d upper Omega equals 0"/>
Neglecting source term and integrating by part the first part of the first term
Inserting the shape functions
(3.28b)
(3.29b)
(3.30b)
(3.31b)
(3.32b)
Equation (3.33) is scalar.
3.4 Conclusions
In this chapter, the governing equations introduced in Chapter 2 are discretized in space and time using various implicit and explicit algorithms. They are now ready for implementation into computer codes. In Chapter 5, we shall address some special modeling aspects and in Chapters 6–8, we shall show some applications for static, quasi‐static, and dynamic examples to illustrate the practical applications of the method and to validate and verify the schemes and constitutive models used.
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