Photoelastic Characterisation of the Stress Transfer at...

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Photoelastic Characterisation of the Stress Transfer at Fibre- break in Model Composites Fangming Zhao and Frank Jones Ceramics and Composites Laboratory Department of Engineering Materials The University of Sheffield CompTest 2006, 10-12 April 2006, Porto, Portugal

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  • Photoelastic Characterisation of the Stress Transfer at Fibre-break in Model Composites

    Fangming Zhao and Frank Jones

    Ceramics and Composites LaboratoryDepartment of Engineering Materials

    The University of Sheffield

    CompTest 2006, 10-12 April 2006, Porto, Portugal

  • Outline• Background

    – Micro-mechanical methods to evaluate fibre surface treatment and composite interface

    • Phase-stepping photoelasticity– Phase-stepping polariscope – Experimental system

    • Photoelastic analysis and Finite Element Analysis– Stress transfer at the end of fibre-break – Results from photoelastic analysis– Results from FEA

    • Conclusions• Acknowledgements

  • Background Current approaches for quantifying interfacial response in a fibre composite

    Fragmentation testPull-out testMicro-bond test

    Interfacial shear strength(shear stress)

    c

    fufi L

    r στ =

    Raman or fluorescencespectroscopy

    Strain or stress in fibre Inferring τi

    dxdr fx

    ixσ

    τ2

    =

    How to quantify the effect of debonding and matrix crack onStress transfer

    Carbon and polymer fibres (high modules)

  • Phase-stepping photoelasticity

    • Stress field in matrix• Interfacial shear stress

    Phase-stepping Photoelasticity

    Direct measurement

    Recording birefringent images at the instantaneous moment that failure events occur

  • Principle of phase-stepping photoelasticity• Four CCD cameras are used for

    collecting photoelastic images simultaneously

    • Cubic beam-splitters provide four elliptically polarized light beam

    • The pairs of quarter-wave plates and analysers are orientated so as to generate four phase-steps in photoelastic data

    Image number

    Orientation of quarter-wave plate

    Orientation of analyser

    1 π/4 π/42 0 03 π/2 π/24 0 π/4

    An arrangement of optical device and light path

  • Theoretical model for the instrument

    )sin2sin1(2

    2

    3 δθ−=aE

    )sin2sin1(2

    2

    2 δθ+=aE

    )cos1(2

    2

    4 δ−=aE

    )sin2cos1(2

    2

    1 δθ−=aE

    E.A. Patterson & Z.F. Wang J Strain Analysis 33 (1998) 1-15

    Isoclinic angle

    Relative retardation

    ⎟⎟⎠

    ⎞⎜⎜⎝

    ⎛−+

    −= −132

    321

    2tan

    21

    EEEEEθ

    ⎟⎟⎠

    ⎞⎜⎜⎝

    ⎛−+

    −= −)2(2

    tan21

    432

    321

    EEESinEE

    θδ

  • Experimental system

    hNf2

    )(21

    21maxσσστ =−=

    αττ 2sinmax=i

    A filter (wavelength: 542±5 nm)produces an essentially mono-chromatic green sourceA multiplex combines four signals into a single compositeimageThe composite image is re-divided into four phase-steepingimages and processed by a software operation

    Mini-tester

    Phase-steppingpolariscope

    Microscope

    πδ2

    =N

  • Single fibre model composites (SFC)

    • Araldite LY5052/HY5052 cold cured epoxy resinCold-cured

    Young’s modulus (GPa): 3.20Tensile strength (MPa) : 72Stress-fringe constant fσ (MPa/fringe/mm): 20.23

    Cold-curing: 7 days at room temperature

    • E-glass and Al2O3 fibresE-glass Al2O3

    Young’s modulus 72 GPa 414 GPaDiameter 80 μm 125 μm

  • Fragmentation test of SFC and photoelasticmeasurement

    Measured area

    Fibre Strain gauge

    F F

    Increasing matrix stress/strain

    Fibre end

    Fibre break& matrix crack

  • Effect of a soft interphase on matrix crackfor glass fibre

    Resin Em(MPa)

    σuts(MPa)

    Cold-draw strength (MPa)

    Matrix resin 3200 72

    Coating epoxy 2100 41 31

    LY 1556 GY 298 NMA Capcure 3-80050 50 55.9 20.9

    The resin cured at 80 ºC for 4 hours and 130 ºC for 3 hours

    Epoxy resin for coating

    Mechanical properties of matrix and coating epoxy resins

  • Uncoated glass fibre Contour maps of fringe order at fibre-break

    (b) σapp = 17.45 MPa, Lf = 3.35 mm

    End of broken fibreTip of matrix crack

    (a) σapp = 14.37 MPa, Lf = 11.26 mm

    0.89 mm

    0.52 mm

    Matrix

    • A zone of higher fringe order appears initially at the tip of the matrix crack

    • At higher applied stress, the zone of higher fringe order extends along the fragment

    • The matrix crack disturbs the stress field inthe matrix close to the interface

    d = 88.65 μm

    Fibre

    Crack

  • Epoxy-coated fibre: Contour maps of fringe order in matrix at fibre-break

    (b) σapp = 12.42 MPa, Lf = 11.03 mm

    (c) σapp = 17.63 MPa, Lf = 0.92 mm

    d = 91.71 μm

    Smaller transverse matrix cracksNo debonding

    (a) σapp = 8.56 MPa, Lf = 11.03 mm

    Crack tip Fibre

    Matrix

    FM Zhao, EA Patterson, FR Jones, Materials Sci Eng A 412 (2005) 83–87

  • 0

    10

    20

    30

    40

    50

    0 0.2 0.4 0.6 0.8 1 1.2

    Distance from fibre break (mm)

