60th Anniversary Symposium of the International Association for Shell and Spatial Structures (IASS Symposium 2019)
9th International Conference on Textile Composites and Inflatable Structures (Structural Membranes 2019)
The conference cover all aspects related to material, design, computation, construction, maintenance, history, environmental impact and sustainability of shell, spatial, tension and inflatable structures in all fields of application.
In addition to incorporating the Annual Symposium of the International Association for Shell and Spatial Structures (IASS), FORM and FORCE 2019 will be proposed as a Thematic Conference of the European Community on Computational Methods in Applied Sciences (ECCOMAS) and a Special Interest Conference of the International Association for Computational Mechanics (IACM).
Technological progress and discovery and mastery of increasingly sophisticated
structural materials have been inexorably tied together since the dawn
of history. In the present era — the so-called Space Age —-, the prevailing
trend is to design and create new materials, or improved existing ones, by
meticulously altering and controlling structural features that span across all
types of length scales: the ultimate aim is to achieve macroscopic proper-
ties (yield strength, ductility, toughness, fatigue limit . . . ) tailored to given
practical applications. Research efforts in this aspect range in complexity
from the creation of structures at the scale of single atoms and molecules —
the realm of nanotechnology —, to the more mundane, to the average civil
and mechanical engineers, development of structural materials by changing
the composition, distribution, size and topology of their constituents at the
microscopic/mesoscopic level (composite materials and porous metals, for
instance).
Abstract Technological progress and discovery and mastery of increasingly sophisticated
structural materials have been inexorably tied together since the dawn
of history. In the [...]
La presente monografía está basada en el texto de la tesis doctoral homónima defendida
en la Universitat Politècnica de Catalunya el 6 de febrero de 2012, en el marco
del programa de doctorado de Análisis Estructural del Departament de Resistència de
Materials i Estructures a l’Enginyeria. En este estudio se analiza la viabilidad del uso
de las técnicas experimentales y numéricas basadas en la respuesta dinámica, para la
detección y localización del daño inducido, la cuantificación del grado de severidad y
la predicción de las propiedades mecánicas residuales de laminados de material compuesto
tras ser sometidos a un impacto a baja velocidad. El trabajo de investigación
comprende un enfoque mixto experimental y numérico. Por un lado constituye un
riguroso estudio experimental que incluye la evaluación de la resistencia a impacto,
la caracterización del daño inducido, la cuantificación de los efectos en la respuesta
dinámica y la evaluación de la capacidad portante residual. El estudio experimental
se completa con un minucioso análisis del efecto inducido por deslaminaciones artificiales en la respuesta dinámica y en la capacidad portante residual de los laminados.
Por otro lado, se ha simulado el fenómeno estimando principalmente la iniciación y la
propagación del daño interlaminar e igualmente los efectos inducidos en la respuesta
dinámica. En el enfoque numérico se trata el material compuesto como un sistema
microestructural, en el cual los fallos surgen en la interacción entre los materiales
constituyentes. Para reproducir la degradación se emplea una estrategia de reducción
localizada de la rigidez elástica del material que no demanda una intervención durante
el preproceso.
Los resultados empíricos aportan conclusiones relevantes en relación al grado de
sensibilidad y a la adecuación de los diferentes criterios de correlación modal para la
identificación del daño inducido por un impacto. Los nuevos criterios de correlación
definidos y el análisis conjunto de las propiedades estáticas y dinámicas residuales, han
permitido acotar el intervalo de incertidumbre y reducir la limitación actual en relación
a la deformación máxima admisible a compresión de los laminados. La herramienta
de cálculo desarrollada permite simular el comportamiento vibratorio de laminados
compuestos definiendo el material y su estado de degradación en la microescala. Los
resultados corroboran la viabilidad del enfoque microestructural para la simulación
del fenómeno.
Abstract La presente monografía está basada en el texto de la tesis doctoral homónima defendida
en la Universitat Politècnica de Catalunya el 6 de febrero [...]
