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an orthotropic continuum model for the analysis of masonry structures

an orthotropic continuum model for the analysis of masonry structures

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TNO-95-NM-R0712 1995 33The expl<strong>an</strong>ation <strong>for</strong> <strong>the</strong> over prediction <strong>of</strong> <strong>the</strong> failure load will now be detailed. Fig. 25a shows that<strong>the</strong> experimental load-displacement diagram is well reproduced until a horizontal displacement dequal to 1.0 mm, which coincides with <strong>the</strong> opening <strong>of</strong> <strong>the</strong> diagonal shear crack. After this point, itseems that <strong>the</strong> behaviour <strong>of</strong> <strong>the</strong> structure is not captured by <strong>the</strong> <strong>model</strong>. The crucial question iswhe<strong>the</strong>r <strong>the</strong> <strong>masonry</strong> macro-<strong>model</strong> here proposed is not acceptable or <strong>the</strong> <strong>model</strong>ling strategy isinadequate. The author believes <strong>the</strong> latter to be true.Fig. 24 clearly shows <strong>an</strong> extremely localized diagonal failure type in which all inelastic phenomenaconcentrate, basically, in a single stepped crack. A complete underst<strong>an</strong>ding <strong>of</strong> <strong>the</strong> behaviour <strong>of</strong> <strong>the</strong>structure is obtained by <strong>the</strong> distribution <strong>of</strong> internal <strong>for</strong>ces calculated by <strong>the</strong> micro-<strong>model</strong>, see Fig.33. Fig. 33a shows that, initially, <strong>the</strong> direction <strong>of</strong> <strong>the</strong> compressive strut is determined by <strong>the</strong> geometry<strong>of</strong> <strong>the</strong> bricks <strong>an</strong>d deviates from <strong>the</strong> strut direction found in <strong>the</strong> macro-<strong>an</strong>alysis. The discrep<strong>an</strong>cybetween <strong>the</strong> micro- <strong>an</strong>d macro-<strong>model</strong> gets only larger under increasing de<strong>for</strong>mation. Fig. 33bshows that in reality two independent struts occur once <strong>the</strong> diagonal crack is fully open <strong>an</strong>d a welldeÞned b<strong>an</strong>d completely unloads, with approximately <strong>the</strong> width <strong>of</strong> a brick at <strong>the</strong> center <strong>of</strong> <strong>the</strong> specimen.This phenomenon c<strong>an</strong>not be captured by a (smeared) macro-<strong>model</strong> unless some internallength scale, that reßects <strong>the</strong> <strong>masonry</strong> micro-structure, is incorporated in <strong>the</strong> <strong>model</strong>. This problemis outside <strong>the</strong> scope <strong>of</strong> <strong>the</strong> present report <strong>an</strong>d, presently, no simple solution is envisaged. It is notedthat <strong>the</strong> task is quite complex because it is not clear yet if <strong>the</strong> above length scale is a geometricalproperty dependent on <strong>the</strong> unit size or a structural property that depends on <strong>the</strong> micro-structure,geometry <strong>of</strong> <strong>the</strong> structure <strong>an</strong>d loading conditions.a) d = 1.0 mm d) d = 4.0 mmFig. 33 - Minimum principal stresses <strong>for</strong> a horizontal displacement d obtained by a micro-<strong>model</strong>Louren•o (1994)For <strong>the</strong> sake <strong>of</strong> completeness a new <strong>an</strong>alysis is carried out with <strong>the</strong> macro-<strong>model</strong> <strong>for</strong>mulated insuch a way that degradation <strong>of</strong> tensile strength induces degradation <strong>of</strong> compressive strength, i.e. acoupled <strong>model</strong>. Coupling is introduced via <strong>an</strong> equation <strong>of</strong> <strong>the</strong> following type:

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