    Inte

    rfac

    ial s

    hear

    stre

    ss (M

    Pa)

    14.37 MPa17.45 MPa

    Role of interphase on shear stress profiles

    0

    5

    10

    15

    20

    25

    30

    0 0.2 0.4 0.6 0.8 1 1.2

    Distance from fibre break (mm)

    Inte

    rfac

    ial s

    hear

    stre

    ss (M

    Pa)

    8.56 MPa12.42 MPa17.63 MPa

    Uncoated fibre Epoxy-coated fibre

  • Effect of the size of transverse matrix crackContour maps of fringe order around the cracks with different sizes

    Crack size: less than 2 μmLf = 3.77 mm, σm = 9.17 MPa

    Crack size: 98.72 μmLf = 1.80 mm, σm = 13.65 MPa

    Crack tip

    Crack size: 62.02 μmLf = 6.37 mm, σm = 9.17 MPa

    Crack tip

    Crack tip

    Matrix

  • Effect of the size of transverse matrix crackDistribution of fringe order at interface

    0.5

    0.6

    0.7

    0.8

    0.9

    0 0.5 1 1.5 2

    Distance from fibre-break (mm)

    Inte

    rfaci

    al fr

    inge

    ord

    er

    B1, crack length: ~ 2 μm

    B2, crack length: 63 μm

    σm = 9.04 MPa1

    1.1

    1.2

    1.3

    1.4

    0 0.5 1 1.5 2

    Distance from fibre-break (mm)

    Inte

    rfaci

    al fr

    inge

    ord

    er

    B3, crack length: 99 μm

    σm = 13.65 MPa

  • FEA results for different sizes of crack

    0

    100

    200

    300

    400

    500

    600

    700

    800

    900

    0 1 2 3 4 5 6Distance from the fibre end (mm)

    Tens

    ile s

    tres

    s in

    the

    fibre

    (MP

    a)

    No matrix crack0.1 mm matrix crack0.2 mm matrix crack0.4 mm matrix crack

    0 0.1 mm0.2 mm0.4 mm

    0

    5

    10

    15

    20

    25

    30

    35

    40

    45

    0 0.2 0.4 0.6 0.8 1Distance from the fibre end (mm)

    Shea

    r stre

    ss a

    t fib

    re/m

    atri

    x in

    terfa

    ce

    (MPa

    )

    No matrix crack0.1 mm matrix crack0.2 mm matrix crack0.4 mm matrix crack

    Maximum

    AC. Johnson, FM. Zhao, SA. Hayes, F. R. Jones Composites Sci and Technol., on-line available

  • Comparison of FEA and experimental results

    0

    5

    10

    15

    20

    25

    30

    35

    0 0.25 0.5 0.75 1 1.25 1.5Distance from the fibre break (mm)

    shea

    r st

    ress

    at t

    he fi

    bre/

    mat

    rix

    inte

    rface

    (MP

    a)Determined by photoelasticity

    Finite element prediction

    Transverse crack length = 0.2 mm

  • Effect of a transverse matrix crack on shear stress transfer

    0

    4

    8

    12

    16

    20

    0.0 0.5 1.0 1.5

    Distance from fibre break (mm)

    Inte

    rfaci

    al sh

    ear s

    tress

    (MPa

    )

    εapp = 0.188%σapp = 6.36 MPa

    εapp = 0.188%, σapp = 6.36 MPaLf = 13.32 mm

    Al2O3 fibre

    Matrix crackFibre

    Matrix

    F.M. Zhao et al Composites Part A, 36 (2005) 229-244

  • Combined effect of transverse matrix crack and debonding at fibre-break (Al2O3 fibre)

    Crack tip

    Crack

    σapp = 16.08 MPa, εapp = 0.48%

    Debonded interface

    Bonded area

    FM Zhao, FR Jones et al., Composites Part A 36 (2005) 229-244

    Crack tip

    σapp = 13.10 MPa, εapp = 0.388%

    Crack

    Matrix

    1.67 mm

    1.00

    mm

  • Conclusions

    • Automated phase-stepping polariscope has been used to measure the micro stress field in the matrix near a fibre-break and the interfacial shear stress for Al2O3 and E-glass fibre epoxy model composites

    • Effect of a transverse matrix crack on stress transfer has been investigated by photoelasticity

    • It has been found that the matrix crack can delay significantly stress transfer

    • A soft interphase can be created, which controls the propagation of a transverse matrix crack

    • The debonding at the fibre break can be detected accurately by photoelasticity

  • Acknowledgements

    • EPSRC for funding the research

    • Photran Inc. (USA) for the supply of sapphire fibre and The Advanced Composites Group (UK) for supplying epoxy resins

    • Prof K Schulte (Germany) for supplying E-glass fibre made by The Institute of Polymer Research Dresden.

