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    FINAL SUMMARY

    High grade strength plate steels were used to improve their applications in EU obtain advantages to the

    overall stiffness of the decks as well as their fatigue resistance. The yield strengths of the steels were in

    the range 4601100 MPa.

    The application of these products were focalised to design and to produce conventional and sandwich

    panels in ship as well as for bridge application.

    In order to met the objectives the project were articulated in the follow tasks:

    - To define the procedures to design, by geometrical parametric inputs, conventional and sandwichdecks.

    - To investigate the fatigue behaviour of the shape of welding joints, by specimens, and to comparethe results to Eurocode 3.

    - To identify the methods for manufacturing heavy sandwich panels and the related weldingprocedure for laser joints.

    - To manufacture conventional panels directly in shipyards in order to obtain industrial products asreference.

    - To manufacture sandwich panel by laser welded joints. Two grades of steel plates (460 and 1100MPa) were selected.

    - To test the conventional and sandwich panels in order to compare with EC3 and to verify theimprovement of their reduction of weight, the increasing both of the stiffness and the fatigue

    behaviour

    Materials

    In order to manufacture conventional and sandwich decks the selection of plates were done in term

    both of thickness and of grade.

    The plates was delivered by Fincantier (Italian shipyards) and produced by ThyssenKrupp Nirosta

    GmbH (Germany) and from Corus (UK)

    Steel Grade YS

    [MPa]

    Thickness [mm] Supplier

    355 8

    560 16

    690 8

    690 12690 16

    690 30

    1100 8

    355 2

    FINCANTIERI

    (TKS)

    355 8

    460 8

    690 8

    355 2

    CORUS

    3

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    Design

    Conventional decks, with upper skin of th=16mm, and grades S560 and S690 MPa were designed by

    FEA. The parameters used to optimise the weight and the stiffness was: bulb area (web thickness and

    height) and web numbers. The minimum deflection obtained applying a medium load was: thickness

    = 10mm, height=275mm, number of web number N=3. A number of 11 conventional decks (in

    particular 5 were in grade S560 and 6 in grade 690 and reinforced bulb in grade S355) were

    manufactured ready to submit under fatigue tests. The dimension of each the conventional panel was:

    length L= 3000mm, width W=1500 mm, height H= 275mm, weight P=800kgm.

    Sandwich decks were designed by 2D. After the valuation of the results the design was improved by a

    3D FEM.

    The objective of the model was to minimize the buckling of the

    corrugate elements as well as the deflection of the panel. The

    parameters used to obtain the expected results were: the shape and

    the size of the corrugate element in term of: thickness, web/plate

    angle, wave length and height.

    Optimised dimensions of the sandwich decks were obtained also

    taking into account the manufacturing problems to weld, by laser

    plant, the internal corrugate elements to upper and lower skin

    plates.

    The dimensions of the corrugate internal parts are reported in the sketch on the right, where the

    thickness of the sheet S355was th=2mm and the upper plates (S1100) and lower plates (S355) was

    th=8mm.

    Welded Joints

    All the shapes (figures) of the welded joints useful to manufacture conventional and sandwich decks

    were manufactured in order to investigate their fatigue resistance and compared with the requirements

    of Eurocode 3.

    For conventional decks MAG, SAW and SMAW welding procedure were considered as well as butt

    and T-Butt joint. Welded joint plates of dimension 1000x1000mm were manufactured directly in

    shipyard in order to test true industrial production.

    Specimens of with W100mm and length L500mm were machined from welded plates and submitted

    under fatigue tests. Fatigue tests were carried out in constant and variable amplitude in order to obtain

    both the Whler and Ganer curves.

    Moreover the notch effect of the welded line was evaluated as well as the real damage. All test data

    clearly are on the safe side. Compared to the experimental data derived from the tests, Eurocode3

    seams to be conservative.

    For sandwich decks laser welding procedure was defined and two shape of spare welded joints

    specimens were investigate as follows::

    Laser welded joints were cut from welded plates manufactured in four series with different grade of

    upper and lower plates:

    TypeA:RD1100/RD355 (Series 2)

    TypeA:RD355/RD355 (Series 3) TypeB:RD355/RD355 (Series 4) TypeB:RD1100/RD355 (Series 1)

    4

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    First Material specification describes thick plate material plate material (th=8mm), second material

    description describes corrugate thin sheet material (th=2mm). Type B specimens are specimens

    welded from the thick plate side to the thin sheet. For Type A specimens the thin sheet is welded to

    the plate from the thin sheet side.