El divulgado uso estructural de barras gruesas tanto rectas como curvas gruesas en
las distintas aplicaciones de las diversas ingenierías, hace que conocer su
comportamiento dinámico frente a solicitaciones arbitrarias, constituya una finalidad
que todo avance tecnológico requiere.
El presente trabajo abarca y extiende, dentro del marco de la Resistencia de
Materiales (RM) y de materiales no homogéneos (materiales funcionales y/o
compuestos), uno previo del autor que consiste en la teoría general de movimiento de
piezas curvas gruesas homogéneas y que está desarrollado en el Capítulo primero de
su Tesis Doctoral [1]. En éste se toman en consideración la totalidad de los aportes
energéticos para hallar el sistema diferencial gobernante de vibración forzada. En el
desarrollo general que presentaremos y que incluye entre otros a los temas
nombrados, se aborda la posibilidad de que el módulo de elasticidad, el módulo de
elasticidad transversal y la densidad puedan variar independiente y arbitrariamente
en el dominio de la sección transversal (aunque de forma simétrica respecto del eje de
simetría de la misma ya que estudiamos el movimiento plano de piezas gruesas).
La teoría presentada incluye a la teoría clásica de barras delgadas rectas y curvas
homogéneas (Bernoulli-Euler y barras de gran curvatura sometidas a flexión
compuesta [2] [3] [4]) y como caso especial cuando tratamos barras rectas pero también
homogéneas, a la denominada Teoría de Vigas Timoshenko [5].
Se desarrollan y se justifican teóricamente temas fundamentales tales como las
expresiones que ligan constitutivamente al esfuerzo de corte con el régimen de
deformación; la expresión general del factor de corte a través de la vía energética
dependiendo de la distribución de las dos componentes de la tensión tangencial –una
según el eje de simetría de la sección y perpendicular al mismo la otra– actuantes en
elementos de área del plano de cada sección de la barra y debidas a un esfuerzo de
corte Q. Una conclusión, que presentamos como “Resullttado Fundamenttall”, permite
obtener el régimen de tensiones tangenciales para barras curvas gruesas no
homogéneas, por medio de barras rectas ficticias. Es decir, se manejan unas barras
rectas (curvatura infinita) en las cuales modificando algunos parámetros físico–
geométricos, pueden hallarse las tensiones tangenciales y con ellas el factor de corte
de barras curvas.
Todavía el trabajo aporta la conclusión más importante en cuanto a la distribución de
las tensiones tangenciales y con ésta el cálculo del ffacttor de cortte, que desarrollamos
en la PARTE SEGUNDA denominándolo como TEOREMA GENERAL. Afirma que una
vez hallada la distribución tangencial en algún tipo de barra gruesa –recta, curva o
ficticia– un cálculo directo, con apropiados intercambios de parámetros físico–geométricos
que dependen del tipo de barra y de la distribución de las no homogeneidades y forma de la
sección transversal de la barra, permite conocer la distribución de las tensiones
tangenciales en los otros dos tipos de barra con la misma sección.
Se incluyen otros dos resultados originales que se denominan métodos I y II de
superposición –para los tres tipos de barras gruesas que el trabajo aborda– que, cuando
las secciones de las barras modifican “a saltos” sus propiedades elásticas y de densidad,
puede hallarse el régimen tensional combinando linealmente regímenes conocidos de
secciones homogéneas. Esto simplifica notablemente el trabajo de búsqueda para estos
tipos de sección no homogénea bajo estudio. Se encuentra también un acople flexo–axial
del movimiento y se trabaja y se generaliza el concepto del corrimiento del eje neutro,
imposición clásica en barras homogéneas de gran curvatura que permite no sólo
simplificar el proceso algebraico sino que extiende naturalmente la definición de eje
neutro que se utiliza tradicionalmente en barras rectas homogéneas.
