1-s2.0-S0261306914004567-main.pdf

Embed Size (px)

Citation preview

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    1/11

    Technical Report

    Dry sliding wear behavior of heat treated hybrid metal matrix composite

    using Taguchi techniques

    T.S. Kiran a,⇑, M. Prasanna Kumar b, S. Basavarajappa c, B.M. Viswanatha a

    a Department of Mechanical Engineering, Kalpataru Institute of Technology, BH Road, NH 206, Tiptur 572201, Karnataka, Indiab Department of Industrial Automation Engineering, PG Center, Visvesvaraya Technological University, Mysore, Indiac Department of Studies in Mechanical Engineering, University BDT College of Engineering, Davangere 577004, India

    a r t i c l e i n f o

     Article history:

    Received 9 February 2014

    Accepted 3 June 2014

    Available online 17 June 2014

    a b s t r a c t

    Dry sliding wear behavior of zinc based alloy and composite reinforced with SiCp (9 wt%) and Gr (3 wt%)

    fabricated by stir casting method was investigated. Heat treatment (HT) and aging of the specimen were

    carried out, followed by water quenching. Wear behavior was evaluated using pin on disc apparatus.

    Taguchi technique was used to estimate the parameters affecting the wear significantly. The effect of 

    HT was that it reduced the microcracks, residual stresses and improved the distribution of microconstit-

    uents. The influence of various parameters like applied load, sliding speed and sliding distance on wear

    behavior was investigated by means and analysis of variance (ANOVA). Further, correlation between the

    parameters was determined by multiple linear regression equation for each response. It was observed

    that the applied load significantly influenced the wear volume loss (WVL), followed by sliding speed

    implying that increase in either applied load or sliding speed increases the WVL. Whereas for composites,

    sliding distance showed a negative influence on wear indicating that increase in sliding distance reduces

    WVL due to the presence of reinforcements. The wear mechanism of the worn out specimen was

    analyzed using scanning electron microscopy. The analysis shows that the formation and retention of 

    ceramic mixed mechanical layer (CMML) plays a major role in the dry sliding wear resistance.

      2014 Elsevier Ltd. All rights reserved.

    1. Introduction

    Life of machine component is an important design consider-

    ation. Various parameters affect the life of components and the

    selection of material directly influences the life significantly.

    The choice of material for a particular application varies depend-

    ing on the variables like cost, density, specific strength, modulus

    and operating condition. The majority of engine components,

    gear drives and so on in automotive and aerospace industries uti-

    lizes metals and alloys. The sliding and rotating components

    intended to work in lubricating conditions may eventually endup working in semi-lubricated or dry conditions. This will result

    in higher operating temperature with increase in wear and lead

    to quicker replacement of components. Hence, wear is one of 

    the major problems that need to be tackled in order to improve

    the life of the component. Composite materials are the promising

    alternate for alloys, specifically in dry operating conditions.

    Current work concentrates on the development of a hybrid

    reinforced composite material that can improve the wear resis-

    tance in components. Historically addition of reinforcements

    has shown significant improvement in tribological properties.

    However in some instances it has shown deterioration in

    mechanical properties.

    Zinc–Aluminum (ZA) alloy is a competitive bearing alloy that

    shows improvement in both mechanical and tribological proper-

    ties compared with phosphor-bronze, SAE 73, SAE 660 and cast

    iron. The density of the latter are much higher compared with

    the former element  [1,2]. ZA alloy exhibits superior wear resis-

    tance at low speed-high load application even in the absence of lubricant, while there is a decline in wear resistance with increase

    in speed and rise in temperature  [3,4]. Seah et al.   [5]  and Babic

    et al. [6] performed dry sliding wear behavior of ZA-27 alloy rein-

    forced with Gr particles. These composite specimens exhibited

    enhanced wear resistance than the alloy. The smeared Gr particles

    formed a protective layer on the specimen. Applied load was

    directly proportional to the wear rate for both alloy and composite

    specimen  [5,6], while variation in sliding speed showed contrast

    results in composite specimen   [6]. The hardness decreased with

    the addition of graphite [5,6] as it is a soft inclusion.

    Reinforcing hard SiCp into soft aluminum alloy improves the

    wear resistance as well as hardness of the composite material

    http://dx.doi.org/10.1016/j.matdes.2014.06.007

    0261-3069/  2014 Elsevier Ltd. All rights reserved.

    ⇑ Corresponding author. Address: #133, Coronation Road, Tiptur 572201,

    Karnataka, India. Tel.: +91 8134 252717, mobile: +91 98441 13298.

    E-mail addresses:   [email protected],   [email protected]

    (T.S. Kiran).

    Materials and Design 63 (2014) 294–304

    Contents lists available at  ScienceDirect

    Materials and Design

    j o u r n a l h o m e p a g e :   w w w . e l s e v i e r . c o m / l o c a t e / m a t d e s

    http://dx.doi.org/10.1016/j.matdes.2014.06.007mailto:[email protected]:[email protected]://dx.doi.org/10.1016/j.matdes.2014.06.007http://www.sciencedirect.com/science/journal/02613069http://www.elsevier.com/locate/matdeshttp://www.elsevier.com/locate/matdeshttp://www.sciencedirect.com/science/journal/02613069http://dx.doi.org/10.1016/j.matdes.2014.06.007mailto:[email protected]:[email protected]://dx.doi.org/10.1016/j.matdes.2014.06.007http://crossmark.crossref.org/dialog/?doi=10.1016/j.matdes.2014.06.007&domain=pdf

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    2/11

    [7–10]. Composites with increased volume fraction and larger rein-

    forcement size increase the wear resistance. Particle pull out and

    fracture was the mechanism observed for smaller and larger rein-

    forcement size respectively [7]. A step by step increase in applied

    load increased the wear rate, whereas a contrast result was

    achieved in case of sliding speed by where the wear rate decreased

    with increase in speed [8]. The increase in SiCp content improved

    the hardness which reduced the wear rate significantly. Compos-

    ites reinforced with SiCp exhibited superior wear resistance over

    the alloy as fractured particles ensured the participation in wear

    behavior avoiding the exposure of alloy   [9]. Wilson and Alpas

    [10]  showed that incorporation of SiCp in Al alloy improves the

    mild wear regime at higher load and speed compared to the unre-

    inforced alloy. Prasanna kumar et al. [11] and Ranganath et al. [12]

    evaluated the dry sliding wear behavior of ZA-27/garnet composite

    and concluded that, increasing garnet content improved the wear

    resistance. Meanwhile the wear resistance dropped with an

    increase in applied load and sliding speed.

