 107** 42.2 8.1

    50 15.8 15.5* 1.23*152 232**2 43.7 9.4

    1583 60 15.7 32.1* 2.04* 121** 46.7 9.1

    110 2.2 7.0 0.35 224 74.74 3.3178

    130 4.8 12.1 0.48224 1735 81.4 6.3115 4.4 12.6 0.506 129219 91.6 4.7

    115 3.8 10.9 0.40215 6217 83.2 8.9

    2208 118 4.6 7.8 0.36 424 91.3 7.4

    113 4.0 13.8 0.50211 2729 84.8 7.8

    21210 115 4.1 8.5 0.36 383 86.9 8.4

    11 189 116 2.2 11.0 0.40 200 81.5 6.0

    112 2.3 12.0 0.47191 21612 80.4 7.6

    150 12.0 59.0 0.7213 n/a249 161.3 9.0

    *, CVN, other impact energies are CPM; **, stress amplitude of 104 MPa, for other fatigue tests was 134 MPa.

    within a timescale in which increasing fragmentation

    was still occurring.

    In comparison with the commercially electromagneti-cally stirred A356 (Fig. 4(f)), the mechanically stir cast

    alloy has slightly smaller particle size, but a similar

    degree of agglomeration. The materials mechanically

    sheared at low fs have higher sphericity (e.g. Fig. 4(e))

    than the EMS equivalent.

    4.2. Propertystructure relationships

    Here the mechanical properties (Table 4) are related

    to microstructural features (Table 3). For both alloys

    there is an improvement in the mechanical properties ofthe stir cast in comparison to the gravity chill cast

    materials. A possible exception is the fatigue life for

    A356. The stir cast materials are also more sound than

    the chill cast ones. For the A356 experiments the me-

    chanical properties were plotted against the image anal-

    ysis results. No definite trends could be identified,

    making it difficult establish these relationships over the

    domain of experiments investigated. The best that can

    be done is to identify best and worst case mechanical

    properties and compare and contrast their microstruc-

    tural features, as follows. For each of the mechanical

    properties listed for A356 stir cast materials in Table 4,the best (i.e. highest value) and second best, worst

    (lowest) and second worst materials were compared

    with their respective microstructural parameters of

    Table 3. For each mechanical property, if the best two

    materials had values of a microstructural parameter

    both greater or both less than the average value of all

    the results for stir cast A356, then this was noted. Then,

    for that property, the worst two materials were noted.

    Ifboth these had values of a microstructural feature on

    the opposite side of the average to those of the best

    materials, then this was noted as an effect. The effects

    found are as follows. UTS, YS and f are highest for a

    low density of particles and a high degree of agglomer-

    ation, and UTS and f are highest for a high aspectratio. These three effects combine to yield the conclu-

    sion that higher static mechanical properties are

    achieved in materials that have a less fragmented struc-

    ture (e.g. material 5 in Fig. 4(d)). It is more difficult to

    relate toughness and fatigue life to these microstruc-

    tural parameters. However, the only strong trend,

    across all experiments, of interest in the stir cast A356

    is actually between two of the properties in Table

    4fatigue life and soundness (Fig. 7). Although

    soundness is included in Table 4, it could equally be

    considered to be a microstructural featureit is as-

    sessed via examination of a sectioned casting. Unfortu-

    nately, no link between porosity levels and

    microstructural features can be established.

    The EMS A356 had superior mechanical properties,

    most notably f and toughness, to those of the stir cast

    materials. It is thought that this was largely due to an

    optimal microstructure in the eutectic phase [30] and

    slightly lower porosity in the EMS alloy.

