StructuralAnalysesOfJack-upsInElevatedCondition

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    Properties of Jack-ups in elevated condition

    Stiffness Hull is stiff

    Legs relative soft

    Masses

    hull mass is high

    leg mass relative small

    Percent critical damping e

    Soil 0% 2%

    Hydrodynamic 2% - 3%

    Material/Friction 0%

    2%

    Total: often 7% assumed

    Natural Periods:

    between 4s und 10s

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    Modal analysisTranseverse and Longitudinal Modes

    Thormodal_wd-50_he9_r0-quer.avi

    Transverse Longitudinal

    Thormodal_w d-50_he9_r0-laengs.av i

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    Loads in a global analysis

    constant, quasi-constant Loads

    Weights

    Crane

    Wind

    CurrentTime varying loads

    Waves

    (irregular sea with varying wave

    periods and wave heights)

    Wave periods between 4s-18s

    RESONANCE possible

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    Method for dynamic analyses of jack-ups (1/2)

    Determination of DAF (DynamicAmplification Factor) due to wave excitation

    Comparison with a single degree of freedom

    system (SDOF) or

    Statistial assessment of the reponses of the

    jack-up due to time history wave loads (1-3hours simulation time of qualified seastate)

    Defintion:

    DAF=Fdynamic/Fstatic

    =(Fstatic+Finertia)/Fstatic,,i.e.

    Finertia=(DAF-1)* Fstatic

    22

    2

    21

    1

    T

    Te

    T

    T

    DAF

    nn

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    Method for dynamic analyses of jack-ups (2/2)

    Base Shear BS is the total

    horizontal load at reaction point

    BSmax=1500 kN

    BSmin=-800 kN

    BSamp=(BSmax-BSmin)/2= 1150 KN

    BSmean=(BSmax+BSmin)/2

    = 350 KN

    Inertia Load:

    Finertia=BSamp*(DAF-1) acting at

    CoG or distributed over the

    legs

    Wave according WAVEL

    -1000

    -500

    0

    500

    1000

    1500

    2000

    0 45 90 135 180 225 270 315 360 405 450 495 540

    Phase [Deg]

    Force [kN]

    -2.000

    -1.500

    -1.000

    -0.500

    0.000

    0.500

    1.000

    1.500

    2.000

    Elevation [m]

    Wave Load Contour [kN] Wave Elevat ion [m]

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    Morison equation (empirical formula for hydrodynamic loads on cylindrical member)

    Fd= Drag force

    Fm= Inertia forcer= Density of water

    D = Reference diameter of cylindrical member

    A = Total cylindrical area of member

    Cd= Drag coefficient

    Cm= Mass coefficientv = relative particle velocity normal to member axis ( v~H/2*w*sin[wt-a] + vcur)

    u = relative particle acceleration normal to member axis ( u~H/2*w**2*cos[wt-a] )

    Wave loads on transparent Structures

    uCAvvCDF

    FFF

    md

    md

    2

    1

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    Total Loads and non-linear Effects

    Total Load on a Wind Turbine Installation Vessel

    F = FGravity+ FCrane+ FWind+ FWave/Current+ FInertia

    All Loads are depend on load directions except gravity

    Non-linear effects at spud can reaction point due to non-linear soil condition

    wave loads according to drag term of Morison equation

    P-Deffect on legs (equilibrium at deformed shape)

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    References:

    Society of Naval Architects & Ocean Engineers (SNAME):

    Technical & Research Bulletin 5-5A

    Guidelines for Site Specific Assessment of Mobile Jack-up

    Units, Rev.3 2008

    and

    ISO 19905-1 and ISO 19905-2

    Site Specific Assessment of Mobile offshore units

    Thank you

    Thomas Jahnke, Tel: +49 40 36149 106

    Jochen Knzel, Tel: +49 40 36149 7424