    Inclusion of only graphite as reinforcement improved wear

    behavior (as it is a solid lubricant), reducing hardness  [5,6]  (soft

    inclusion) while SiCp inclusion showed improvement in both wear

    and hardness [7–10]. The attempt to obtain the combined effect of 

    solid lubrication and improved hardness attributed to the creation

    of hybrid composites. The effect of sliding speed in deciding the

    wear behavior of hybrid composites was evaluated by Basavarajap-

    pa et al.   [13]. It was witnessed that, the specimen experienced

    higher wear rate followed by seizure behavior at higher speeds

    for alloy, while there was a minor effect of increase in speed for

    hybrid composite reinforced with SiCp and Gr. On the contrary,

    Suresha and Sridhara   [14,15]  evaluated that as sliding speed was

    increased, wear loss was reduced for different combinations of 

    SiCp and Gr. Hardness reduces with inclusion of Gr particles in

    Al-SiCp composite specimen.

    Basavarajappa et al.   [16]   used Taguchi’s technique to identify

    the influence of wear parameters and concluded that sliding

    distance is the major contributor followed by applied load and

    sliding speed. Graphite plays an important role in the formationof mechanical mixed layer (MML). Several researchers’   [17–19]

    studied the heat treated ZA-27 alloy followed by water quenching

    to investigate the hardness, tensile and wear behavior. Heat

    treatment to ZA-27 alloy improved the distribution of microcon-

    stituents. Heat treatment resulted in reduction of the hardness

    and tensile properties but had a positive effect on the dry sliding

    wear behavior [17–19]. The specimen heat treated for 5 h [18,19]

    and aged for 8 h  [17]   showed superior wear behavior over other

    heat treatment and aging conditions. The addition of solid lubri-

    cant (Gr) with SiC particles in Al alloy proved to be positive on

    the dry sliding wear behavior [20,21]. A detailed study on the for-

    mation of mechanical mixed layer (MML) and its advantages on the

    worn surface of the specimen were presented [22,23]. A statistical

    approach was used to find out the significance of the factors affect-ing the wear behavior of hybrid MMCs  [24–26].

    The previous studies on ZA-27 alloy have concentrated on

    utilization of SiCp and Gr particles separately. The current work

    concentrates on the HT of ZA-27 alloy reinforced with SiCp and

    Gr particles which were not investigated in earlier research works

    to the best of author knowledge. The parameters that influence the

    wear behavior of heat treated ZA-27 alloy and ZA-27/9SiC–3Gr are

    evaluated by Taguchi technique in the present investigation.

    2. Design of experiments (DOE)

    DOE is an important and powerful statistical technique that

    evaluates the effect of multiple parameters simultaneously. Exper-

    iments have to be conducted in a sequence, with a series of steps,so that the process performance is better understood. A certain

    combinations of factors and levels are considered and varied in a

    strategic manner. The results obtained are observed and analyzed,

    to find out the significant factors and preferred levels [27]. The data

    can be acquired in an orderly way by DOE based on Taguchi

    approach. There are three main phases in the Taguchi process: (i)

    the planning phase (ii) the conducting phase and (iii) the analysis

    phase. Among the three listed phases, planning phase is vital

    where the factors and levels are decided. The results obtained from

    experiments are analyzed for better understanding of the influen-

    tial factors.

    3. Experimental procedure

     3.1. Specimen preparation and wear test 

    ZA-27 is identified as the matrix material and the reinforce-

    ments used are 9 wt% of SiCp with 45 lm and 3 wt% of Gr with

    25lm in size. The composite specimen was prepared by stir

    casting method. The ZA-27 alloy was heated above its liquidus

    temperature of 500 C. A aluminite coated stirrer was introduced

    in the molten slurry to homogenize the temperature. The mixture

    of reinforcements were preheated and poured into the rotatingmolten slurry. To improve the wettability of reinforcements,

    1 wt% of magnesium was added along with the reinforcements.

    The molten slurry was stirred for 10 min, so that the reinforce-

    ments distribute uniformly in the alloy. The melt was later poured

    into permanent castings. The alloy and composite specimen were

    subjected to T6 type of heat treatment in four steps: first, the spec-

    imen were heat treated at 370 C for 5 h; second, the heat treated

    specimen were quenched in water at room temperature; third, the

    quenched specimen were aged at 180 C for 8 h; fourth, the aged

    specimen were quenched in water at room temperature.

    The dry sliding wear behavior of specimen were evaluated with

    pin-on-disc apparatus at room temperature. The specimen were

    machined as per ASTM: G99-05(2010) standards, with a dimension

    of 8 mm diameter and 30 mm height. The specimen was pressed

    against the rotating EN32 steel disc of hardness 65HRc and load

    was applied on the specimen by cantilever mechanism. The disc

    and specimen surface were cleaned with acetone before each

    experiment to remove any traces on the surface. The specimen

    were weighed before and after wear test using an electronic

    weighing machine which can measure up to 0.1 mg. The difference

    in the weight was measured and volume loss was calculated. The

    weight loss of the disc is not considered as the hardness of disc

    was more compared to specimen.

     3.2. Plan of experiments

    Wear tests of the base alloy and composite specimen were

    conducted under dry sliding conditions for three parameters:

    Applied load, sliding speed and sliding distance with variation of 

    3 levels as shown in Table 1. The experiments were planned based

    on standard L27  orthogonal array (OA), consisting of 27 rows and

    13 columns. The 1st, 2nd and 5th columns were assigned to

    applied load (L), sliding distance (D) and sliding speed (S ) respec-

    tively in the Orthogonal Array, while the remaining columns were

    assigned to their interactions. The present investigation is based on

    the objective to study smaller – the-better wear response.

     Table 1

    Process parameters used in the experiment.

    Level Load,  L  (N) Sliding distance,  D  (m) Sliding speed, S  (m/s)

    1 15 1000 0.63

    2 45 3000 1.88

    3 75 5000 3.14

    T.S. Kiran et al./ Materials and Design 63 (2014) 294–304   295

    http://-/?-

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    3/11

    4. Results and discussion

    4.1. Heat treatment 

    As the dendrites dissolve uniformly after HT, the microstructure

    of as-cast specimen is shown in Fig. 1. In as-cast alloy (Fig. 1a), the

    aluminumrich (A)a-phase and zinc rich (B) g-phase can be clearly

    differentiated as white and black regions respectively. The

    eutectoid (C)  a + g  phase is rarely visible which is the vital phase

    for tribological applications [17–19]. The SiC and graphite particles

    are shown in  Fig. 1b. As the Heat treatment was carried out, the

    microstructure was fully transformed into eutectoid phase, giving

    added advantage to both alloy and composite specimen. Themicrocracks and residual stresses present in the as-cast specimen

    were reduced by HT process facilitating improved wear resistance.