    • Prof EA Patterson for introducing the phase-stepping photoelastictechnique

    • Dr C Johnson,Mr H Sugihara and Mr Z Liu for coating E-glass fibres

    • Dr Z Wang for technique support

    Photoelastic Characterisation of the Stress Transfer at Fibre-break in Model Composites OutlineBackground Current approaches for quantifying interfacial response in a fibre compositePhase-stepping photoelasticityPrinciple of phase-stepping photoelasticityTheoretical model for the instrumentExperimental systemSingle fibre model composites (SFC)Fragmentation test of SFC and photoelastic measurementEffect of a soft interphase on matrix crack�for glass fibreUncoated glass fibre Contour maps of fringe order at fibre-breakEpoxy-coated fibre: Contour maps of fringe order in matrix at fibre-breakRole of interphase on shear stress profilesEffect of the size of transverse matrix crack�Contour maps of fringe order around the cracks with different sizesEffect of the size of transverse matrix crack�Distribution of fringe order at interfaceFEA results for different sizes of crackComparison of FEA and experimental resultsEffect of a transverse matrix crack on shear stress transferCombined effect of transverse matrix crack and debonding at fibre-break (Al2O3 fibre)Conclusions Acknowledgements

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    Photoelastic Characterisation of the Stress Transfer at Fibre-break in Model Composites

    Fangming Zhao and Frank Jones

    Ceramics and Composites Laboratory

    Department of Engineering Materials

    The University of Sheffield

    CompTest 2006, 10-12 April 2006, Porto, Portugal

    Outline

    Background

    Micro-mechanical methods to evaluate fibre surface treatment and composite interface

    Phase-stepping photoelasticity

    Phase-stepping polariscope

    Experimental system

    Photoelastic analysis and Finite Element Analysis

    Stress transfer at the end of fibre-break

    Results from photoelastic analysis

    Results from FEA

    Conclusions

    Acknowledgements

    Background Current approaches for quantifying interfacial response in a fibre composite

    Fragmentation test

    Pull-out test

    Micro-bond test

    Interfacial shear strength

    (shear stress)

    Raman or fluorescence

    spectroscopy

    Strain or stress

    in fibre

    Inferring ti

    How to quantify the effect of

    debonding and matrix crack on

    Stress transfer

    Carbon and polymer fibres

    (high modules)

    Phase-stepping photoelasticity

    Stress field in matrix

    Interfacial shear stress

    Phase-stepping Photoelasticity

    Direct measurement

    Recording birefringent images

    at the instantaneous moment that failure events occur

    Principle of phase-stepping photoelasticity

    Four CCD cameras are used for collecting photoelastic images simultaneously

    Cubic beam-splitters provide four elliptically polarized light beam

    The pairs of quarter-wave plates and analysers are orientated so as to generate four phase-steps in photoelastic data

    An arrangement of optical device

    and light path

    Image numberOrientation of quarter-wave plateOrientation of analyser

    1/4/4

    200

    3/2/2

    40/4

    142.psd

    Theoretical model for the instrument

    E.A. Patterson & Z.F. Wang J Strain Analysis 33 (1998) 1-15

    Isoclinic angle

    Relative retardation

    Experimental system

    A filter (wavelength: 5425 nm)

    produces an essentially mono-

    chromatic green source

    A multiplex combines four

    signals into a single composite

    image

    The composite image is re-

    divided into four phase-steeping

    images and processed by a

    software operation

    Mini-tester

    Phase-stepping

    polariscope

    Microscope

    Single fibre model composites (SFC)

    Araldite LY5052/HY5052 cold cured epoxy resin

    Cold-cured

    Young’s modulus (GPa): 3.20

    Tensile strength (MPa) : 72

    Stress-fringe constant fs (MPa/fringe/mm): 20.23

    Cold-curing: 7 days at room temperature

    E-glass and Al2O3 fibres

    E-glass Al2O3

    Young’s modulus 72 GPa 414 GPa

    Diameter 80 mm 125 mm

    Fragmentation test of SFC and photoelastic measurement

    Measured area

    Fibre

    Strain gauge

    F

    F

    Increasing

    matrix stress/strain

    Fibre end

    Fibre break

    & matrix crack

    Effect of a soft interphase on matrix crack

    for glass fibre

    The resin cured at 80 ºC for 4 hours and 130 ºC for 3 hours

    Epoxy resin for coating

    Mechanical properties of matrix and coating epoxy resins

    ResinEm (MPa)suts (MPa)Cold-draw strength (MPa)