Al desarrollar el ítem de vibraciones naturales de las barras gruesas partiendo de las
ecuaciones de movimiento, tanto rectas como curvas, se encuentran las condiciones de
ortogonalidad entre formas modales (extensión ad-hoc del tradicional modelo de Sturm–
Liouville [6]) para ser utilizadas en una eventual superposición modal clásica en problemas
lineales y separables, para hallar la respuesta dinámica del sistema (Vibración Forzada).
Algunos Apéndices y varios Ejemplos resueltos analítica y numéricamente completan el
trabajo que permite inferir que los resultados encontrados coinciden con muy buena
precisión con los hallados con otras metodologías aproximadas como son las de elementos
finitos en 2D y 3D pero por medio de un encuadre mucho más directo, sencillo y abarcativo.
Cabe todavía agregar que la propuesta para llegar al régimen de tensiones
tangenciales de las secciones de formas arbitrarias constitutivamente no homogéneas,
y aún múltiplemente conexas, reemplaza a las utilizadas comúnmente para barras
rectas homogéneas y que son conocidas como de Collignon o de Jourawsky. Por otro
lado estas metodologías tradicionales serían prácticamente inadecuadas de utilizar
para ciertos casos dentro del espectro de aplicaciones que presentamos.
Fundamentalmente, lo dicho permite hallar el factor de corte de las secciones de
barras gruesas y entonces completar los coeficientes del sistema diferencial que
gobierna el movimiento de estos tipos estructurales.
Por último entendemos que el Resullttado Fundamenttall, el TEOREMA GENERAL, los
Métodos de Superposición, las Ecuaciones de Movimiento y las Condiciones de
Ortogonalidad presentadas, son resultados originales dentro de la bibliografía afín.
Abstract El divulgado uso estructural de barras gruesas tanto rectas como curvas gruesas en
las distintas aplicaciones de las diversas ingenierías, hace que conocer su
comportamiento [...]
We present three new stabilized finite element (FE) based Petrov–Galerkin methods for the convection–diffusion–reaction (CDR), the Helmholtz and the Stokes problems, respectively. The work embarks upon a priori analysis of some consistency recovery procedures for some stabilization methods belonging to the Petrov–Galerkin framework.
It was found that the use of some standard practices (e. g.M-Matrices theory) for the design of essentially non-oscillatory numerical methods is not appropriate when consistency recovery methods are employed. Hence, with respect to convective stabilization, such recovery methods are not preferred. Next, we present the design of a high-resolution Petrov–Galerkin (HRPG) method for the CDR problem. The structure
of the method in 1d is identical to the consistent approximate upwind (CAU) Petrov–Galerkin method [68] except for the definitions of the stabilization parameters.
Such a structure may also be attained via the Finite Calculus (FIC) procedure [141] by an appropriate definition of the characteristic length. The prefix high-resolution is used here in the sense popularized by Harten, i. e.second order accuracy for smooth/regular regimes and good shock-capturing in non-regular regimes. The design procedure in 1d embarks on the problem of circumventing the Gibbs phenomenon observed in L2 projections. Next, we study the conditions on the stabilization parameters to circumvent the global oscillations due to the convective term. A conjuncture of the two results is made to deal with the problem at hand that is usually plagued by Gibbs, global and dispersive oscillations in the numerical solution. A multi dimensional extension of the HRPG method using multi-linear block finite elements is also presented.
Next, we propose a higher-order compact scheme (involving two parameters) on structured meshes for the Helmholtz equation. Making the parameters equal, we recover the alpha-interpolation of the Galerkin finite element method (FEM) and the classical central finite difference method. In 1d this scheme is identical to the alphainterpolation method [140] and in 2d choosing the value 0.5 for both the parameters, we recover the generalized fourth-order compact Padé approximation [81, 168] (therein using the parameter
gamma = 2). We follow [10] for the analysis of this scheme and its performance on square meshes is compared with that of the quasi-stabilized FEM [10]. Generic expressions for the parameters are given that guarantees a dispersion accuracy of sixth-order should the parameters be distinct and fourth-order should they be equal. In the later case, an expression for the parameter is given that minimizes the maximum relative phase error in 2d. A Petrov–Galerkin formulation that yields the aforesaid scheme on structured meshes is also presented. Convergence studies of the
error in the L2 norm, the H1 semi-norm and the l1 Euclidean norm is done and the pollution effect is found to be small.
