Download Computational Solid Mechanics: Variational Formulation and by Marco L. Bittencourt PDF

By Marco L. Bittencourt

Presents a scientific procedure for Modeling Mechanical versions utilizing Variational Formulation―Uses Real-World Examples and functions of Mechanical Models

Utilizing fabric constructed in a school room environment and validated over a 12-year interval, Computational reliable Mechanics: Variational formula and High-Order Approximation information an process that establishes a logical series for the therapy of any mechanical challenge. Incorporating variational formula according to the primary of digital paintings, this article considers quite a few facets of mechanical types, explores analytical mechanics and their variational rules, and provides version approximations utilizing the finite point approach. It introduces the fundamentals of mechanics for one-, two-, and third-dimensional types, emphasizes the simplification points required of their formula, and offers correct purposes.

Introduces Approximation innovations progressively during the Chapters

Organized into ten chapters, this article offers a transparent separation of formula and finite aspect approximation. It info ordinary methods to formulate and approximate versions, whereas while illustrating their program through software program. bankruptcy one presents a basic advent to variational formula and an outline of the mechanical types to be provided within the different chapters. bankruptcy makes use of the techniques on equilibrium that readers must have to introduce simple notions on kinematics, duality, digital paintings, and the PVW. Chapters 3 to 10 current mechanical types, approximation and purposes to bars, shafts, beams, beams with shear, basic - and three-d beams, solids, aircraft versions, and everyday torsion and plates.

Learn concept Step by means of Step

In every one bankruptcy, the fabric profiles all elements of a particular mechanical version, and makes use of an analogous series of steps for all types. the stairs comprise kinematics, pressure, inflexible physique deformation, inner quite a bit, exterior lots, equilibrium, constitutive equations, and structural design.

The textual content makes use of MATLAB® scripts to calculate analytic and approximated recommendations of the thought of mechanical versions.

Computational good Mechanics: Variational formula and excessive Order Approximation

presents mechanical versions, their major speculation, and functions, and is meant for graduate and undergraduate engineering scholars taking classes in good mechanics.

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Extra info for Computational Solid Mechanics: Variational Formulation and High Order Approximation

Example text

For models with nonzero strain measures, loads are represented by continuous functions over the domain of the body. As continuum mechanics assumes that matter is continuous, it is natural that all involved quantities, including kinematics and internal and external loads, are represented by continuous functions. The PVW can also be applied to obtain the solution to specific examples. In the most general case, the standard procedure for the formulation of the mechanical models considered here is given by the following steps: 1.

P P (a) Real. B (b) Idealized. P O P (c) Equivalent system. 5 Couple and equivalent concentrated moment. In other cases, the forces are applied over a larger portion of the body and are called distributed loads. 4 illustrates constant and linearly varying distributed forces, with the corresponding idealizations. 5. 5(b)]. This pair of forces with same intensity and opposite directions is called couple. 5(c). It should be observed that when the couple applied at A and B is transferred to point O, we obtain a zero resultant force in the horizontal direction.

Even if we consider two distinct virtual actions δ vA and δ vB to points A and B, the components of these vectors along line AB must be equal, because the distance between two points must be constant for rigid bodies. Designating these components as δ v, the power associated to the motion of points A and B are given by δ Pe = fAB · δ v + fBA · δ v = (fAB − fAB) · δ v = 0. Hence, the power associated to internal forces between any two points of a rigid body is zero, independently of the considered virtual motion used to evaluate the equilibrium.

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