    These specimens were submitted under axial loading with constant and variable amplitude in order to

    derive Whler and Ganer curves as well as the real damage.

    The results lead to define appropriate FAT classes for laser welded specimens Type A and Type B,

    as these details are not listed in Eurocode tables.

    Possible classification for Type A was:

    FAT 36 : Transverse butt weld, welded from one side without backing, full penetration (t region, thus crack initiation sites are decided by the localnotch factor value only. This behavior presumes a very severe residual stress state in the weld zone.

    The unusual failure behaviour at higher load levels could have different explanations, the easiest onebeing related to the uncertainties in notch factor evaluation: specimens E13, E15, E17and E21 could

    without difficulty have different geometrical features with respect to the others (it has to be

    remembered that only two E specimens have been measured, and both have not been tested).

    The distortion of E series specimens could also play a role. As pointed out above, the E series

    specimens are quite distorted around the weld axis (up to 5) due to the welding procedure; since the

    stress flux lines inside the specimen tend to follow the shortest path, evidently weld notches on one

    side are less stressed (so on the other side theyre more stressed) with respect to the no distortion

    condition.

    The influence of the curvature on the notch factors has been investigated through a plane FEM model

    reproducing the butt weld cross section; r/20 has been adopted as minimum element size in the highly

    stressed regions. The actual test configuration of the E specimens and a curvature equal to 5 have been

    taken into account: in this conditions the top-right and the bottom right notch factors are respectively

    +5% higher and -10% lower then the ideal situation, thus such notch factors are closer if the actual

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    shape of the specimens is considered. Figure 93 shows the FEM results for two equal notches in terms

    equivalent stresses of acc.to von Mises (in plane stress conditions such a stress is equal to the first

    principal stress in the tensile area, and to the third principal stress in the compressive area): the top and

    bottom highly stressed areas evidently experience different stress levels (the reference value of the

    notch factor is 3.20).

    Since the weld geometry is measured in the actual condition, the distortion is already taken into

    account, thus the curvature effect can be perhaps better considered as a fictitious increment and/ordecrement of the nominal stress.

    In Figure 94 the SN curves are shown in terms of local stress amplitude, that is obtained multiplying

    the nominal stress amplitude for the stress concentration factor related to the initiation notch. The three

    original SN curves in terms of nominal stresses can be evidently transformed to one common curve (the

    local fatigue strength ranges between 278 MPa and 287 MPa for R=0). In the knee point area the

    scatter is high, mainly due to the SMAW series, which is scattered in itself.

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    Figure

    84-Notchradiusstatisticaldistr

    ibutionfor

    MAGSeries.

    Figure85-Notchanglestatisticaldistributionfo

    r

    MAGSeries.

    Figure86-Notchradiusstatisticaldistributionfor

    SAWSe

    ries.

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    Figure8

    7-Notchanglestatisticaldistribu

    tionforSAW

    Series.

    Figure88-Notchradiusstatisticaldistributionf

    or

    SMAWSeries.

    Figure89-Notchanglest

    atisticaldistributionfor

    SMAWSeries.

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    Figure90-Notchfactorstatisticaldistributionfor

    MAGSeries.

    Figure91-Notchfactorstatisticaldistributionfor

    SAWSeries.

    Figure92-Notchfactorst

    atisticaldistributionfor

    SMAWSeries.

    93

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    Figure 93 - Local equivalent stress acc. to Von Mises calculated by FEM.

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    10

    4

    2

    4

    6

    810

    5

    2

    4

    6

    810

    6

    2

    4

    6

    810

    7

    2

    100

    100

    200

    300

    400

    500

    600

    700

    800

    900

    1000

    1000

    MAG:

    Gasmetalarcwelding

    SAW

    :

    Submergedarcwelding

    SMAW

    :Shieldedmetalarcwelding

    287

    _

    _

    P

    =50%

    T=

    1:1.35

    Specim

    en

    TypeC

    Fig16_Fat_test_local_280186.

    OPJ

    Fatigue

    Strength

    of

    Buttw

    elds

    Fig.8

    LBF280186

    MPa

    k=

    3.5

    Localstressamplitudea,n,a,n

    CyclestoruptureNr,Nr

    Material:

    S690QL

    Geometry:

    Buttweld

    Thickness:

    30mm

    Load:

    Bending

    Ratio:

    R

    =0

    Constantamplitude

    CA

    .MA

    G

    MAG

    CA

    .SAW

    SAW

    CA

    .SMAW

    SMAW

    Figure94-Fatiguestrengthofbu

    ttweldsintermsoflocalstressamplitude.

