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JPE - Sept09 - cover2-4.pmd - Pipes & Pipelines International ...

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152<br />

axis, due to the existence of the flaw, compared with<br />

the unflawed condition.<br />

• Global collapse: corresponds to failure, by yielding<br />

mechanisms, of the whole section containing the<br />

flaw. This is deemed to occur when the global<br />

deformation, displacement and/or rotation, of the<br />

section become unbounded. Global collapse occurs<br />

at a higher load than that corresponding to local<br />

collapse.<br />

Most codified limit-load or reference-stress solutions for<br />

part-thickness (surface or embedded) flaws are based on the<br />

local-collapse approach. Although some standards, such as<br />

R6 [2] also provide solutions based on the global-collapse<br />

approach, further checks, such as against finite-element<br />

analyses, may be required to verify that such solutions<br />

provide safe assessments.<br />

An alternative method for determining limit loads, which<br />

requires J data from finite-element analyses, consists of<br />

defining the limit load such that it is consistent with the J<br />

data and the reference stress J-estimation scheme represented<br />

by Equn 2. The main benefit of this approach is that it does<br />

not require the analyst to specify in advance whether a localor<br />

global-collapse model is more suitable. The limit load is<br />

found by solving Equns 2 and 3 using J results from an<br />

elastic-plastic finite-element analysis of the flawed<br />

component. A simple version of this approach is<br />

recommended in Section B.6.4.3(e) of API 579 [3] and in<br />

a slightly different form in Section B.1.89 of API-579-1/<br />

ASME-FFS-1 [4] as follows:<br />

L<br />

r<br />

t<br />

Fig.3. Idealized elliptical embedded flaw in a flat plate, used in BS 7910 (BSI, 2005).<br />

P<br />

=<br />

P<br />

ref<br />

where P ref is determined from the following relationship:<br />

(9)<br />

The Journal of Pipeline Engineering<br />

J 0.002E 1 ⎛ 0.002E⎞<br />

⎟<br />

= 1+ +<br />

⎜<br />

⎜1<br />

⎟<br />

Je σy 2<br />

⎜ + ⎟<br />

⎜⎝ σ ⎟ y ⎠<br />

P= Pref<br />

−1<br />

(10)<br />

where J is the total value of J determined from an elasticplastic<br />

analysis of the flawed component; J e is the elastic J<br />

determined from an elastic analysis by, for example, using<br />

Equns 4 or 5; P is a characteristic applied load (or stress)<br />

such as axial force, bending moment, or a combination<br />

thereof; and P ref is the reference load (or stress) defined as<br />

the load at which the ratio J/J e reaches the value defined by<br />

Equn 10.<br />

If P ref is used to construct a BS 7910 Level 3C FAD (with L r<br />

defined according to Equn 9), it will intersect the<br />

corresponding BS 7910 Level 2B/3B material-specific FAD,<br />

and give the same K r value, at L r = 1.0. Thus, the limit load<br />

P ref is defined in a manner which is consistent with the Level<br />

2B/3B material-specific FAD, at least at L r = 1.0. In this<br />

case, the limit load may depend on the strain-hardening<br />

characteristics of the material.<br />

Sample issue<br />

Codified reference-stress<br />

solutions for embedded flaws<br />

General<br />

Whereas there are several well-established reference-stress<br />

solutions for circumferential surface flaws in pipe girth<br />

welds, there are no such solutions for circumferential<br />

embedded flaws. Consequently, most analysts use referencestress<br />

solutions originally derived for flat plates to assess<br />

circumferential embedded flaws in pipe girth welds. The<br />

most widely used of these solutions are the reference-stress<br />

equations given in BS 7910 [1] and R6 [2]. These are given<br />

in terms of the membrane stress, P m , and through-wall

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