    EDX of the base alloy and hybrid composite are shown in  Fig. 1c

    and d respectively, which confirms the presence of reinforcements

    (Fig. 1d). Since, all the specimen considered were heat treated, the

    advantage of HT on as-cast is not discussed in the present work.

    4.2. Hardness

    Vicker hardness test was performed on the heat treated alloy

    and composite specimen. The results showed a slight increase in

    hardness of composite (108 HV) compared with the alloy

    (106 HV). The reason for the slight increase is due to the presence

    of soft Gr particle that hindered the hardness value   [14,15]. Onemore factor that influenced the reduction in hardness value is heat

    treatment [17–19].

    4.3. Wear test 

    The dry sliding wear experiments were conducted as per the OA

    and the results are tabulated as shown in Table 2. For better under-

    standing of the various factors considered  L  (applied load, in  N ), D

    (sliding distance, in m),  S  (sliding speed, in m/s) and their interac-

    tions, it is required to develop an analysis of variance (ANOVA). The

    experimental results were analyzed using commercial software

    MINITAB, which is used in DOE applications. The effects and order

    of significance of the design parameter with their interactions are

    to be studied on the wear behavior. The analysis was carried outfor a confidence level of 1%.

    Fig. 1.  Microstructure of as-cast (a) alloy, (b) composite, (c) EDX of alloy and (d) EDX of hybrid composite.

     Table 2

    Experimental design using  L27 OA.

    Test Load L, (N) Distance D, (m) Speed S , (m/s) Wear volume loss in

    mm3

    Alloy Composite

    1 15 1000 0.63 1.4 0.5

    2 15 1000 1.88 1.6 0.8

    3 15 1000 3.14 2.2 1.2

    4 15 3000 0.63 1.5 0.7

    5 15 3000 1.88 2.4 1.0

    6 15 3000 3.14 3.2 1.6

    7 15 5000 0.63 2.5 0.9

    8 15 5000 1.88 3.3 1.2

    9 15 5000 3.14 4.6 1.810 45 1000 0.63 1.7 0.9

    11 45 1000 1.88 2.3 1.1

    12 45 1000 3.14 2.7 1.5

    13 45 3000 0.63 2.7 1.4

    14 45 3000 1.88 2.7 1.7

    15 45 3000 3.14 4.1 2.1

    16 45 5000 0.63 3.8 1.3

    17 45 5000 1.88 4.6 1.9

    18 45 5000 3.14 6.1 2.6

    19 75 1000 0.63 3.5 1.5

    20 75 1000 1.88 4.6 2.1

    21 75 1000 3.14 6.5 2.8

    22 75 3000 0.63 4.7 1.9

    23 75 3000 1.88 5.9 2.6

    24 75 3000 3.14 7.7 3.2

    25 75 5000 0.63 5.9 2.7

    26 75 5000 1.88 7.9 3.8

    27 75 5000 3.14 9.5 4.1

    296   T.S. Kiran et al. / Materials and Design 63 (2014) 294–304

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    4/11

    Tables 3 and 4  shows the ANOVA results for the WVL of alloy

    and composites respectively. It can be noted from column 7 of 

    Tables 3 and 4   that the p-value is zero for applied load, sliding

    speed and sliding distance, which indicates that these play a major

    role in the wear volume loss and have statistical significance.

    Table 3 shows that applied load ( p = 55.86%) had a great influence

    on wear loss of the alloy, while sliding distance ( p = 21.35%) and

    speed ( p = 15.93%) showed less influence on the WVL. The interac-

    tions (L * S) had a negligible influence ( p = 0.66%) on the WVL,

    while the other two interactions (L * D and  D  * S ) had no effect on

    the wear behavior. It can be observed from  Table 4   that applied

    load ( p = 56.67%) has highest influence followed by sliding distance

    ( p = 19.25%) and speed ( p = 14.22%). The influence of interaction

    (L * D) is negligible ( p = 1.63%) on wear volume loss. Thus load is

    an important factor that controls the WVL of both alloy and com-

    posite materials.

    4.4. Analysis of control factors

    The response table for WVL of alloy and composite is presented

    in Table5, to analyze the influence of the control factors. Analysis of 

    control factors will give the additional important information about

    the nature of the process under consideration. The highest differ-

    ence of control factors indicates the strongest influence on WVL.

    It can be seen from Table 5 that the strongest influence on WVL 

    was applied load, followed by sliding distance and sliding speedrespectively in case of alloy. In case of composite, applied load

    was the most influential factor and sliding speed was the second

    most influential factor followed by sliding distance.   Fig. 2(a and

    b) shows the interaction plot for alloy and composites. Three levels

    (low, medium and high) are considered in the experimentation and

    a straight line can be drawn for second and third column. In the

    first column of  Fig. 2(a and b), there is a sudden increase in the

    slope after 45 N, which shows that increase of applied load will

    affect the wear performance of the specimen (Fig. 2a). The increase

    in sliding distance has positive effect on the composite as the line

    shows a reduction in slope (Fig. 2b), while the alloy (Fig. 2a) shows

    no change in the wear behavior. The reason for the reduction in

    slope of composite specimen is the smearing of reinforcements

    and formation of protective layer inhibiting the WVL. Hence, as

    sliding distance is increased, the wear resistance improves margin-

    ally for composite (Fig. 2b).

    Fig. 3(a and b) shows the main effects plot for means of alloy

    and composite respectively. The rise in slope of lines indicates

    the increase in WVL due to increase in applied load from 45 to

    75 N, which can be analyzed that the wear phenomenon has

    entered severe wear from mild wear.

    4.5. Regression analysis

    To ascertain the correlation between the factors (applied load,

    sliding speed and sliding distance) and responses (volume loss),

    multiple linear regression equations were generated using

    MINITAB software. The regression equations are as follows:

    WearðalloyÞðmm3Þ ¼  0:078þ 0:0266L þ 1:84e4D þ 0:020S 

    þ 0:5e5LD þ 0:0111LS  þ 1:06e4DS 

    ðR-Sq ¼  93:59%   R-SqðadjÞ ¼  91:66%Þ ð1Þ

    WearðCompositeÞðmm3Þ ¼0:137þ0:00987L1:8e5Dþ0:154S 

    þ0:4e5LDþ0:00332LS þ3:3e5DS 

    ðR-Sq¼95:32%   R-SqðadjÞ ¼93:92%Þ ð2Þ

    Eqs. (1) and (2) refers to the linear regression equation for cal-

    culating volume loss by substituting the values of variables of alloyand composite respectively. The positive sign of the co-efficients

     Table 3

    Analysis of variance for alloy.

