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