    4.3. Propertyprocessing relationships

    As noted in Section 4.2, there is a general improve-ment in mechanical properties and soundness in the stir

    Table 5

    Density and porosity measurements on chill cast stir cast material,

    determined using Archimedes principle

    PorosityDensity (g cm3)

    2.67Al4Si as chill cast Low

    2.68Al4Si stir cast Lowest

    A356 as chill cast 2.65 Highest

    2.66 HighA356 stir cast

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381 379

    Fig. 5. Average effects plots of stir casting parameters on microstructural parameters for A356.

    cast over the conventional chill cast condition, for both

    alloys. The more globular primary solid structure in the

    mushy stir cast material would be more favourable to

    liquid penetration for feeding, in comparison to a more

    tortuous route through dendritic solid in the conven-

    tional process. Also, less shrinkage and associated

    porosity is expected in the stir castings because pouring

    occurs at a temperature below the liquidus.In Section 4.1 it was noted that alloy A356 stirred at

    low fs and for long ts has a high degree of microstruc-

    ture fragmentation. But in Section 4.2 it was noted that

    the static mechanical properties are best for the less

    fragmented structure. By superposition, therefore, it is

    postulated that the material processed at high fsand for

    short ts has better mechanical properties. Due to the

    design of experiments approach, it is possible to link

    the outcomes to the principal variables via the main

    effects plots of Fig. 6. Indeed, Fig. 6(ad) back up the

    casual link made above. A strong relationship between

    microstructural parameters and either toughness or fa-

    tigue life could not be ascertained for the A356 stir

    castings in Section 4.2, and indeed the resultant depen-

    dence on fraction solid is lower for these properties

    (Fig. 6(e and g)).

    Fig. 6(h) shows that fraction solid has a significant

    effect on porosity of the stir cast material, with greater

    porosity at the higher level of fraction solid. This maybe due to a greater degree of air entrapment as the less

    fluid material exits the device. Much lower levels of

    porosity are evident in all stir cast material in compari-

    son to the conventional chill castings (Table 4).

    4.4. Benchmarking of mechanical properties

    Considerable improvement in mechanical properties

    of stir cast A356 has been observed over the gravity

    chill cast condition. Material 4 in this work has very

    similar properties to those reported in the literature for

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381380

    permanent mould cast A356 [31]. Material 13 also has

    very similar mechanical properties to those reported

    elsewhere for commercial EMS rheocast material [32].

    This agreement with other available results serves to

    calibrate and thereby validate all of the present work.

    The stir cast alloy also has UTS and YS values quite

    similar to those reported (e.g.[33]) for as-thixocast ma-

    terial. However, the fvalues for the latter are typically

    higher, usually in excess of 10%.

    5. Conclusions

    A novel stir caster/rheometer has been designed and

    built for processing aluminium alloys in the mushy

    state. In controlled experiments, stir cast A356 alloy

    showed significant improvement in mechanical proper-

    ties and reduced porosity in comparison to conven-

    tional gravity permanent mould (chill) castings. The

    microstructure of conventional and stir cast material

    Fig. 6. Average effects plots of stir casting parameters on measured properties and recorded observations for A356.

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    D. Brabazon et al./Materials Science and Engineering A326 (2002) 370381 381

    Fig. 7. Fatigue life vs. relative soundness index for stir cast A356.

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    has been quantified by computer-aided image analysis.

    It has been shown that static mechanical properties are

    a function of microstructure, which has been success-

    fully related to process variables. In particular, these

    properties are at their maximum for a low degree of

    primary phase structural breakdown, and this occurs athigh fs, low and ts. Materials with a more globular

    primary phase structure have lower mechanical proper-

    ties. Fatigue properties of the stir cast alloy vary in-

    versely with porosity. The mechanical properties of the

    new stir castings are not as good as the same alloy

    commercially rheocast using EMS, but have a very

    similar primary phase morphology. Differences in

    porosity and eutectic phase microstructure could ex-

    plain these differences. The stir cast material also has

    twice the Fe content than is contained in the EMS

    equivalent, and an unmodified coarse/coupled eutectic

    Si. Both of these features promote easy void formationand fracture when the material is stressed. Fe content is

    also known to hinder fluid flow in the mushy state and

    promote microporosity. Careful design of the stir cast-

    ing process, however, yields superior material than that

    produced in other stir casting work, e.g. [25], and static

    mechanical strength equivalent to thixocast material,

    albeit with lower values of elongation and ductility.

    Rheometric experiments are currently being carried

    out by the authors on the alloys stir cast in this work.

    Acknowledgements

    The authors wish to thank Materials Ireland for

    funding this work. The authors would also like to

    thank Nick Lumsden for his technical assistance in the

    Solidification Laboratory.

    References

    [1] M.C. Flemings, Metall. Trans. 22A (1991) 957.