    Source Degrees of freedom Sum of squares Adjusted sum of squares Adjusted mean of Squares   F -ratio   P -value Percentage (%) of contribution

    L   2 68.019 68.018 34.009 553.16 0.000 55.86

    D   2 26.605 26.605 13.303 216.37 0.000 21.35

    S    2 20.099 20.098 10.049 163.45 0.000 15.93

    L * S    4 2.761 2.761 0.690 11.23 0.002 0.66

    L * D   4 1.128 1.128 0.282 4.59 0.032 –

    D * S    4 0.901 0.901 0.225 3.67 0.056 –Error 8 0.492 0.492 0.061 6.20

    Total 26 120.005 ‘ 100

    S  = 0.620278, R-Sq = 93.6% and R-Sq(adj) = 91.7%.

     Table 4

    Analysis of variance for hybrid composite.

    Source Degrees of freedom Sum of squares Adjusted sum of squares Adjusted mean of Squares   F -ratio   P -value Percentage (%) of contribution

    L   2 13.040 13.040 6.520 397.83 0.000 56.67

    S    2 4.602 4.602 2.301 140.41 0.000 19.25

    D   2 3.469 3.469 1.734 105.83 0.000 14.22

    L * D   4 0.891 0.891 0.223 13.59 0.001 1.63

    L * S    4 0.304 0.304 0.076 4.64 0.031 –

    D * S    4 0.109 0.109 0.027 1.66 0.251 –

    Error 8 0.131 0.131 0.016 8.23Total 26 22.547 100

    S  = 0.229643, R-Sq = 95.3% and R-Sq(adj) = 93.9%.

     Table 5

    Response table for means: smaller is better.

    Level Wear response of alloy Wear response of composite

    L D S L D S  

    1 2.522 2.944 3.078 1.078 1.378 1.311

    2 3.411 3.878 3.922 1.611 1.800 1.800

    3 6.244 5.356 5.178 2.744 2.256 2.322

    Delta 3.722 2.411 2.100 1.667 0.878 1.011

    Rank 1 2 3 1 3 2

    T.S. Kiran et al./ Materials and Design 63 (2014) 294–304   297

    http://-/?-http://-/?-http://-/?-http://-/?-

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    5/11

    refers to increase in the wear volume loss with increase in their

    associated variables. While negative sign indicates that WVL 

    decreases with increase in the associated variables. The negative

    sign in Eq. (2) indicates that as sliding distance is increased, wear

    resistance is increased due to the smearing of reinforcements that

    act as ceramic mixed mechanical layer (CMML). However, the

    effects of interactions are relatively insignificant.

    Fig. 4(a and b) shows the normal probability plot for alloy and

    composite. These probability plots clearly indicates that the

    values lies closer to the normal probability line implying that

    the errors are distributed normally and the model is adequate.

    Thus the model formulated for prediction of volume loss of alloy

    and composite which are represented by Eq.  (1)   and Eq.   (2)   is

    adequate.

    4.6. Response surface analysis

    Response surface methodology (RSM) is a statistical method

    that make use of quantitative data from suitable tests conducted

    to determine and solve multi-variable equations. RSM, which is

    used to analyze the results and surface plots for alloy and compos-

    ites are shown in Figs. 5 and 6 respectively. WVL at any zone from

    the tests conducted can be predicted from the surface plots. From

    Figs. 5 and 6  it is clear that applied load has the most dominant

    effect on WVL for both alloy and composite. The remaining factors,

    sliding distance and sliding speed were less dominant compared to

    load. In Fig. 5, the interactions L * D and L * S  show that the slope of 

    load is more compared to the other two factors, clearly indicating

    that applied load has more effect on the WVL.

    Fig. 2.  Interaction plots for wear volume loss (mm3) of (a) alloy and (b) composites.

    298   T.S. Kiran et al. / Materials and Design 63 (2014) 294–304

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    6/11

    The magnitude of wear volume loss of alloy (Fig. 5), when com-

    pared with composite (Fig. 6) is nearly double, which confirms the

    wear resistance of composites and the presence of reinforcements

    that inhibit the WVL. The smeared and adhered reinforcements actas a medium preventing the specimen from excessive wear.

    4.7. Determination of accuracy of wear volume loss

    For each experiment in the design matrix, the WVL model of 

    Eqs. (1) and (2) were used to calculate the theoretical wear volume

    loss for alloy and composite. The results are summarized in

    Table 6.

    The experimental values were compared with the calculated

    values and the comparison is shown in Fig. 7. It can be noticed that

    the WVL values calculated from the multiple linear regression

    model follows almost the similar trend as that of the experimental

    values. The peaks of the alloy and composites reveal that the exces-

    sive wear was inhibited due to the addition of reinforcements. Theslopes of the alloy are higher while that of composites are lower

    signifying the importance of reinforcements. The variation may

    be due to the irregularities in the experiment like environmental

    condition, machine vibration or human errors.

    4.8. Wear mechanism

    Fig. 8(a and b) and  Fig. 8(c–e) show the worn out surfaces of 

    alloy and composites respectively at a sliding speed of 1.88 m/s,

    sliding distance of 3000 m and at different applied load. The single

    arrow shows the sliding direction of worn surface. It is evident that

    the surface of alloy (Fig. a and b) is rough with deep grooves com-

    pared with the composite specimen (Fig. 8c–e) with fine grooves.

    Fig. 8a and   Fig. 8b shows the worn out surfaces of alloy at an

    applied load of 15 and 75 N respectively. Due to the increase in

    applied load, the morphology shows that the alloy (Fig. 8a and b)

    has experienced severe wear under the absence of reinforcements.

    The composites (Fig. 8c–e) show smooth surface in black region

    (double arrow) due to the presence of graphite that smears outduring sliding and acts as a layer, protecting the specimen from

    Fig. 3.  Main effects plot for means (a) alloy and (b) composite.

    T.S. Kiran et al./ Materials and Design 63 (2014) 294–304   299

    http://-/?-http://-/?-

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    7/11

    direct contact with the disc, thus enhancing wear resistance

    [10,13–16]. The presence of SiCp and Gr are shown in   Figs. 8e

    and 9(a–c). These reinforcements participate in the wear process,

    protecting the specimen from excessive wear.

    During the wear process, the asperity on the surface of the

    rotating steel disc comes in contact with the surface of the speci-

    men (composite). Due to a large difference in the hardness of alloy

    and reinforcement, the asperities in the counterface are pressedinto the specimen and the soft surface of composites is scratched.

    Due to work-hardening of the surface layer of composite, the pro-

     jected Fe asperity may detach from the counterface and adhere on

    the composite surface. Due to severe scratching on the counterface,

    large delamination cavities are formed as a result of fracture of the

    surface material. The debris (Fig. 10) from both (specimen and

    steel disc) materials are pushed down into the cavities and grooves

    of specimen, until it becomes flat as the surrounding surface. The

    formation of debris from the counterface may be by two ways.