    95

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    respectively the actual endurance and the endurance expected Test results and Eurocode3: comparison

    The real damage sum has been calculated for butt welds subjected to variable amplitude loading tests.

    Such calculation has been performed according to the procedure illustrated in Figure 95. Partial

    damages are evaluated starting from the relevant Whler curve, and summed up to cover the actual

    operating life of the specimen.

    Values of Dreal are reported in Table 29: The fact that the real damage is significantly higher then 1

    has strongly to be noted.

    Such a result is expressed differently in Figure 96 where the Ganer curves (Pf=50%) are calculated in

    order to obtain D=1; for damage calculations Whler curves slope after the knee point is assessed by

    Haibachs recommendation for welded steel:

    1k2k =' (14)Evidently the specimens endure longer then expected making reference to a damage sum equal to one,

    even if E series is quite close to the relevant Ganer curve.

    In Figure 97 test results and curves suggested by Eurocode3 (latest version available: April 1992) are

    shown and compared.

    Eurocode3 design curves are ideally divided into three segments according to fatigue life ranges: for

    normally loaded welds, up to 5 million cycles the slope is k=3, between 5 million cycles and 100

    million cycles the slope becomes k=5, after 100 million cycles the inclination becomes null (cut offlimit). Every curve is so completely determined if the FAT Class is known: the FAT Class corresponds

    to the nominal stress range at 2 million cycles, and its value in MPa depends on the weld geometry and

    loading. Design curves refer to 2,3% of probability of rupture, i.e. 2 standard deviations less then the

    mean value; it has also to be noted that Eurocode3 expresses Whler curve in terms of nominal stress

    range , and not nominal stress amplitude.

    Butt welds pertain to the FAT90 Class, so fatigue strength in terms of nominal stress amplitude at 2

    million cycles is 45 MPa. In Figure 97 fatigue strength of Eurocode3 design curve is not exactly 45

    MPa, but 43 MPa, since Eurocode3 suggests the following multiplying factor in order to take into

    account the thickness effect:

    25025

    ,

    tRjR.tj

    =

    (15)

    Whler curves obtained by tests refer to 2.3% probability of rupture in order to perform the

    comparison. Clearly the SN curve suggested by Eurocode3 is well suitable to be used for safe design of

    butt welds in consideration.

    Figure 97 shows the Ganer curves for the three specimens series and for Eurocode3 as well: each one

    is evaluated for D=1, and refers to 2.3% of probability of rupture. Derived slopes are k=3.6 and k=3

    respectively.

    The results illustrates above are condensed in Figure 98, 99 and 100: for each diagram the abscissa and

    the ordinate arefor a damage sum equal to 1.

    If D=1 is the underlying design condition, Eurocode3 provides very conservative results.

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    Modificationo

    ftheS-N-Curveand

    CalculationofFatig

    ueLife

    (schematical)

    DIA4784e

    i=1:steel,

    aluminium

    i=2:cast

    andsintered

    materials

    exper.

    s

    .

    spec

    real

    real

    .

    spec

    s

    calc.

    N

    LD

    D

    D

    DL

    N

    =

    =

    .

    calc

    N

    k'=2k-i

    Cumulativefre

    quency

    distribution(sp

    ectrum)

    Woehlercurve

    Gassnercurve

    slope k

    Dam

    agesumofthespectrum:

    n1

    n2

    n3

    n4

    Ls

    N k

    .

    Spec

    n1

    i

    ii

    D

    Nn

    =

    =

    1

    2

    3

    4

    N1

    N2

    N3

    N4

    max

    ,a

    Stressamplitudea,a

    k(kneepoint)

    Cy

    clesN,N

    k'=k

    Figure95-Procedureforassessingtherealdamagesum

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    Nominal

    stress

    amplitude

    (ideal)

    Cycles to

    rupture

    Real

    Damage

    Sum

    Spec.No.

    SheetNo.