    Matrix resin320072

    Coating epoxy21004131

    LY 1556GY 298NMACapcure 3-800

    505055.920.9

    Uncoated glass fibre Contour maps of fringe order at fibre-break

    A zone of higher fringe order appears

    initially at the tip of the matrix crack

    At higher applied stress, the zone of higher

    fringe order extends along the fragment

    The matrix crack disturbs the stress field in

    the matrix close to the interface

    (b) sapp = 17.45 MPa, Lf = 3.35 mm

    End of broken fibre

    Tip of matrix crack

    (a) sapp = 14.37 MPa, Lf = 11.26 mm

    0.89 mm

    0.52 mm

    Matrix

    d = 88.65 mm

    Fibre

    Crack

    Epoxy-coated fibre: Contour maps of fringe order in matrix at fibre-break

    d = 91.71 mm

    Smaller transverse matrix cracks

    No debonding

    FM Zhao, EA Patterson, FR Jones, Materials Sci Eng A 412 (2005) 83–87

    (b) sapp = 12.42 MPa, Lf = 11.03 mm

    (c) sapp = 17.63 MPa, Lf = 0.92 mm

    Crack tip

    Fibre

    Matrix

    (a) sapp = 8.56 MPa, Lf = 11.03 mm

    162.psd

    Role of interphase on shear stress profiles

    Uncoated fibre

    Epoxy-coated fibre

    Effect of the size of transverse matrix crack

    Contour maps of fringe order around the cracks with different sizes

    Crack size: less than 2 mm

    Lf = 3.77 mm, sm = 9.17 MPa

    Crack size: 98.72 mm

    Lf = 1.80 mm, sm = 13.65 MPa

    Crack tip

    Crack size: 62.02 mm

    Lf = 6.37 mm, sm = 9.17 MPa

    Crack tip

    Crack tip

    Matrix

    Effect of the size of transverse matrix crack

    Distribution of fringe order at interface

    B1, crack length: ~ 2 mm

    B2, crack length: 63 mm

    sm = 9.04 MPa

    B3, crack length: 99 mm

    sm = 13.65 MPa

    FEA results for different sizes of crack

    AC. Johnson, FM. Zhao, SA. Hayes, F. R. Jones

    Composites Sci and Technol., on-line available

    Maximum

    Comparison of FEA and experimental results

    Transverse crack length = 0.2 mm

    Effect of a transverse matrix crack on shear stress transfer

    eapp = 0.188%

    sapp = 6.36 MPa

    F.M. Zhao et al Composites Part A, 36 (2005) 229-244

    eapp = 0.188%,

    sapp = 6.36 MPa

    Lf = 13.32 mm

    Al2O3 fibre

    Matrix crack

    Fibre

    Matrix

    Chart3

    0.007196

    0.014392

    0.021588

    0.028784

    0.03598

    0.043176

    0.050372

    0.057568

    0.064764

    0.07196

    0.079156

    0.086352

    0.093548

    0.100744

    0.10794

    0.115136

    0.122332

    0.129528

    0.136724

    0.14392

    0.151116

    0.158312

    0.165508

    0.172704

    0.1799

    0.187096

    0.194292

    0.201488

    0.208684

    0.21588

    0.223076

    0.230272

    0.237468

    0.244664

    0.25186

    0.259056

    0.266252

    0.273448

    0.280644

    0.28784

    0.295036

    0.302232

    0.309428

    0.316624

    0.32382

    0.331016

    0.338212

    0.345408

    0.352604

    0.3598

    0.366996

    0.374192

    0.381388

    0.388584

    0.39578

    0.402976

    0.410172

    0.417368

    0.424564

    0.43176

    0.438956

    0.446152

    0.453348

    0.460544

    0.46774

    0.474936

    0.482132

    0.489328

    0.496524

    0.50372

    0.510916

    0.518112

    0.525308

    0.532504

    0.5397

    0.546896

    0.554092

    0.561288

    0.568484

    0.57568

    0.582876

    0.590072

    0.597268

    0.604464

    0.61166

    0.618856

    0.626052

    0.633248

    0.640444

    0.64764

    0.654836

    0.662032

    0.669228

    0.676424

    0.68362

    0.690816

    0.698012

    0.705208

    0.712404

    0.7196

    0.726796

    0.733992

    0.741188

    0.748384

    0.75558

    0.762776

    0.769972

    0.777168

    0.784364

    0.79156

    0.798756

    0.805952

    0.813148

    0.820344

    0.82754

    0.834736

    0.841932

    0.849128

    0.856324

    0.86352

    0.870716

    0.877912

    0.885108

    0.892304

    0.8995

    0.906696

    0.913892

    0.921088

    0.928284

    0.93548

    0.942676

    0.949872

    0.957068

    0.964264

    0.97146

    0.978656

    0.985852

    0.993048

    1.000244

    1.00744

    1.014636

    1.021832

    1.029028

    1.036224

    1.04342

    1.050616

    1.057812

    1.065008

    1.072204

    1.0794

    1.086596

    1.093792

    1.100988

    1.108184

    1.11538

    1.122576

    1.129772

    1.136968

    1.144164

    1.15136

    1.158556

    1.165752

    1.172948

    1.180144

    1.18734

    1.194536

    1.201732

    1.208928

    1.216124

    1.22332

    1.230516

    1.237712

    1.244908

    1.252104

    1.2593

    1.266496

    1.273692

    1.280888

    1.288084

    1.29528

    1.302476

    1.309672

    1.316868

    1.324064

    1.33126

    1.338456

    1.345652

    1.352848

    1.360044

    1.36724

    1.374436

    1.381632

    1.388828

    1.396024

    1.40322

    1.410416

    1.417612

    1.424808

    Left end of F2

    Distance from fibre break (mm)

    Interfacial shear stress (MPa)

