Continuum Mechanics using Mathematica®: Fundamentals, by Antonio Romano

By Antonio Romano

This book's methodological technique familiarizes readers with the mathematical instruments required to properly outline and remedy difficulties in continuum mechanics. The e-book covers crucial rules and basic purposes, and offers a superb foundation for a deeper learn of tougher and really expert difficulties with regards to elasticity, fluid mechanics, plasticity, fabrics with reminiscence, piezoelectricity, ferroelectricity, magneto-fluid mechanics, and kingdom changes.
Key subject matters and contours:
* Concise presentation moves a stability among basics and applications
* needful mathematical historical past rigorously amassed in introductory chapters and appendices
* contemporary advancements highlighted via insurance of extra major purposes to parts similar to porous media, electromagnetic fields, and section transitions
Continuum Mechanics utilizing Mathematica® is aimed toward complex undergraduates, graduate scholars, and researchers in utilized arithmetic, mathematical physics, and engineering. it might function a direction textbook or self-study reference for an individual looking an exceptional starting place within the field.

Show description

By Antonio Romano

This book's methodological technique familiarizes readers with the mathematical instruments required to properly outline and remedy difficulties in continuum mechanics. The e-book covers crucial rules and basic purposes, and offers a superb foundation for a deeper learn of tougher and really expert difficulties with regards to elasticity, fluid mechanics, plasticity, fabrics with reminiscence, piezoelectricity, ferroelectricity, magneto-fluid mechanics, and kingdom changes.
Key subject matters and contours:
* Concise presentation moves a stability among basics and applications
* needful mathematical historical past rigorously amassed in introductory chapters and appendices
* contemporary advancements highlighted via insurance of extra major purposes to parts similar to porous media, electromagnetic fields, and section transitions
Continuum Mechanics utilizing Mathematica® is aimed toward complex undergraduates, graduate scholars, and researchers in utilized arithmetic, mathematical physics, and engineering. it might function a direction textbook or self-study reference for an individual looking an exceptional starting place within the field.

Show description

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Extra info for Continuum Mechanics using Mathematica®: Fundamentals, Applications and Scientific Computing

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The components of the corresponding eigenvectors can be obtained by solving the following homogeneous system: T ij uj = λδ ij uj . 101) become 3u1 + 2u2 − u3 = 0, 2u1 + 3u2 + u3 = 0, −u1 + u2 + 2u3 = 0. Imposing the normalization condition ui ui = 1 to these equations gives 1 u1 = √ , 3 1 u2 = − √ , 3 1 u3 = √ . 3 Proceeding in the same way for λ = 4 and λ = 6, we obtain the components of the other two eigenvectors: 1 1 2 −√ , √ , √ 6 6 6 , 1 1 √ , √ ,0 . 2 2 From the symmetry of T, the three eigenvectors are orthogonal (verify).

14 Chapter 1. Elements of Linear Algebra The Program VectorSys Aim of the Program VectorSys The program VectorSys determines, for any system Σ of applied vectors, an equivalent vector system Σ and, when the scalar invariant vanishes, its central axis. Moreover, it plots in the space both the system Σ and Σ , as well as the central axis. Description of the Problem and Relative Algorithm Two systems Σ = {(Ai , vi )}i=1,···,n and Σ = {(Bj , wj )}j=1,···,m of applied vectors are equivalent if they have the same resultants and moments with respect to any pole O.

Then the only real eigenvalue is λ = 1. The one-dimensional eigenspace belonging to the eigenvalue λ = 1 is called the rotation axis. 10 Chapter 1. Elements of Linear Algebra Cauchy’s Polar Decomposition Theorem In this section we prove a very important theorem, called Cauchy’s polar decomposition theorem. 10 Let F be a 2-tensor for which det F > 0 in a Euclidean vector space E3 . 84) where U, V, and R are uniquely defined by the relations U= √ FT F, −1 R = FU =V V= −1 √ FFT , F. 85) PROOF To simplify the notation, an orthonormal basis (e1 , e2 , e3 ) is chosen in E3 .

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