    First, the asperities on the surface of counterface break off and

    are pressed against the composite surface during sliding, but are

    obstructed by the surface material of composite. Secondly, the hard

    reinforcements that bear the load on the composite surface will

    certainly scratch heavily the counterface surface. These resultsare in agreement with Basavarajappa et al.  [30].

    Due to friction between the specimen and rotating disc during

    dry sliding, temperature rises leading the specimen to lower its

    mechanical property  [1,2].   Due to rise in temperature, the alloy

    loses its property of bonding with neighboring elements, resulting

    in thin plate like wear debris (Fig. 10a). Even though zinc rich (g)

    phase contributes in wear resistance, it is unable to withstand the

    higher temperature due to higher applied load. The rise in the tem-

    perature was noticeable as the applied load was increased, whichcauses a negative effect on the performance of specimen. As the

    temperature rises, the bonding within the matrix begins to fail,

    leading to severe wear and further changing to delamination with

    further increase in applied load   [25,26,28–30]. For composite

    specimen, the rise in temperature was negligible as the formation

    of protective layer secludedfurther exposureof newlayer inhibiting

    the severe wear at lower load (15 and 45 N). At higher load (75 N),

    the protective layer of composite specimen gradually exposed

    newmaterial that were unableto retain and leading to severe wear.

    In composites, due to rise in temperature, reinforcements gradually

    start separating from the alloy, resulting in the direct exposure to

    the rotating disc. The presence of microcracks (Fig. 8e) on the worn

    out surfaces were observed. The effect of HT is that the residual

    stress and microcrack is greatly reduced which affects the wearbehavior positively   [17–19]. The reinforcements that smear out

    Fig. 4.  Normal probability plot of residuals of WVL (mm3) of (a) alloy and (b) composite.

    300   T.S. Kiran et al. / Materials and Design 63 (2014) 294–304

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    8/11

    during the lower applied load and sliding speed get retained on the

    specimen. As the applied load and sliding speed increases the

    particles projected will brake and act as third body and startsremoving the matrix material. The metal oxides are formed because

    of the rise in temperature, the crushed SiCp particles, the smeared

    graphite along with a matrix material crush between the pin and

    disc forming a ceramic mixed mechanical layer (CMML) preventingthe specimen from excessive wear (Fig. 8e). As the applied load is

    Fig. 5.  Response surface plot for alloy.

    Fig. 6.  Response surface plot for hybrid composite.

    T.S. Kiran et al./ Materials and Design 63 (2014) 294–304   301

    http://-/?-http://-/?-

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    9/11

    increasedfurther, the layer formed will be destroyed at a faster rate

    leading to direct contact between the new surface of specimen and

    disc resulting in higher WVL. The similar results were observed by

    other researchers  [10,21,22,26,30].

    The presence of Fe in  Fig. 9(b and c) clearly shows that, there

    was a formation of CMML on the surface on the specimen. But as

    the applied load increased, there was a progressive increase in

    the WVL. At lower load (15 N), the transfer of the disc material

    onto the specimen surface was observed and the intensity of Fe

    peak was higher experiencing mild wear. As the applied load was

    increased (75 N), CMML formed on the specimen surface was

    eroded. The formation and removal of the CMML at lower applied

    load is slow, hence retaining the protective layer. At higher applied

    load, the removal rate of the protective layer is at a faster rate than

    the layer formation, leading to severe wear   [22]. The study has

     Table 6

    Experimental and calculated values of alloy and composites.

    Test Load L, (N) Distance D, (m) Speed S , (m/s) Wear volume loss in mm3

    Alloy Composite

    Experimental Calculated Experimental Calculated

    1 15 1000 0.63 1.4 0.93 0.5 0.48

    2 15 1000 1.88 1.6 1.29 0.8 0.77

    3 15 1000 3.14 2.2 1.66 1.2 1.074 15 3000 0.63 1.5 1.57 0.7 0.60

    5 15 3000 1.88 2.4 2.21 1.0 0.98

    6 15 3000 3.14 3.2 2.84 1.6 1.36

    7 15 5000 0.63 2.5 2.22 0.9 0.73

    8 15 5000 1.88 3.3 3.12 1.2 1.19

    9 15 5000 3.14 4.6 4.03 1.8 1.65

    10 45 1000 0.63 1.7 2.08 0.9 0.96

    11 45 1000 1.88 2.3 2.86 1.1 1.38

    12 45 1000 3.14 2.7 3.65 1.5 1.80

    13 45 3000 0.63 2.7 3.03 1.4 1.32

    14 45 3000 1.88 2.7 4.08 1.7 1.82

    15 45 3000 3.14 4.1 5.13 2.1 2.33

    16 45 5000 0.63 3.8 3.98 1.3 1.69

    17 45 5000 1.88 4.6 5.29 1.9 2.27

    18 45 5000 3.14 6.1 6.62 2.6 2.86

    19 75 1000 0.63 3.5 3.23 1.5 1.43

    20 75 1000 1.88 4.6 4.43 2.1 1.9821 75 1000 3.14 6.5 5.64 2.8 2.53

    22 75 3000 0.63 4.7 4.48 1.9 2.04

    23 75 3000 1.88 5.9 5.95 2.6 2.67

    24 75 3000 3.14 7.7 7.42 3.2 3.30

    25 75 5000 0.63 5.9 5.73 2.7 2.65

    26 75 5000 1.88 7.9 7.46 3.8 3.36

    27 75 5000 3.14 9.5 9.21 4.1 4.07

    Fig. 7.  Experimental and calculated values of alloy and composites.

    Fig. 8.  SEM of worn surfaces of Alloy (a) 15 N, (b) 75 N, hybrid composite (c) 15 N, (d) 45 N and (e) 75 N.

    302   T.S. Kiran et al. / Materials and Design 63 (2014) 294–304

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    10/11

    clearly indicated the instability and the consequent removal of 

    CMML resulting in high WVL and further causing transition frommild to severe wear.

    The wear debris thrown out from the rotating disc is been pre-

    sented in   Fig. 10   which shows the size of wear debris of alloy(Fig. 10a) and composite (Fig. 10b) at applied load of 75 N, sliding

    Fig. 9.  EDX of worn surfaces of hybrid composite at load (a) 15 N, (b) 45 N and (c) 75 N.

    Fig. 10.   Wear debris at 75 N (a) alloy and (b) hybrid composite.