    17.8137669948

    20.0987265496

    18.8341403649

    14.4426665422

    10.4192118281

    7.9026922007

    6.3902585892

    5.1190847294

    3.9519989271

    3.276674982

    2.5448879222

    1.9744761267

    1.6669316785

    1.3116060747

    0.9201926538

    0.5341895007

    0.2476468525

    0.172571924

    0.1770517694

    0.178569812

    0.0456755991

    0.2700959246

    0.4779870602

    0.6008421138

    0.6008421138

    0.8213796678

    0.8369863033

    0.8438696458

    0.9807260921

    1.3293383437

    1.4511498858

    1.6917336585

    1.5730203617

    1.5572237747

    1.8837944762

    1.8837944762

    2.1547456379

    2.316918968

    2.5621156316

    2.5426354894

    2.6638081318

    2.7635031021

    3.0083295824

    3.2782053949

    3.4717545553

    3.7139253696

    4.0527364063

    4.2186767129

    4.1415807025

    4.3288439965

    4.3420310219

    4.5144743402

    4.7228659954

    4.8741088778

    4.8266732391

    4.8266732391

    4.8725112305

    4.9932862661

    5.1073691108

    5.4496161668

    5.5388729499

    5.3730280448

    5.4515108886

    5.5957036688

    5.6719200278

    5.7790907715

    5.8125240975

    5.9934570768

    6.0655601861

    6.2516631995

    6.1278353088

    5.9695484131

    5.8126812944

    5.8507862143

    5.9463778929

    5.8629074806

    6.0574195407

    6.2233644786

    6.5289226238

    6.4785157626

    6.2770049473

    6.1358686789

    6.1358686789

    6.1977696454

    6.2281659649

    6.2894229566

    6.2211058485

    6.1648755103

    6.1648755103

    6.0783126813

    6.1352529288

    6.2352509402

    6.0859976042

    6.2594786117

    6.1520661038

    6.0448283295

    6.1315258823

    6.0963081272

    6.1040542877

    6.2209743265

    6.2209743265

    6.0880461274

    5.9892460739

    5.9399907493

    5.8217281964

    5.7199817632

    5.5878639986

    5.5878639986

    5.5454606449

    5.547155918

    5.6266032908

    5.5262058269

    5.5764650394

    5.6558453149

    5.4535641442

    5.3818135795

    5.2775917235

    5.2319503023

    5.2857159771

    5.2319503023

    4.9729569291

    4.8992601337

    4.7322286765

    4.982704777

    5.0676054499

    5.0676054499

    5.0893275542

    4.9936753599

    4.7934939732

    4.6639065957

    4.5931753143

    4.4952611772

    4.4384475643

    4.5656996214

    4.6683126239

    4.6998047238

    4.5691087592

    4.3668457622

    4.2691403747

    4.2377945138

    4.3959292321

    4.270778823

    4.081732479

    3.9848541879

    4.0445718623

    3.9755811907

    3.8398353175

    3.7381557239

    3.6783602526

    3.7772340054

    3.6783602526

    3.638256164

    3.7037665976

    3.7293071815

    3.6913930377

    3.6265903708

    3.5992181207

    3.7017590778

    3.5648543586

    3.5236812848

    3.4488579813

    3.5368530638

    3.6005622886

    3.6005622886

    3.329225885

    3.2848529265

    3.301493876

    3.4063668624

    3.4763215361

    3.4763215361

    3.344011994

    3.2090160978

    3.2090160978

    3.3146194549

    3.3028646889

    3.0893488597

    3.1645160038

    3.0871699767

    3.1607208189

    3.0420566342

    3.0420566342

    2.996099234

    2.8540000441

    2.883576627

    2.7969293666

    2.714614474

    2.608834315

    2.5300684194

    2.4478425046

    2.6624601407

    2.6624601407

    2.7148689414

    2.5033828044

    2.4478425046

    2.3655616199

    2.2381215852

    2.0931669844

    2.052037904

    Sheet1

    Sheet1

    00

    0.0071960.007196

    0.0143920.014392

    0.0215880.021588

    0.0287840.028784

    0.035980.03598

    0.0431760.043176

    0.0503720.050372

    0.0575680.057568

    0.0647640.064764

    0.071960.07196

    0.0791560.079156

    0.0863520.086352

    0.0935480.093548

    0.1007440.100744

    0.107940.10794

    0.1151360.115136

    0.1223320.122332

    0.1295280.129528

    0.1367240.136724

    0.143920.14392

    0.1511160.151116

    0.1583120.158312

    0.1655080.165508

    0.1727040.172704

    0.17990.1799

    0.1870960.187096

    0.1942920.194292

    0.2014880.201488

    0.2086840.208684

    0.215880.21588

    0.2230760.223076

    0.2302720.230272

    0.2374680.237468

    0.2446640.244664

    0.251860.25186

    0.2590560.259056

    0.2662520.266252

    0.2734480.273448

    0.2806440.280644

    0.287840.28784

    0.2950360.295036

    0.3022320.302232

    0.3094280.309428

    0.3166240.316624

    0.323820.32382

    0.3310160.331016

    0.3382120.338212

    0.3454080.345408

    0.3526040.352604

    0.35980.3598

    0.3669960.366996

    0.3741920.374192

    0.3813880.381388

    0.3885840.388584

    0.395780.39578

    0.4029760.402976

    0.4101720.410172

    0.4173680.417368

    0.4245640.424564

    0.431760.43176

    0.4389560.438956

    0.4461520.446152

    0.4533480.453348

    0.4605440.460544

    0.467740.46774

    0.4749360.474936

    0.4821320.482132

    0.4893280.489328

    0.4965240.496524

    0.503720.50372

    0.5109160.510916

    0.5181120.518112

    0.5253080.525308

    0.5325040.532504

    0.53970.5397

    0.5468960.546896

    0.5540920.554092

    0.5612880.561288

    0.5684840.568484

    0.575680.57568

    0.5828760.582876

    0.5900720.590072

    0.5972680.597268

    0.6044640.604464

    0.611660.61166

    0.6188560.618856

    0.6260520.626052

    0.6332480.633248

    0.6404440.640444

    0.647640.64764

    0.6548360.654836

    0.6620320.662032

    0.6692280.669228

    0.6764240.676424

    0.683620.68362

    0.6908160.690816

    0.6980120.698012

    0.7052080.705208

    0.7124040.712404

    0.71960.7196

    0.7267960.726796

    0.7339920.733992

    0.7411880.741188

    0.7483840.748384

    0.755580.75558

    0.7627760.762776

    0.7699720.769972

    0.7771680.777168

    0.7843640.784364

    0.791560.79156

    0.7987560.798756

    0.8059520.805952

    0.8131480.813148

    0.8203440.820344

    0.827540.82754

    0.8347360.834736

    0.8419320.841932

    0.8491280.849128

    0.8563240.856324

    0.863520.86352

    0.8707160.870716

    0.8779120.877912

    0.8851080.885108

    0.8923040.892304

    0.89950.8995

    0.9066960.906696

    0.9138920.913892

    0.9210880.921088

    0.9282840.928284

    0.93548

    0.942676

    0.949872

    0.957068

    0.964264

    0.97146

    0.978656

    0.985852

    0.993048

    1.000244

    1.00744

    1.014636

    1.021832

    1.029028

    1.036224

    1.04342

    1.050616

    1.057812

    1.065008

    1.072204

    1.0794

    1.086596

    1.093792

    1.100988

    1.108184

    1.11538

    1.122576

    1.129772

    1.136968

    1.144164

    1.15136

    1.158556

    1.165752

    1.172948

    1.180144

    1.18734

    1.194536

    1.201732

    1.208928

    1.216124

    Left end of F1

    Right end of F2

    Distance from fibre end (mm)

