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1178 SATYANADHAM ATLURI<br />

Incremental <strong>for</strong>mulati<strong>on</strong>s <strong>of</strong> <strong>finite</strong> displacement large-strain problems, using a compatible<br />

displacement <strong>finite</strong> <strong>element</strong> <strong>model</strong>, have also been presented by H<strong>of</strong>meister et al.<br />

[17j, Pian and T<strong>on</strong>g [f$], Stricklin et al. [19] and Washizu [20]. A significant c<strong>on</strong>clusi<strong>on</strong><br />

in Refs. [17, 191 was that a “check” <strong>on</strong> <strong>the</strong> equilibrium in <strong>the</strong> current reference state prior<br />

to <strong>the</strong> additi<strong>on</strong> <strong>of</strong> a fur<strong>the</strong>r load increment was indispensible <strong>for</strong> obtaining meaningful<br />

computati<strong>on</strong>al results in an <strong>incremental</strong> <strong>for</strong>mulati<strong>on</strong> <strong>of</strong> large strain, n<strong>on</strong>linear problems.<br />

Since, as discussed by Pian [15], <strong>the</strong> <strong>hybrid</strong> assumed <strong>stress</strong> <strong>finite</strong> <strong>element</strong> <strong>model</strong> has<br />

proved to be a more versatile structural tool, it is <strong>the</strong> purpose <strong>of</strong> <strong>the</strong> present note to present<br />

a c<strong>on</strong>sistent variati<strong>on</strong>al <strong>for</strong>mulati<strong>on</strong> <strong>of</strong> <strong>the</strong> <strong>hybrid</strong> <strong>stress</strong> <strong>model</strong> <strong>for</strong> <strong>the</strong> <strong>incremental</strong> <strong>analysis</strong><br />

<strong>of</strong> large deflecti<strong>on</strong> problems. The c<strong>on</strong>cept <strong>of</strong> initial <strong>stress</strong> is employed, wherein, during<br />

any given step in which <strong>the</strong> displacements, <strong>stress</strong>es and external loads undergo increments,<br />

<strong>the</strong> state at <strong>the</strong> beginning <strong>of</strong> <strong>the</strong> step is c<strong>on</strong>sidered as <strong>on</strong>e <strong>of</strong> initial <strong>stress</strong>. A “check” <strong>on</strong> <strong>the</strong><br />

equilibrium in <strong>the</strong> state prior to <strong>the</strong> additi<strong>on</strong> <strong>of</strong> fur<strong>the</strong>r load increment, analogous to <strong>the</strong><br />

<strong>on</strong>e suggested by H<strong>of</strong>meister et al. [ 171, is included.<br />

BASIC FORMULATION<br />

For clarity in presentati<strong>on</strong>, <strong>the</strong> ideas will be developed within <strong>the</strong> framework,<strong>of</strong> threedimensi<strong>on</strong>al<br />

elasticity <strong>the</strong>ory. Some <strong>of</strong> <strong>the</strong> initial development <strong>of</strong> <strong>the</strong> <strong>the</strong>ory follows closely<br />

that <strong>of</strong> Washizu [21], and Truesdell and Toupin (221 and is repeated here <strong>for</strong> <strong>the</strong> sake <strong>of</strong><br />

completeness.<br />

Each material particle in <strong>the</strong> three-dimensi<strong>on</strong>al c<strong>on</strong>tinuum in <strong>the</strong> original reference<br />

c<strong>on</strong>figurati<strong>on</strong> C, is identified, in general, by three curvilinear coordinates

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