Clasification Society Rulefinder 2020 - Version 9.33 - Fix
Common Structural Rules - Common Structural Rules for Bulk Carriers and Oil Tankers, January 2019 - Part 1 General Hull Requirements - Chapter 5 Hull Girder Strength - Appendix 2 Hull Girder Ultimate Capacity - 2 Incremental-Iterative Method |
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![]() 2 Incremental-Iterative Method2.1 Assumptions 2.1.1 In applying the procedure described in [2.2], the following
assumptions are generally to be made:
These elements are:
These curves are to be calculated, for the failure mechanisms of the element, from the formulae specified in [2.2]. The stress, σ is selected as the lowest among the values obtained from each of the considered load-end shortening curves σ-ε. The procedure is to be repeated until the value of the imposed curvature reaches the value χF in m-1, in hogging and sagging condition, obtained from the following formula: where: MY : Lesser of the values MY1 and
MY2, in kNm.
If the value χF is not sufficient to evaluate the peaks of the curve M-χ, the procedure is to be repeated until the value of the imposed curvature permits the calculation of the maximum bending moments of the curve. 2.2 Procedure 2.2.1 General The curve M-χ is to be obtained by means of an incremental-iterative approach, summarised in the flow chart in Figure 1. In this procedure, the ultimate hull girder bending moment capacity, MU is defined as the peak value of the curve with vertical bending moment M versus the curvature χ of the ship cross section as shown in Figure 1. The curve is to be obtained through an incremental-iterative approach. Each step of the incremental procedure is represented by the calculation of the bending moment Mi which acts on the hull transverse section as the effect of an imposed curvature χi. For each step, the value χi is to be obtained by summing an increment of curvature, Δχ to the value relevant to the previous step χi-1. This increment of curvature corresponds to an increment of the rotation angle of the hull girder transverse section around its horizontal neutral axis. This rotation increment induces axial strains, ε in each hull structural element, whose value depends on the position of the element. In hogging condition, the structural elements above the neutral axis are lengthened, while the elements below the neutral axis are shortened, and vice-versa in sagging condition. The stress σ induced in each structural element by the strain ε is to be obtained from the load-end shortening curve σ-ε of the element, which takes into account the behaviour of the element in the non-linear elasto-plastic domain. The distribution of the stresses induced in all the elements composing the hull transverse section determines, for each step, a variation of the neutral axis position, since the relationship σ-ε is non-linear. The new position of the neutral axis relevant to the step considered is to be obtained by means of an iterative process, imposing the equilibrium among the stresses acting in all the hull elements. Once the position of the neutral axis is known and the relevant stress distribution in the section structural elements is obtained, the bending moment of the section Mi around the new position of the neutral axis, which corresponds to the curvature χi imposed in the step considered, is to be obtained by summing the contribution given by each element stress. The main steps of the incremental-iterative approach described above are
summarised as follows (see also Figure 1):
2.2.2 Modelling of the hull girder cross section Hull girder transverse sections are to be considered as being constituted by the members contributing to the hull girder ultimate strength. Sniped stiffeners are also to be modelled, taking account that they do not contribute to the hull girder strength. The structural members are categorised into a stiffener element, a stiffened plate element or a hard corner element. The plate panel including web plate of girder or side stringer is idealised into either a stiffened plate element, an attached plate of a stiffener element or a hard corner element. The plate panel is categorised into the following two kinds:
Figure 2 : Extension of the breadth of the attached plating and hard corner element ![]() The typical examples of modelling of hull girder section are illustrated in Figure 3 and Figure 4. Notwithstanding the foregoing principle, these figures are to be applied to the modelling in the vicinity of upper deck, sheer strake and hatch side girder. Figure 3 : Examples of the configuration of stiffened plate elements, stiffener elements and hard corner elements on a hull section ![]()
Figure 4 : Extension of the breadth of the attached plating and hard corner element ![]() Figure 5 : Plating with knuckle point ![]() Figure 6 : Element with different thickness and yield strength ![]() 2.3 Load-end shortening curves 2.3.1 Stiffened plate element and stiffener element Stiffened plate element and stiffener element composing the hull girder
transverse sections may collapse following one of the modes of failure specified in
Table 1.