    Test

    #)

    Stressratio

    [MPa] Nr, r

    F4 F1-F9 VA 0 360 947500 3,33

    F7 F1-F9 VA 0 360 808000 2,84

    F3 F1-F9 VA 0 300 1704000 3,14

    F6 F1-F9 VA 0 300 1283000 2,36

    F2 F1-F9 VA 0 250 4617200 4,42

    F5 F1-F9 VA 0 250 2746000 2,63

    AS5 AS1-AS12 VA 0 520 633054 4,47

    AS7 AS1-AS12 VA 0 520 274539 1,94

    AS2 AS1-AS12 VA 0 430 1255000 4,54

    AS8 AS1-AS12 VA 0 430 734653 2,66

    AS4 AS1-AS12 VA 0 360 5330075 10,29

    AS6 AS1-AS12 VA 0 360 1587005 3,06

    E5 E1-E9 VA 0 360 1061000 1,41

    E1 E1-E9 VA 0 360 1093000 1,45

    E6 E1-E9 VA 0 300 1700000 1,16

    E3 E1-E9 VA 0 300 2505000 1,71E4 E1-E9 VA 0 250 3212000 1,09

    E7 E1-E9 VA 0 250 3232000 1,10

    Table 29 - Real damage sums for butt welds.

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    6

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    6

    2

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    810

    7

    2

    60

    80

    100

    100

    200

    300

    400

    500

    600

    k=3.7

    k=6

    k=3.8

    k=3.7

    100 9

    0

    _

    _

    P

    =50%

    T=1:1.35

    SpecimenTypeC

    Fig18

    _D

    _calc

    _butt

    _280186.

    OPJ

    runo

    ut(withoutfailure)

    retes

    tedatahigherlevel(broken)

    GassnerCurves(D

    =1)andVariableAmplitudeLoadingTe

    stResults:compar

    ison

    Fig.xxx

    LBF

    280186

    76

    MPa

    k=3.5

    Nominalstressamplitudea,n,a,n

    Cyclestorupture

    N r,N r

    Material:

    S690QL

    Geometry:

    Buttweld

    Thickness:

    30mm

    Load:

    Bending

    Ratio:

    R=0

    TestResults(ConstantAmplitude

    )

    CA.MAG

    CA.SAW

    CA.SMAW

    TestResults(Gauss,L

    s,G

    =5104 )

    VA.MAG

    VA.SAW

    VA.SMAW

    WhlerandGassner(D=1)Curve

    s

    MAG

    SAW

    SMAW

    Figure96-GanercurvescalculatedforD=1.

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    6

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    7

    2

    2020

    40

    60

    80

    100

    100

    200

    300

    400

    500

    600

    k=3,6

    k=

    6

    k=3,5

    k=3

    436

    0

    k

    =5

    Material:

    S690QL

    Geometry:

    Buttweld

    Thickness:

    30mm

    Load:

    Bending

    Ratio:

    R=0

    ConstantAmplitudeand

    VariableAmplitude(Gauss,Ls

    ,G

    =510

    4)

    LoadingTests:Results

    CA.MAG

    V

    A.MAG

    CA.SAW

    V

    A.SAW

    CA.SMAW

    V

    A.SMAW

    WhlerandGaner(D=1)Cur

    ves

    MAG

    SAW

    SMAW

    Eurocode3

    79

    71

    _

    _

    P

    =2

    ,3%

    T=1:1.35

    SpecimenTypeC

    Fig19_D_calc_butt_280186.OPJ

    runo

    ut(withoutfailure)

    retes

    tedatahigherlevel(broken)

    Eurocode3(D=1)andVariableAmplitudeLoadingTestResu

    lts:comparison

    Fig.xx

    LBF280186

    32

    MPa

    k=

    3

    Nominalstressamplitudea,n,a,n

    CyclestoruptureNr

    ,Nr

    Figure97-GanercurvescalculatedforD=1.

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    10

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    105

    10

    6

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    7

    Dreal1

    D=

    1,Pf=

    50%

    MAG

    CyclesexpectedforD=1

    10

    4

    10

    5

    10

    6

    10

    7

    10

    4

    10

    5

    10

    6

    10

    7

    Dreal1

    D=

    1,Pf=

    50%

    SAW

    Cyclestorupture

    10

    4

    10

    5

    106

    10

    7

    10

    4

    10

    5

    10

    6

    10

    7

    D=

    1,Pf=

    50% D

    real>1

    Dreal1

    Dreal1

    D=

    1,Pf=

    2,3%

    SAW

    Cyc

    lestorupture

    10

    4

    10

    5

    10

    6

    10

    7

    10

    4

    10

    5

    10

    6

    10

    7

    Dreal1

    Dreal1

    Dreal1

    D=

    1,Pf=

    2,3%

    SAW

    C

    yclestorupture

    10

    4

    10

    5

    10

    6

    10

    7

    10

    4

    10

    5

    10

    6

    10

    7

    Dreal1

    Dreal