    Interfacial shear stress (MPa)

    11.8525224155

    10.1460931241

    12.4653381267

    10.4743563779

    12.2540195349

    10.2619192049

    10.7438775701

    9.5694559099

    8.1782462701

    9.7042918756

    6.1101760989

    10.3494542986

    4.7153212115

    10.7150360796

    3.9565258707

    10.3672389512

    3.405370528

    9.4339850578

    2.690572914

    8.4411729791

    1.8261944543

    8.2150973034

    1.5460827076

    8.3205434314

    1.490927626

    8.1898135668

    1.1281145957

    7.86892449

    1.1205626991

    7.2312048129

    1.1130108025

    6.5907734975

    1.3150129724

    5.6394771015

    1.8586062934

    5.0160670585

    2.3459832714

    4.5859824594

    2.4218268035

    4.5070695276

    2.6236055029

    4.4651675906

    2.31012279

    4.6426870558

    1.9693417258

    4.8897534639

    1.1708659319

    5.0932435261

    0.518990233

    4.9505004688

    0.3299611029

    4.5055608359

    0.5541655627

    4.1384015207

    1.6339950532

    4.0326626857

    2.6086774019

    3.9651822172

    3.418396805

    3.8610116553

    4.3098062215

    3.6017834796

    4.9857031324

    3.378950272

    5.8626899103

    3.2661147137

    6.7162106762

    2.9817795595

    7.6704298416

    2.6115847543

    7.8343440038

    2.0830101006

    8.6535019052

    1.9924968615

    9.1512146014

    2.074943263

    9.5338366229

    2.2730271215

    9.5760881675

    2.2908513626

    9.6655671593

    2.2199103519

    9.9397459165

    1.4733513659

    10.3297326493

    0.8225086341

    10.6911275573

    0.2199911017

    11.1580689563

    0.0269529076

    11.3559619998

    0.0455716568

    11.7281815906

    0.2863769739

    11.3641457298

    0.5296085694

    11.4714045622

    0.9355267623

    11.4284617623

    1.5921071699

    11.9617570085

    2.097208371

    12.283422603

    2.763301319

    12.2239294269

    3.2585288778

    12.1007645611

    3.8824396718

    11.9908359168

    4.3908183142

    12.0383193248

    4.7182392441

    12.6040133307

    5.1720617392

    12.5179095367

    5.2192925623

    12.2979012913

    5.3020989231

    12.0014852082

    5.5177688093

    11.8384743963

    5.8646057273

    12.0830498134

    6.0581210661

    11.7467097174

    6.3238985321

    11.452822632

    6.4261997352

    11.8247091488

    6.4910189358

    12.2065913353

    6.8520240162

    12.4226649563

    7.0998620052

    12.4006625221

    7.2111991636

    12.1547601906

    7.2286590692

    11.9383568907

    7.2995586991

    11.9383568907

    7.4233552995

    11.6917967063

    7.6420710008

    11.7302866513

    7.6922231597

    11.9119728008

    7.6264505989

    11.8817250557

    7.6725958521

    12.071975494

    7.9786251205

    11.9873204925

    8.1425509576

    11.7005499967

    8.1380072631

    11.7436948262

    8.0045974031

    11.6446622206

    8.0063147482

    11.3969162414

    8.0484477357

    11.21573492

    7.9291210101

    11.2404616881

    7.8777056836

    11.3749489648

    7.9241290023

    11.5757413107

    8.1521418504

    11.5654059139

    8.252220181

    11.1893808027

    8.3060296934

    11.0069897451

    7.9506193236

    11.0069897451

    7.8484866638

    10.9836608499

    8.0790988092

    10.7953129503

    8.2218433408

    11.0416705499

    8.1957751785

    10.8073358877

    7.9556230477

    10.9475576562

    7.8430000987

    10.819670851

    7.8560494477

    10.6639198502

    7.9171758689

    10.7825880701

    7.9171758689

    11.008425019

    7.9556230477

    11.134787562

    7.8044345942

    11.0806739707

    7.7030130406

    11.1181415449

    7.5876202107

    11.0995296293

    7.8136030475

    11.035275047

    7.812219886

    10.6360740713

    7.8136030475

    10.2471008283

    7.6388093444

    10.5953602868

    7.6891431751

    10.673281808

    7.6891431751

    10.836142148

    7.7435651345

    10.5139619585

    7.6277852295

    10.3630228548

    7.5141806711

    10.0033864915

    7.4129712997

    10.1133314013

    7.6025192465

    10.1531908704

    7.7226485504

    10.3774891694

    7.5386224846

    10.4082941744

    7.3560499624

    10.4996170283

    7.4357167294

    10.619502387

    7.492258622

    10.2188675437

    7.4313401816

    10.1063818258

    7.3493460143

    9.8829372402

    7.2855851351

    9.6218414357

    7.0798868253

    9.7146292768

    6.7353403205

    9.3865496187

    6.5080822216

    9.7859808413

    6.6781845435

    9.7164138172

    6.8456928374

    9.8397236081

    6.603926474

    9.5463929418

    6.5556182426

    9.5463929418

    6.392612301

    9.5743556692

    6.694272926

    9.6581515913

    6.5755866966

    9.758215145

    9.9441369198

    9.8463668741

    9.758215145

    9.8266874397

    9.8266874397

    9.6830085404

    9.4830715026

    9.2487081522

    9.3028288646

    9.6830085404