Table 1 : Modes of failure of stiffened plate element and stiffener element
2.3.2 Hard corner element The relevant load-end shortening curve σ-ε is to be obtained for lengthened and shortened hard corners according to [2.3.3]. 2.3.3 Elasto-plastic collapse of structural elements The equation describing the load-end shortening curve σ-ε for the elasto-plastic collapse of structural elements composing the hull girder transverse section is to be obtained from the following formula, valid for both positive (shortening) and negative (lengthening) strains, see Figure 7: σ = Φ ReHA where: ReHA : Equivalent minimum yield stress, in
N/mm2, of the considered element, obtained by the following formula:
Φ : Edge function, equal to:
ε : Relative strain, equal to:
εE : Element strain. εY : Strain at yield stress in the element, equal to:
Figure 7 : Load-end curve σ-ε for elasto plastic collapse ![]() 2.3.4 Beam column buckling The equation describing the load-end shortening curve σCR1-ε for the beam column buckling of stiffeners composing the hull girder transverse section is to be obtained from the following formula, see Figure 8: where: Φ : Edge function, as defined in [2.3.3]. σC1 : Critical stress, in N/mm2, equal to:
ReHB : Equivalent minimum yield stress, in
N/mm2, of the considered element, obtained by the following formula:
ApEl-n50 : Effective area, in cm2, equal to:
ε : Relative strain, as defined in [2.3.3]. σE1 : Euler column buckling stress, in N/mm2,
equal to:
IE-n50 : Net moment of inertia of stiffeners, in cm4, with attached plating of width bE1. AE-n50 : Net area, in cm2, of stiffeners with attached plating of width bE. bE1 : Effective width corrected for relative strain, in m,
of the attached plating, equal to:
βE: ApE--n50 : Net sectional area, in cm2, of
attached plating of width bE, equal to:
bE : Effective width, in m, of the attached plating, equal
to:
Figure 8 : Load-end shortening curve σCR1-ε for beam column buckling ![]() 2.3.5 Torsional buckling The equation describing the load-end shortening curve σCR2-ε for the flexural-torsional buckling of stiffeners composing the hull girder transverse section is to be obtained according to the following formula, see Figure 9. where: Φ : Edge function, as defined in [2.3.3]. σC2 : Critical stress, in N/mm2, equal to:
σE2 : Euler torsional buckling stress, in N/mm2, taken as σET in Ch 8, Sec 5, [2.3.4] ε : Relative strain, as defined in [2.3.3]. σCP : Buckling stress of the attached plating, in
N/mm2, equal to:
βE : Coefficient, as defined in [2.3.4]. Figure 9 : Load-end shortening curve σCR2-ε for flexural-torsional buckling ![]() 2.3.6 Web local buckling of stiffeners made of flanged profiles The equation describing the load-end shortening curve σCR3-ε for the web local buckling of flanged stiffeners composing the hull girder transverse section is to be obtained from the following formula: where: Φ : Edge function, as defined in [2.3.3]. bE : Effective width, in m, of the attached shell plating, as defined in [2.3.4]. hwe : Effective height, in mm, of the web, equal to:
βw : ε : Relative strain, as defined in [2.3.3]. 2.3.7 Web local buckling of stiffeners made of flat bars The equation describing the load-end shortening curve σCR4-ε for the web local buckling of flat bar stiffeners composing the hull girder transverse section is to be obtained from the following formula, see Figure 10: where: Φ : Edge function, as defined in [2.3.3]. σCP : Buckling stress of the attached plating, in N/mm2, as defined in [2.3.5]. σC4 : Critical stress, in N/mm2, equal to:
σE4 : Local Euler buckling stress, in N/mm2,
equal to:
ε : Relative strain, as defined in [2.3.3]. Figure 10 : Load-end shortening curve σCR4-ε for web local buckling ![]() 2.3.8 Plate buckling The equation describing the load-end shortening curve σCR5-ε for the buckling of transversely stiffened panels composing the hull girder transverse section is to be obtained from the following formula: where: Φ : Edge function, as defined in [2.3.3]. βE : s : Plate breadth, in m, taken as the spacing between the stiffeners.
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