    T.S. Kiran et al./ Materials and Design 63 (2014) 294–304   303

    http://-/?-http://-/?-

  • 8/20/2019 1-s2.0-S0261306914004567-main.pdf

    11/11

    speed of 1.88 m/s and sliding distance of 3000 m. The size of the

    wear debris proves that the extent of wear of alloy (Fig. 10a) expe-

    riencing delamination wear. The mechanical layer formed on the

    alloy surface were incapable of withstanding the higher load

    (75 N) and the layer were detached and thrown away as thin plate

    like particles (Fig. 10a). Whereas for composite specimen, the

    smeared reinforcements were fragmented and crushed between

    the specimen and rotating disc, forming a protective layer. The

    wear debris of composites (Fig. 10b) exhibits mild wear with small

    particles thrown out from the rotating disc. The debris emerged

    out of the alloy measures up to 500 lm (Fig. 10a) and the average

    size of debris are nearly 200 lm. In case of composite specimen,

    the debris measured are below 100 lm   (Fig. 10b). The size of 

    debris explains the extent of wear in alloy (delamination) in

    comparison with the composite specimen.

    5. Conclusions

    The following conclusions were drawn:

    (1) The microconstituents of heat treated materials are well dis-

    tributed and gets dissolved providing wear resistance by the

    zinc rich (g) constituent. The effort to reduce the residual

    stresses is attained by heat treatment. The microcracks pres-

    ent in the as-cast specimen which causes excessive wear are

    reduced by heat treatment resulting in superior wear

    resistance.

    (2) The significant parameters in the wear analysis were found

    from ANOVA. Applied load is the most significant factor fol-

    lowed by sliding distance and sliding speed in causing wear

    in case of the alloy. Similarly the contributions for compos-

    ites are applied load, sliding speed and sliding distance.

    The interactions show negligible contribution for both alloy

    and composite specimen.

    (3) The metal oxides are formed because of the rise in tempera-

    ture, the crushed SiCp particles, the smeared graphite parti-

    cles along with a matrix material crush between the pin and

    disc forming a ceramic mixed mechanical layer (CMML).

    (4) The addition of solid lubricant (Gr) as secondary reinforce-

    ment along with SiCp improves the wear resistance by form-

    ing a CMML on the contact geometry. The formation and

    retention of CMML acts as a protective layer, thereby reduc-

    ing the wear volume loss in case of composites.

    (5) The size of wear debris that emerged out of wear specimen

    demarcated the severity of wear in alloy while fine wear

    debris showed mild wear in composites.

    References

    [1] Murphy S, Savaskan T. Comparative wear behavior of Zn–Al-based alloys in anautomotive engine application. Wear 1984;98:151–61.

    [2] Savaskan T, Murphy S. Mechanical properties and lubricated wear of Zn–25Al-

    based alloys. Wear 1987;116:211–24.

    [3] Pandey JP, Prasad BK. Sliding wear response of a zinc-based alloy compared to

    a copper-based alloy. Metall Mater Trans A 1998;29(April):1245–55.

    [4] Prasad BK, Patwardan AK, Yegneswaran AH. Dry sliding wear characteristics of 

    some zinc–aluminiumalloys: a comparative study witha conventionalbearing

    bronze at a slow speed. Wear 1996;199:142–51.

    [5] Seah KHW, Sharma SC, Girish BM, Lima SC. Wear characteristics of as-cast ZA-

    27/graphite particulate composites. Mater Des 1996;17(2):63–7.

    [6]  Babic M, Slobodan M, Dzunic D, Jeremic B, Ilija B. Tribological behavior of 

    composites based on ZA-27 alloy reinforced with graphite particles. Tribol Lett

    2010:401–10.

    [7] Kumar S, Balasubramanian V. Effect of reinforcement size and volume fraction

    on the abrasive wear behaviour of AA7075 Al/SiCp P/M composites — a

    statistical analysis. Tribiol Int 2010;43(1–2):414–22.

    [8]  Sharma SC, Girish BM, Kamath R, Satish BM. Effect of SiC particle

    reinforcement on the unlubricated sliding wear behaviour of ZA-27 alloy

    composites. Wear 1997;213:33–40.[9] Prasad BK. Investigation into sliding wear performance of zinc-based alloy

    reinforced with SiC particles in dry and lubricated conditions. Wear

    2007;262:262–73.

    [10]   Wilson S, Alpas AT. Wear mechanism maps for metal matrix composites. Wear

    1997;212(1):41–9.

    [11]   Prasanna kumar M, Sadashivappa K, Prabhukumar GP, Basavarajappa S. Dry

    sliding wear behaviour of garnet particles reinforced zinc–aluminium alloy

    metal matrix composites. Mater Sci 2006;12(3):209.

    [12]  Ranganath G, Sharma SC, Krishna M. Dry sliding wear of garnet reinforced

    zinc/aluminium metal matrix composites. Wear 2001;251:1408–13.

    [13]  Basavarajappa S, Chandramohan G, Arjun M, Thanagavelu M, Subramanian R,

    Gopalkrishnan P. Influence of sliding speed on the dry sliding wear behaviour

    and the subsurface deformation on hybrid metal matrix composite. Wear

    2007;262:1007–12.

    [14]   Suresha S, Sridhara BK. Wear characteristics of hybrid aluminium matrix

    composites reinforced with graphite and silicon carbide particulates. Compos

    Sci Technol 2010;70(11):1652–9.

    [15]   Suresha S, Sridhara BK. Effect of silicon carbide particulates on wear resistance

    of graphitic aluminium matrix composites. Mater Des 2010;31(9):4470–7.

    [16]   Basavarajappa S, Chandramohan G, Paulo Davim J. Application of Taguchi

    techniques to study dry sliding wear behaviour of metal matrix composites.

    Mater Des 2007;28:1393–8.

    [17]   Prasad BK. Influence of heat treatment parameters on the lubricated sliding

    wear behaviour of a zinc-based alloy. Wear 2004;257(11):1137–44.

    [18]  Bobic M, Aleksandar V, Slobodan M, Ilija B. Influence of T4 heat treatment on

    tribological behavior of Za27 alloy under lubricated sliding condition. Tribol

    Lett 2009;36:125–34.

    [19]  Bobic M, Mitrovic S, Jeremic B. The influence of heat treatment on the sliding

    wear behavior of a ZA-27 alloy. Tribiol Int 2010;43(1–2):16–21 .

    [20]  Suresha S, Sridhara BK. Effect of addition of graphite particulates on the wear

    behaviour in aluminium–silicon carbide–graphite composites. Mater Des

    2010;31(4):1804–12.

    [21]  Ravindran P, Manisekar K, Narayanasamy R, Narayanasamy P. Tribological

    behaviour of powder metallurgy-processed aluminium hybrid composites

    with the addition of graphite solid lubricant. Ceram Int 2013;39(2):1169–82.

    [22]   Venkatraman B, Sundararajan G. Correlation between the characteristicsof the

    mechanically mixed layer and wear behavior of aluminium, Al-7075 alloy andAl-MMCs. Wear 2000;245:22–38.