    9.7027995416

    9.6837728524

    9.5859015572

    9.4369483886

    9.5515310397

    9.3810035625

    9.3810035625

    9.2014656252

    9.2014656252

    9.1013086465

    9.131085008

    9.0032800107

    9.1363611681

    8.8707596683

    8.6540853957

    8.5720679242

    8.5720679242

    8.5899235758

    8.8459974664

    8.7403722574

    8.6054456409

    8.4237102464

    8.3672516607

    8.2069782602

    8.4995709891

    8.3696136588

    8.3696136588

    8.3696136588

    8.369614281

    Sheet2

    0.0071960.007196

    0.0143920.014392

    0.0215880.021588

    0.0287840.028784

    0.035980.03598

    0.0431760.043176

    0.0503720.050372

    0.0575680.057568

    0.0647640.064764

    0.071960.07196

    0.0791560.079156

    0.0863520.086352

    0.0935480.093548

    0.1007440.100744

    0.107940.10794

    0.1151360.115136

    0.1223320.122332

    0.1295280.129528

    0.1367240.136724

    0.143920.14392

    0.1511160.151116

    0.1583120.158312

    0.1655080.165508

    0.1727040.172704

    0.17990.1799

    0.1870960.187096

    0.1942920.194292

    0.2014880.201488

    0.2086840.208684

    0.215880.21588

    0.2230760.223076

    0.2302720.230272

    0.2374680.237468

    0.2446640.244664

    0.251860.25186

    0.2590560.259056

    0.2662520.266252

    0.2734480.273448

    0.2806440.280644

    0.287840.28784

    0.2950360.295036

    0.3022320.302232

    0.3094280.309428

    0.3166240.316624

    0.323820.32382

    0.3310160.331016

    0.3382120.338212

    0.3454080.345408

    0.3526040.352604

    0.35980.3598

    0.3669960.366996

    0.3741920.374192

    0.3813880.381388

    0.3885840.388584

    0.395780.39578

    0.4029760.402976

    0.4101720.410172

    0.4173680.417368

    0.4245640.424564

    0.431760.43176

    0.4389560.438956

    0.4461520.446152

    0.4533480.453348

    0.4605440.460544

    0.467740.46774

    0.4749360.474936

    0.4821320.482132

    0.4893280.489328

    0.4965240.496524

    0.503720.50372

    0.5109160.510916

    0.5181120.518112

    0.5253080.525308

    0.5325040.532504

    0.53970.5397

    0.5468960.546896

    0.5540920.554092

    0.5612880.561288

    0.5684840.568484

    0.575680.57568

    0.5828760.582876

    0.5900720.590072

    0.5972680.597268

    0.6044640.604464

    0.611660.61166

    0.6188560.618856

    0.6260520.626052

    0.6332480.633248

    0.6404440.640444

    0.647640.64764

    0.6548360.654836

    0.6620320.662032

    0.6692280.669228

    0.6764240.676424

    0.683620.68362

    0.6908160.690816

    0.6980120.698012

    0.7052080.705208

    0.7124040.712404

    0.71960.7196

    0.7267960.726796

    0.7339920.733992

    0.7411880.741188

    0.7483840.748384

    0.755580.75558

    0.7627760.762776

    0.7699720.769972

    0.7771680.777168

    0.7843640.784364

    0.791560.79156

    0.7987560.798756

    0.8059520.805952

    0.8131480.813148

    0.8203440.820344

    0.827540.82754

    0.8347360.834736

    0.8419320.841932

    0.8491280.849128

    0.8563240.856324

    0.863520.86352

    0.8707160.870716

    0.8779120.877912

    0.8851080.885108

    0.8923040.892304

    0.89950.8995

    0.9066960.906696

    0.9138920.913892

    0.9210880.921088

    0.9282840.928284

    0.935480.93548

    0.9426760.942676

    0.9498720.949872

    0.9570680.957068

    0.9642640.964264

    0.971460.97146

    0.9786560.978656

    0.9858520.985852

    0.9930480.993048

    1.0002441.000244

    1.007441.00744

    1.0146361.014636

    1.0218321.021832

    1.0290281.029028

    1.0362241.036224

    1.043421.04342

    1.0506161.050616

    1.0578121.057812

    1.0650081.065008

    1.0722041.072204

    1.07941.0794

    1.0865961.086596

    1.0937921.093792

    1.1009881.100988

    1.1081841.108184

    1.115381.11538

    1.1225761.122576

    1.1297721.129772

    1.1369681.136968

    1.1441641.144164

    1.151361.15136

    1.1585561.158556

    1.1657521.165752

    1.1729481.172948

    1.1801441.180144

    1.187341.18734

    1.1945361.194536

    1.2017321.201732

    1.2089281.208928

    1.2161241.216124

    1.223321.22332

    1.2305161.230516

    1.2377121.237712

    1.2449081.244908

    1.2521041.252104

    1.25931.2593

    1.2664961.266496

    1.2736921.273692

    1.2808881.280888

    1.2880841.288084

    1.295281.29528

    1.3024761.302476

    1.3096721.309672

    1.3168681.316868

    1.3240641.324064

    1.331261.33126

    1.3384561.338456

    1.3456521.345652

    1.3528481.352848

    1.3600441.360044

    1.367241.36724

    1.3744361.374436

    1.3816321.381632

    1.3888281.388828

    1.3960241.396024

    1.403221.40322

    1.4104161.410416

    1.4176121.417612

    1.4248081.424808

    1.432004

    1.4392

    1.446396

    1.453592

    1.460788

    1.467984

    Right end of F1

    Left end of F2

    Distance from fibre break (mm)

