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Bursting and Spalling in Pretensioned U-Beams - Ferguson ...

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3.2.1.1 L<strong>in</strong>ear <strong>and</strong> Nonl<strong>in</strong>ear Stress DistributionsWith<strong>in</strong> the end region of a prestressed concrete beam, concentrated prestress<strong>in</strong>gforces spread to the entire beam cross section. At some distance from the beam end, the<strong>in</strong>ternal stresses become distributed l<strong>in</strong>early, there conform<strong>in</strong>g to one of the basic tenetsof beam theory: the Bernoulli-Navier assumption that “plane sections rema<strong>in</strong> plane.”Closer to the end, however, the state of stress is “disturbed” (i.e. nonl<strong>in</strong>ear). Strut-<strong>and</strong>-tietheory (Schlaich, Schäfer & Jennewe<strong>in</strong>, 1987) refers to regions with l<strong>in</strong>ear stressdistributions as B-regions, after Beam theory or <strong>in</strong> honor of Bernoulli; <strong>and</strong> regions withnonl<strong>in</strong>ear stress distributions as D-regions, after the Disturbed state of stress.Strictly speak<strong>in</strong>g, no hard l<strong>in</strong>e divides D-regions from B-regions. Elastic analysisof a post-tensioned beam (Figure 3.1) shows the gradual transition to a l<strong>in</strong>ear stressdistribution. In this figure, the stress distribution is l<strong>in</strong>ear where the stress trajectories areparallel, or about a distance h from the end of the beam as predicted by Sa<strong>in</strong>t-Vénant’spr<strong>in</strong>ciple.hhFigure 3.1 Elastic stress trajectories <strong>in</strong> a post-tensioned concrete beam, illustrat<strong>in</strong>gthe division <strong>in</strong>to D- <strong>and</strong> B-regions (after Schlaich, Schäfer & Jennewe<strong>in</strong>, 1987)98

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