    [23]  Alidokht SA, Abdollah-zadeh A, Assadi H. Effect of applied load on the dry

    sliding wear behaviour and the subsurface deformation on hybrid metal

    matrix composite. Wear 2013;305(1–2):291–8.

    [24]   Basavarajappa S, Chandramohan G. Dry sliding wear behavior of metal matrix

    composites: a statistical approach. JMEPEG 2006;15:656–60.

    [25]   Kumar R, Dhiman S. A study of sliding wear behaviors of Al-7075 alloy and Al-

    7075 hybrid composite by response surface methodology analysis. J Mater Des

    2013;50:351–9.

    [26]  Ravindran P, Manisekar K, Narayanasamy P, Selvakumar N, Narayanasamy R.

    Application of factorial techniques to study the wear of Al hybrid composites

    with graphite addition. Mater Des 2012;39:42–54.

    [27]  Ross Phillip J. Taguchi techniques for quality engineering. NewYork: McGraw-

    Hill; 1988.

    [28]   Soleymani S, Alidokht SA. Microstructural and tribological properties of 

    Al5083 based surface hybrid composite produced by friction stir processing.

    Wear 2012;278–279:41–7.

    [29]  Rao RN, Das S, Mondal DP, Dixit G. Effect of heat treatment on the sliding wear

    behaviour of aluminium alloy (Al–Zn–Mg) hard particle composite. Tribiol Int2010;43(1–2):330–9.

    [30]   Basavarajappa S, ChandramohanG, Mukund K, Ashwin M, Prabu M. Dry sliding

    wear behavior of Al 2219/SiCp-Gr hybrid metal matrix composites. JMEP

    2006;15:668–74.