Finally, we present a collection of stabilized FE methods derived via first-order and second-order FIC procedures for the Stokes problem. It is shown that several well known existing stabilized FE methods such as the penalty technique, the Galerkin Least Square (GLS) method [93], the Pressure Gradient Projection (PGP) method [35] and the orthogonal sub-scales (OSS) method [34] are recovered from the general
iii residual-based FIC stabilized form. A new family of Pressure Laplacian Stabilization (PLS) FE methods with consistent nonlinear forms of the stabilization parameters are derived. The distinct feature of the family of PLS methods is that they are nonlinear and residual-based, i. e.the stabilization terms depend on the discrete residuals of the momentum and/or the incompressibility equations. The advantages and disadvantages of these stabilization techniques are discussed and several examples of application are presented.
Abstract We present three new stabilized finite element (FE) based Petrov–Galerkin methods for the convection–diffusion–reaction (CDR), the Helmholtz and the Stokes [...]
En este trabajo, se estableció una metodología de soporte al diagnostico de AD, principalmente
en sus etapas MCI ocasionado por AD y demencia ocasionada por AD.
Para este fin fueron obtenidos casos clínicos de dos proyectos de investigación en demencia
del tipo AD de reconocida trayectoria: las bases de datos Alzheimer's Disease
Neuroimaging Initiative (ADNI) (www.loni.ucla.edu/ADNI) y la base de datos The
Open Access Series of Imaging Studies (OASIS) (http://www.oasis-brains.org/).
Asimismo, fueron establecidas dos tareas principales: la selección de variables predictoras
de AD y la construcción de modelos de clasificacion basados en máquinas
de soporte vectorial (SVM), entrenados a partir de las variables seleccionadas. Las
variables predictoras seleccionadas estuvieron conformadas por biomarcadores morfométricos y características socio-demográficas y neuropsicológicas. Estas variables
deberan ser útiles para la discriminación de casos clínicos en tres estados: (1) Estado
normal (generalmente personas mayores sanas);
(2) Estado MCI ocasionado por
AD; y (3) Etapa de demencia ocasionada por AD. Por otro lado, los modelos SVM
estarán enfocados a dos tareas principales: (1) Diagnóstico de AD mediante la discriminación entre sujetos sanos y sujetos con AD; y (2) Predicción de AD, orientada
a la discriminación de sujetos MCI con riesgo de convertirse a AD y sujetos MCI
sin riesgo de conversión. Asimismo, estos modelos deberán garantizar resultados
aceptables, respecto a la sensibilidad y especificidad de las tareas de clasificación.
Los resultados obtenidos en esta investigación son prometedores. Por un lado, el
subconjunto de variables seleccionadas como relevantes para el diagnóstico de AD,
tienen correlación con los resultados de investigaciones previas. Asimismo, en la
etapa de testeo, los resultados demostraron que los modelos SVM son de gran utilidad
para el soporte diagnóstico clínico de esta enfermedad, siendo capaces de discriminar
sujetos con AD de sujetos sanos (diagnóstico) con una exactitud mayor al 99% y
distinguir a los sujetos MCI con riesgo de conversión a AD de los sujetos MCI sin
riego de conversión (predicción) con una exactitud superior al 94%.
Abstract En este trabajo, se estableció una metodología de soporte al diagnostico de AD, principalmente
en sus etapas MCI ocasionado por AD y demencia ocasionada por [...]
Rockfill dams are nowadays often preferred over concrete dams because of their economic advantages, their flexible and thank to the great advance achieved in geosciences and geomechanics.
Unfortunately their behavior in case of overtopping is still an open issue. In fact very little is known on this phenomenon that in most cases leads to the complete finite failure o the structure with catastrophic
consequences in term of loss of lives and economic damage.