    Interfacial shear stress (MPa)

    14.947664224

    17.8137669948

    15.420881365

    20.0987265496

    14.1760504122

    18.8341403649

    12.2513823809

    14.4426665422

    10.0192775612

    10.4192118281

    7.6515046905

    7.9026922007

    6.2687136118

    6.3902585892

    5.3299685951

    5.1190847294

    4.681935587

    3.9519989271

    4.1468688226

    3.276674982

    3.5631288343

    2.5448879222

    2.8903196717

    1.9744761267

    2.2285978192

    1.6669316785

    1.9420871601

    1.3116060747

    1.7488305662

    0.9201926538

    1.4417005655

    0.5341895007

    1.4656101749

    0.2476468525

    1.2501667055

    0.172571924

    1.1806930847

    0.1770517694

    0.8667238983

    0.178569812

    0.7760823827

    0.0456755991

    0.6909429733

    0.2700959246

    0.3478170286

    0.4779870602

    0.1153126959

    0.6008421138

    0.2491654543

    0.6008421138

    0.4890657035

    0.8213796678

    0.7442055825

    0.8369863033

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    0.8438696458

    0.7709044518

    0.9807260921

    0.9947739741

    1.3293383437

    1.3427708447

    1.4511498858

    1.7009174595

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    5.5388729499

    6.1632269242

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    5.6719200278

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    5.7790907715

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    6.1648755103

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    6.0783126813

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    5.9892460739

    6.7621441383

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    5.8217281964

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    5.5878639986

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    2.6624601407

    3.7733150795

    2.7148689414

    3.6507009991

    2.5033828044

    3.6034603774

    2.4478425046

    3.5770100223

    2.3655616199

    3.8781171075

    2.2381215852

    3.9511126807

    2.0931669844

    3.862038059

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    3.9371286097

    4.0146857398

    3.881420286

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    4.2706222267

    4.3236448179

    Sheet3

    Combined effect of transverse matrix crack and debonding at fibre-break (Al2O3 fibre)

    FM Zhao, FR Jones et al., Composites Part A 36 (2005) 229-244

    Crack tip

    Crack

    sapp = 16.08 MPa, eapp = 0.48%

    Debonded interface

    Bonded area

    Crack tip

    sapp = 13.10 MPa, eapp = 0.388%

    Crack

    Matrix

    1.67 mm

    1.00 mm

    Conclusions

    Automated phase-stepping polariscope has been used to measure the micro stress field in the matrix near a fibre-break and the interfacial shear stress for Al2O3 and E-glass fibre epoxy model composites

    Effect of a transverse matrix crack on stress transfer has been investigated by photoelasticity

    It has been found that the matrix crack can delay significantly stress transfer

    A soft interphase can be created, which controls the propagation of a transverse matrix crack

    The debonding at the fibre break can be detected accurately by photoelasticity

    Acknowledgements

    EPSRC for funding the research

    Photran Inc. (USA) for the supply of sapphire fibre and The Advanced Composites Group (UK) for supplying epoxy resins

    Prof K Schulte (Germany) for supplying E-glass fibre made by The Institute of Polymer Research Dresden.

    Prof EA Patterson for introducing the phase-stepping photoelastic technique

    Dr C Johnson,Mr H Sugihara and Mr Z Liu for coating E-glass fibres

    Dr Z Wang for technique support

    0

    10

    20

    30

    40

    50

    00.20.40.60.811.2

    Distance from fibre break (mm)

    Interfacial shear stress (MPa)

    14.37 MPa

    17.45 MPa

    0

    5

    10

    15

    20

    25

    30

    00.20.40.60.811.2

    Distance from fibre break (mm)

    Interfacial shear stress (MPa)

    8.56 MPa

    12.42 MPa

    17.63 MPa

    0

    4

    8

    12

    16

    20

    0.00.51.01.5

    Distance from fibre break (mm)

    Interfacial shear stress (MPa)

    0.5

    0.6

    0.7

    0.8

    0.9

    00.511.52

    Distance from fibre-break (mm)

    Interfacial fringe order

    1

    1.1

    1.2

    1.3

    1.4

    00.511.52

    Distance from fibre-break (mm)

    Interfacial fringe order

    0

    100

    200

    300

    400

    500

    600

    700

    800

    900

    0123456

    Distance from the fibre end (mm)

    Tensile stress in the fibre (MPa)

    No matrix crack

    0.1 mm matrix crack

    0.2 mm matrix crack

    0.4 mm matrix crack

    0

    0.1 mm

    0.2 mm

    0.4 mm

    0

    5

    10

    15

    20

    25

    30

    35

    40

    45

    00.20.40.60.81

    Distance from the fibre end (mm)

    Shear stress at fibre/matrix interface

    (MPa)

    No matrix crack

    0.1 mm matrix crack

    0.2 mm matrix crack

    0.4 mm matrix crack

    0

    5

    10

    15

    20

    25

    30

    35

    00.250.50.7511.251.5

    Distance from the fibre break (mm)

    shear stress at the fibre/matrix

    interface (MPa)

    Determined by photoelasticity

    Finite element prediction

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