    304   T.S. Kiran et al. / Materials and Design 63 (2014) 294–304

    http://refhub.elsevier.com/S0261-3069(14)00456-7/h0005http://refhub.elsevier.com/S0261-3069(14)00456-7/h0005http://refhub.elsevier.com/S0261-3069(14)00456-7/h0005http://refhub.elsevier.com/S0261-3069(14)00456-7/h0010http://refhub.elsevier.com/S0261-3069(14)00456-7/h0010http://refhub.elsevier.com/S0261-3069(14)00456-7/h0010http://refhub.elsevier.com/S0261-3069(14)00456-7/h0015http://refhub.elsevier.com/S0261-3069(14)00456-7/h0015http://refhub.elsevier.com/S0261-3069(14)00456-7/h0020http://refhub.elsevier.com/S0261-3069(14)00456-7/h0020http://refhub.elsevier.com/S0261-3069(14)00456-7/h0020http://refhub.elsevier.com/S0261-3069(14)00456-7/h0025http://refhub.elsevier.com/S0261-3069(14)00456-7/h0025http://refhub.elsevier.com/S0261-3069(14)00456-7/h0030http://refhub.elsevier.com/S0261-3069(14)00456-7/h0030http://refhub.elsevier.com/S0261-3069(14)00456-7/h0030http://refhub.elsevier.com/S0261-3069(14)00456-7/h0035http://refhub.elsevier.com/S0261-3069(14)00456-7/h0035http://refhub.elsevier.com/S0261-3069(14)00456-7/h0035http://refhub.elsevier.com/S0261-3069(14)00456-7/h0040http://refhub.elsevier.com/S0261-3069(14)00456-7/h0040http://refhub.elsevier.com/S0261-3069(14)00456-7/h0040http://refhub.elsevier.com/S0261-3069(14)00456-7/h0045http://refhub.elsevier.com/S0261-3069(14)00456-7/h0045http://refhub.elsevier.com/S0261-3069(14)00456-7/h0045http://refhub.elsevier.com/S0261-3069(14)00456-7/h0050http://refhub.elsevier.com/S0261-3069(14)00456-7/h0050http://refhub.elsevier.com/S0261-3069(14)00456-7/h0055http://refhub.elsevier.com/S0261-3069(14)00456-7/h0055http://refhub.elsevier.com/S0261-3069(14)00456-7/h0055http://refhub.elsevier.com/S0261-3069(14)00456-7/h0055http://refhub.elsevier.com/S0261-3069(14)00456-7/h0060http://refhub.elsevier.com/S0261-3069(14)00456-7/h0060http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0070http://refhub.elsevier.com/S0261-3069(14)00456-7/h0070http://refhub.elsevier.com/S0261-3069(14)00456-7/h0070http://refhub.elsevier.com/S0261-3069(14)00456-7/h0075http://refhub.elsevier.com/S0261-3069(14)00456-7/h0075http://refhub.elsevier.com/S0261-3069(14)00456-7/h0080http://refhub.elsevier.com/S0261-3069(14)00456-7/h0080http://refhub.elsevier.com/S0261-3069(14)00456-7/h0080http://refhub.elsevier.com/S0261-3069(14)00456-7/h0085http://refhub.elsevier.com/S0261-3069(14)00456-7/h0085http://refhub.elsevier.com/S0261-3069(14)00456-7/h0090http://refhub.elsevier.com/S0261-3069(14)00456-7/h0090http://refhub.elsevier.com/S0261-3069(14)00456-7/h0090http://refhub.elsevier.com/S0261-3069(14)00456-7/h0095http://refhub.elsevier.com/S0261-3069(14)00456-7/h0095http://refhub.elsevier.com/S0261-3069(14)00456-7/h0100http://refhub.elsevier.com/S0261-3069(14)00456-7/h0100http://refhub.elsevier.com/S0261-3069(14)00456-7/h0100http://refhub.elsevier.com/S0261-3069(14)00456-7/h0105http://refhub.elsevier.com/S0261-3069(14)00456-7/h0105http://refhub.elsevier.com/S0261-3069(14)00456-7/h0105http://refhub.elsevier.com/S0261-3069(14)00456-7/h0110http://refhub.elsevier.com/S0261-3069(14)00456-7/h0110http://refhub.elsevier.com/S0261-3069(14)00456-7/h0110http://refhub.elsevier.com/S0261-3069(14)00456-7/h0115http://refhub.elsevier.com/S0261-3069(14)00456-7/h0115http://refhub.elsevier.com/S0261-3069(14)00456-7/h0115http://refhub.elsevier.com/S0261-3069(14)00456-7/h0120http://refhub.elsevier.com/S0261-3069(14)00456-7/h0120http://refhub.elsevier.com/S0261-3069(14)00456-7/h0125http://refhub.elsevier.com/S0261-3069(14)00456-7/h0125http://refhub.elsevier.com/S0261-3069(14)00456-7/h0125http://refhub.elsevier.com/S0261-3069(14)00456-7/h0130http://refhub.elsevier.com/S0261-3069(14)00456-7/h0130http://refhub.elsevier.com/S0261-3069(14)00456-7/h0130http://refhub.elsevier.com/S0261-3069(14)00456-7/h0135http://refhub.elsevier.com/S0261-3069(14)00456-7/h0135http://refhub.elsevier.com/S0261-3069(14)00456-7/h0140http://refhub.elsevier.com/S0261-3069(14)00456-7/h0140http://refhub.elsevier.com/S0261-3069(14)00456-7/h0140http://refhub.elsevier.com/S0261-3069(14)00456-7/h0145http://refhub.elsevier.com/S0261-3069(14)00456-7/h0145http://refhub.elsevier.com/S0261-3069(14)00456-7/h0145http://refhub.elsevier.com/S0261-3069(14)00456-7/h0145http://refhub.elsevier.com/S0261-3069(14)00456-7/h0150http://refhub.elsevier.com/S0261-3069(14)00456-7/h0150http://refhub.elsevier.com/S0261-3069(14)00456-7/h0150http://refhub.elsevier.com/S0261-3069(14)00456-7/h0150http://refhub.elsevier.com/S0261-3069(14)00456-7/h0150http://refhub.elsevier.com/S0261-3069(14)00456-7/h0150http://refhub.elsevier.com/S0261-3069(14)00456-7/h0145http://refhub.elsevier.com/S0261-3069(14)00456-7/h0145http://refhub.elsevier.com/S0261-3069(14)00456-7/h0145http://refhub.elsevier.com/S0261-3069(14)00456-7/h0140http://refhub.elsevier.com/S0261-3069(14)00456-7/h0140http://refhub.elsevier.com/S0261-3069(14)00456-7/h0140http://refhub.elsevier.com/S0261-3069(14)00456-7/h0135http://refhub.elsevier.com/S0261-3069(14)00456-7/h0135http://refhub.elsevier.com/S0261-3069(14)00456-7/h0130http://refhub.elsevier.com/S0261-3069(14)00456-7/h0130http://refhub.elsevier.com/S0261-3069(14)00456-7/h0130http://refhub.elsevier.com/S0261-3069(14)00456-7/h0125http://refhub.elsevier.com/S0261-3069(14)00456-7/h0125http://refhub.elsevier.com/S0261-3069(14)00456-7/h0125http://refhub.elsevier.com/S0261-3069(14)00456-7/h0120http://refhub.elsevier.com/S0261-3069(14)00456-7/h0120http://refhub.elsevier.com/S0261-3069(14)00456-7/h0115http://refhub.elsevier.com/S0261-3069(14)00456-7/h0115http://refhub.elsevier.com/S0261-3069(14)00456-7/h0115http://refhub.elsevier.com/S0261-3069(14)00456-7/h0110http://refhub.elsevier.com/S0261-3069(14)00456-7/h0110http://refhub.elsevier.com/S0261-3069(14)00456-7/h0110http://refhub.elsevier.com/S0261-3069(14)00456-7/h0105http://refhub.elsevier.com/S0261-3069(14)00456-7/h0105http://refhub.elsevier.com/S0261-3069(14)00456-7/h0105http://refhub.elsevier.com/S0261-3069(14)00456-7/h0100http://refhub.elsevier.com/S0261-3069(14)00456-7/h0100http://refhub.elsevier.com/S0261-3069(14)00456-7/h0100http://refhub.elsevier.com/S0261-3069(14)00456-7/h0095http://refhub.elsevier.com/S0261-3069(14)00456-7/h0095http://refhub.elsevier.com/S0261-3069(14)00456-7/h0090http://refhub.elsevier.com/S0261-3069(14)00456-7/h0090http://refhub.elsevier.com/S0261-3069(14)00456-7/h0090http://refhub.elsevier.com/S0261-3069(14)00456-7/h0085http://refhub.elsevier.com/S0261-3069(14)00456-7/h0085http://refhub.elsevier.com/S0261-3069(14)00456-7/h0080http://refhub.elsevier.com/S0261-3069(14)00456-7/h0080http://refhub.elsevier.com/S0261-3069(14)00456-7/h0080http://refhub.elsevier.com/S0261-3069(14)00456-7/h0075http://refhub.elsevier.com/S0261-3069(14)00456-7/h0075http://refhub.elsevier.com/S0261-3069(14)00456-7/h0070http://refhub.elsevier.com/S0261-3069(14)00456-7/h0070http://refhub.elsevier.com/S0261-3069(14)00456-7/h0070http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0065http://refhub.elsevier.com/S0261-3069(14)00456-7/h0060http://refhub.elsevier.com/S0261-3069(14)00456-7/h0060http://refhub.elsevier.com/S0261-3069(14)00456-7/h0055http://refhub.elsevier.com/S0261-3069(14)00456-7/h0055http://refhub.elsevier.com/S0261-3069(14)00456-7/h0055http://refhub.elsevier.com/S0261-3069(14)00456-7/h0050http://refhub.elsevier.com/S0261-3069(14)00456-7/h0050http://refhub.elsevier.com/S0261-3069(14)00456-7/h0045http://refhub.elsevier.com/S0261-3069(14)00456-7/h0045http://refhub.elsevier.com/S0261-3069(14)00456-7/h0045http://refhub.elsevier.com/S0261-3069(14)00456-7/h0040http://refhub.elsevier.com/S0261-3069(14)00456-7/h0040http://refhub.elsevier.com/S0261-3069(14)00456-7/h0040http://refhub.elsevier.com/S0261-3069(14)00456-7/h0035http://refhub.elsevier.com/S0261-3069(14)00456-7/h0035http://refhub.elsevier.com/S0261-3069(14)00456-7/h0035http://refhub.elsevier.com/S0261-3069(14)00456-7/h0030http://refhub.elsevier.com/S0261-3069(14)00456-7/h0030http://refhub.elsevier.com/S0261-3069(14)00456-7/h0030http://refhub.elsevier.com/S0261-3069(14)00456-7/h0025http://refhub.elsevier.com/S0261-3069(14)00456-7/h0025http://refhub.elsevier.com/S0261-3069(14)00456-7/h0020http://refhub.elsevier.com/S0261-3069(14)00456-7/h0020http://refhub.elsevier.com/S0261-3069(14)00456-7/h0020http://refhub.elsevier.com/S0261-3069(14)00456-7/h0015http://refhub.elsevier.com/S0261-3069(14)00456-7/h0015http://refhub.elsevier.com/S0261-3069(14)00456-7/h0010http://refhub.elsevier.com/S0261-3069(14)00456-7/h0010http://refhub.elsevier.com/S0261-3069(14)00456-7/h0005http://refhub.elsevier.com/S0261-3069(14)00456-7/h0005