The principal aim of the present work is the development of a computational method
to simulate the overtopping and the beginning of failure of the downstream shoulder of
a rockfill dam. The whole phenomenon is treated in a continuous framework.
The fluid free surface problem outside and inside the rockfill slop e is treated using a
unique Eulerian fixed mesh formulation. A level set technique is employed to track the
evolution of the free surface. The traditional Navier-Stokes equations are modified in
order to automatically detect the presence of the porous media. The non-linear seepage
is evaluated using a quadratic form of the resistance law for which the Ergun's coefficients
have been chosen.
Abstract Rockfill dams are nowadays often preferred over concrete dams because of their economic advantages, their flexible and thank to the great advance achieved in geosciences and [...]
The methodology proposed in this research work explores the use of the strain injection concept in a combination of classical strain localization methods and
embedded strong discontinuities, to remove the flaws (stress locking and mesh
bias dependence) of the former, and simultaneously abdicate of the global tracking
algorithms usually required by the later. The basic idea is to use, after the
bifurcation instant, i.e. after the time that elements are amenable to develop discontinuities,
a mixed continuous displacements - discontinuous constant strains
condensable finite element formulation (Q1/e0 ) for quadrilaterals in 2D. This
formulation provides improved behavior results, specially, in avoiding mesh bias
dependence. In a first, very short, stage after the bifurcation the concept of strong
discontinuity is then left aside, and the apparent displacement jump is captured
across the finite element length (smeared) like in classical strain localization settings.
Immediately after, in a second stage, the kinematics of those finite elements
that have developed deep enough strain localization is enriched with the injection
of a weak/strong discontinuity mode that minimizes the stress locking defects.
The necessary data to inject the discontinuity (the discontinuity direction and its
position inside the finite element) is obtained by a post process of the strain-like
internal variable field obtained in the first stage, this giving rise to a local (elemental
based) tracking algorithm (the crack propagation problem) that can be
locally and straightforwardly implemented in a finite element code in a non invasive
manner. The obtained approach enjoys the benefits of embedded strong discontinuity
methods (stress locking free, mesh bias independence and low computational
cost), at a complexity similar to the classical, and simpler, though less
accurate, strain localization methods. Moreover, the methodology is applicable to
any constitutive model (damage, elasto-plasticity, etc.) without apparent limitations.
Representative numerical simulations validate the proposed approach.
Abstract The methodology proposed in this research work explores the use of the strain injection concept in a combination of classical strain localization methods and
embedded strong [...]
One of the most important engineering tasks over the years has been the design
and manufacture of increasingly sophisticated structural materials as a result of the
requirements related to the technological progress. In the last decades, the growing
needs for improved properties of products have been partially solved through the
development of composite materials. A key to the success of many modern structural
components is the tailored behavior of the material to given applications.
Therefore, research efforts in material science engineering have been focused in the
design of new materials either through the creation of new structures at the scale
of single atoms and molecules or through the development of structural materials
by changing the composition, size, arrangement and topology of the constituents
at larger scales: the microscopic/mesoscopic level.
The development of new materials has been linked to the development of a new
theoretical field within the mechanics of solids. This branch of the mechanical,
known as Continuum Micromechanics, introduces a series of new concepts that are
key to the definition of the macroscopic properties of composite materials on the
basis of the definition of the characteristics of its components. Starting from the
premise of separation of scales and the concept of Representative Volume Element,
defined the so-called homogenization methods, whose number has been increasing
as the Micromechanics is gone extend over the years. Such methods are many and
varied, although especially there have been two that have been used and developed
by the majority of authors: the so-called Mean-Homogenization techniques and the
multi-scale based on Finite Element Approaches.
