Finite Element Multidisciplinary Analysis, Second Edition

4.4: Three-Dimensional Solid Elements

4.4 Three-Dimensional Solid Elements

4.4.1 Constant Strain Tetrahedron

Figure 4.10 shows the natural coordinates system for a four-noded tetrahedron element with the face 1-2-3 on the local x- y plane. [11] , [12] The relationship between element local and natural coordinate systems may be expressed as


which, referring to Fig. 4.10, reduces to



Figure 4.10: Four-noded tetrahedron and other solid elements.

In the volume coordinate system ? i = V i/V, in which V i is the tetrahedron bound by the center of volume point P and surface opposite to the node i of the element. The volume V of the element is defined as


where


The inverse transformation of Eq. (4.103) is obtained as


or


A linear displacement distribution is assumed within the element. Thus typically


which with substitution of nodal boundary conditions yields


and similarly for u y and u z displacements, N y = N z = N x = N. Using the chain rule of differentiation, e.g., in the x direction for a function f


Now for f = u x, it follows that


because ? N/ ? ? is a unit matrix of order four. Similar expressions can be obtained for other displacement derivatives. The strain-displacement relationships for the three-dimensional case are


which can be written in matrix form:


or


Then the stiffness matrix is given by


because B is constant. The inertia...

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