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Aluminium Design and Construction John Dwight

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The effective section is obtained by replacing the area Az of the<br />

nominal HAZ in each softened region by an effective area kzAz . The<br />

effective section properties may then be found by one or other of the<br />

following methods (refer also to Sections 10.2.4, 10.3.4):<br />

1. Method 1. An effective plate thickness of kzt is generally assumed in<br />

each nominal HAZ region, instead of the true thickness t. In thick<br />

material, such that the nominal HAZ penetration s is less than t, the<br />

effective thickness is taken equal to {t-s(1-kz )}. The properties of the<br />

effective section thus obtained are then determined in the usual way.<br />

2. Method 2. The section properties are first calculated with HAZ softening<br />

ignored, <strong>and</strong> suitable deductions then made corresponding to a ‘lost<br />

area’ of Az (1–kz ) at each HAZ.<br />

Method 2 is generally preferred for members just containing small<br />

longitudinal welds, since it only involves A z which is readily found<br />

(equation (6.6)), without the need to know the exact location of the<br />

softened metal.<br />

For any given material there are in general three possible k z -values<br />

(see Section 6.4.1). The first two of these are needed for member design<br />

<strong>and</strong> are selected as follows:<br />

k z1 shear force resistance in beams (Section 8.3);<br />

local failure in tension <strong>and</strong> compression members (Section 9.3).<br />

k z2 moment resistance in beams (Section 8.2);<br />

general yielding in tension members (Section 9.4);<br />

overall buckling (Sections 8.7.4, 9.5, 9.6).<br />

In service, the strains arising in the softened zones at a partially welded<br />

cross-section are the same as those in the adjacent unsoftened material.<br />

With the above method of calculation therefore, using an effective section,<br />

the HAZ material will yield prematurely—well before the calculated<br />

resistance of the member is reached, <strong>and</strong> possibly even at working<br />

load. Some inelastic deflection therefore takes place, leading to a slight<br />

permanent set after the first loading. This does not matter, since the<br />

component will behave elastically under further load applications, <strong>and</strong><br />

the inelastic deflection is small. (A similar state of affairs exists with<br />

steel members, where premature yielding occurs in parts of a section<br />

due to the very considerable locked-in stresses present in all steel<br />

components—much worse than in aluminium.)<br />

6.6.2 <strong>Design</strong> of joints<br />

In determining the resistance of a load transmitting joint, two calculations<br />

are generally needed: one for failure of the actual weld metal, <strong>and</strong> one<br />

for failure in the fusion zone—see Section 11.3. The latter refers to a<br />

Copyright 1999 by Taylor & Francis Group. All Rights Reserved.

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