Mean-fifieeld homogenization schemes are an efficient way to predict the behavior
of heterogeneous materials. They range from the simplest hypotheses of the stress
or strain sharing among the phases which do not require analytical solution on the
associated boundary-value problem to more involved geometric models based on
the solution of a boundary-value problem involving a single or composite inclusion
embedded in an equivalent homogenized medium whose elastic module become part
of the solution procedure. In general, they are based on analytical solutions of the
boundary value problem defined in the microstructure level of the inhomogeneous
material and provide good predictions for the mean values over the RVE. Although
originally designed for elastic materials, some approaches to deal with elastoplastic
materials and even with viscoplastic materials have been developed over the years
and compared with the results obtained using Finite Element Approaches. The comparison between different methods of homogenization allows the definition of
a range of validity between the different methods, which helps to discover the
limitations of the various methods and aspects to take into account for future
developments and research.
The main goal of this work is, firstly, to present a general overview of the
different techniques that have been developed in the last years in order to obtain
a prediction of the behavior of elastoplastic composites by taking into account
geometrical and mechanical aspects. Secondly, a comparison between the different
approaches is carried out through a numerical implementation of such techniques.
Both objectives will be carried out through eight different chapters. The first
chapter serves as an introduction and historical review of the advances that have
been made in the field of micromechanics. On the other hand, the second chapter
deals with some important theoretical background that is important in the field
of Continuum Micromechanics, as well as a short introduction of the different
approaches that traditionally have been considered to solve the problem. One group
of methods, based on analytical solutions { the so-called Mean Field Analysis {
will be commented in chapter 3. Chapter 4 is devoted to the implementation
and validation of a numerical tool that solves the mean-field homogenization using
analytical schemes for elastoplastic materials. Subsequent chapters are devoted to
the comparison of the results with the results given by the Finite Element Method.
The general formulation of such method { applied to multi-scale problems { is
presented in chapter 5 from a theoretical point of view, as well as the corresponding
numerical examples. Finally, last chapter will be dedicated to enumerate some
conclusions extracted from the present work, including some aspects that can be
object of future works or improvements.
The current work presents some important aspects about the theoretical concepts
and the numerical implementation of some key approaches for solving the
mechanical problem regarding composite materials. There exist a large number
of possibilities to approximate the response of such complex materials, based in
different assumptions. This document shows the general efficiency of the so-called
mean-field homogenization schemes to capture correctly the macroscopic behavior
of composites. Although these techniques show some limitations, like the incapability
to provide results for the distribution of the different variables over the
microgeometry or the low accuracy in the case of complex microgeometries (like
porous materials), they represent an efficient way to predict the main general behavior
of a composite material spending low computational effort. They are specially
indicated to be used in the previous steps of an analysis or as a tool to validate the
results with more involved approaches.
Abstract One of the most important engineering tasks over the years has been the design
and manufacture of increasingly sophisticated structural materials as a result of the
requirements [...]
In computational mechanics, scientific visualization provides researchers and engineers with
tools for studying numerical data. The basis of each of these tools is comprised by scientific
visualization techniques.
This thesis deals with the necessary changes to conventional scientific visualization techniques
in order to visualize the results obtained from the application of particle based methods and
mesh-less methods. This is done taking into account the large amount of data that results from
the application of these methods and the presence or absence of contour information.
Moreover, it is developed a visualization technique for representing micro-cracks and
discontinuities, which are the beginning of chains of structural failures. A mesh generation
method is selected, given its provided facilities, and it is adapted to generate point clouds for
representing volumes and surfaces.
For each proposed technique we study the advantages of the data structures used, and show
its contributions to computer graphics and to data analysis.
Abstract In computational mechanics, scientific visualization provides researchers and engineers with
tools for studying numerical data. The basis of each of these tools is comprised [...]
E. Soudah, M. Bordone, E. Kwee, T. Loong, C. Tan, P. Uei, N. Sriram
Monograph CIMNE (2013). M137
Abstract
The aim of this document is to report the study process and the work carried on by CIMNE, in
order that NTU and TTSH can validate the AAA results obtained during this analysis. The
structure of this numerical analysis will be used for the following cases.
Abstract The aim of this document is to report the study process and the work carried on by CIMNE, in
order that NTU and TTSH can validate the AAA results obtained during this analysis. [...]