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Material Coefficients (material + coefficient)
Selected AbstractsEin Trocknungskoeffizient für BaustoffeBAUPHYSIK, Issue 3 2009Gregor A. Scheffler Dr.-Ing. Berechnungsverfahren; Feuchte Wärme; Versuche Abstract Ein wesentliches Element der hygrothermischen Charakterisierung von Baustoffen ist der Trocknungsversuch. Im Gegensatz zu anderen Feuchtetransportexperimenten wie dem Diffusionsversuch oder dem Wasseraufnahmeexperiment ist es bislang nicht möglich, aus der Trocknung einen einfachen Kennwert abzuleiten. In vielen Fällen, beispielsweise in der Interaktion von Forschung und Industrie, aber auch beim praktischen Vergleich bzw. der Auswahl geeigneter Baustoffe wäre ein solcher Kennwert jedoch wünschenswert. Im vorliegenden Artikel wird zunächst die Bedeutung des Trocknungsversuches für die hygrische Charakterisierung von Baustoffen herausgestellt, aus der sich das Bestreben ableitet, das Trocknungsverhalten zu standardisieren und einen Einzahlen-Materialkennwert zu definieren. Nach einer die verschiedenen Einflussfaktoren der Trocknung differenzierenden Einleitung werden bestehende Ansätze für die Standardisierung des Trocknungsverlaufes bzw. die Ableitung eines Trocknungskoeffizienten vorgestellt. Die einhergehenden Probleme werden diskutiert und weitere Möglichkeiten evaluiert. Ein einfacher Trocknungskoeffizient, der sich aus dem Trocknungsverlauf ableiten lässt, wird definiert. Die Korrelation dieses Koeffizienten mit dem Wasseraufnahmekoeffizienten und dem Dampfdiffusionswiderstand wird analysiert. Sein zusätzlicher Informationsgehalt wird in diesem Zusammenhang kritisch hinterfragt. Im Ergebnis steht die Definition des Trocknungskoeffizienten als ein neuer, unabhängiger Materialkennwert, der die Feuchtetransporteigenschaften im Übergang zwischen hygroskopischem und gesättigtem Transport beschreibt. Mit diesem Kennwert ist es möglich, Baustoffe einfach und schnell hinsichtlich ihres Trocknungsverhaltens zu unterscheiden und zu beurteilen, was insbesondere bei feuchtesensitiven Materialien von Bedeutung ist. A drying coefficient for building materials. The drying experiment is an important element of the hygrothermal characterisation of building materials. Contrary to other moisture transport experiments as the vapour diffusion and the water absorption test, it is until now not possible to derive a simple coefficient for the drying. However, in many cases such a coefficient would be highly appreciated, e.g. in interaction of industry and research or for the distinction and selection of suitable building materials throughout design and practise. This article first highlights the importance of drying experiments for hygrothermal characterisation of building materials on which the attempt is based to standardize the drying experiment as well as to derive a single number material coefficient. The drying itself is briefly reviewed and existing approaches are discussed. On this basis, possible definitions are evaluated. Finally, a drying coefficient is defined which can be determined based on measured drying data. The correlation of this coefficient with the water absorption and the vapour diffusion coefficient is analyzed and its additional information content is critically challenged. As result, a drying coefficient has been derived and defined as a new and independent material parameter. It contains information about the moisture transport properties throughout the wide range of moisture contents from hygroscopic up to saturation. With this new and valuable coefficient, it is now possible to distinguish and select building materials quickly and easily by means of their drying behaviour. This is particularly important for moisture sensitive materials. [source] Heat and mass transfer during microwave-convective dryingAICHE JOURNAL, Issue 1 2010Stefan J. Kowalski Abstract The article presents a mathematical model of drying that describes the kinetics of combined microwave-convective drying for the process as a whole. Based on this model, the drying curves and the temperature evolutions of the drying body were constructed by a number of computer-simulated drying programs, which were chosen to follow the respective experimental processes carried out on a cylindrical sample made of kaolin. The experimental data allowed both the estimate of material coefficients arising in the model and the validation of the theory. A very satisfactory correlation of the theoretical predictions with the experimental data is found. The main novelty of this article is the mathematically complete drying model that describes all periods of the microwave-convective drying process. Application of such a complete model is necessary if we want to optimize drying processes with respect to drying time and consumption of energy via computer simulations. © 2009 American Institute of Chemical Engineers AIChE J, 2009 [source] Medial collateral ligament insertion site and contact forces in the ACL-deficient kneeJOURNAL OF ORTHOPAEDIC RESEARCH, Issue 4 2006Benjamin J. Ellis Abstract The objectives of this research were to determine the effects of anterior cruciate ligament (ACL) deficiency on medial collateral ligament (MCL) insertion site and contact forces during anterior tibial loading and valgus loading using a combined experimental-finite element (FE) approach. Our hypothesis was that ACL deficiency would increase MCL insertion site forces at the attachments to the tibia and femur and increase contact forces between the MCL and these bones. Six male knees were subjected to varus,valgus and anterior,posterior loading at flexion angles of ,0° and 30°. Three-dimensional joint kinematics and MCL strains were recorded during kinematic testing. Following testing, the MCL of each knee was removed to establish a stress-free reference configuration. An FE model of the femur,MCL,tibia complex was constructed for each knee to simulate valgus rotation and anterior translation at 0° and 30°, using subject-specific bone and ligament geometry and joint kinematics. A transversely isotropic hyperelastic material model with average material coefficients taken from a previous study was used to represent the MCL. Subject-specific MCL in situ strain distributions were used in each model. Insertion site and contact forces were determined from the FE analyses. FE predictions were validated by comparing MCL fiber strains to experimental measurements. The subject-specific FE predictions of MCL fiber stretch correlated well with the experimentally measured values (R2,=,0.95). ACL deficiency caused a significant increase in MCL insertion site and contact forces in response to anterior tibial loading. In contrast, ACL deficiency did not significantly increase MCL insertion site and contact forces in response to valgus loading, demonstrating that the ACL is not a restraint to valgus rotation in knees that have an intact MCL. When evaluating valgus laxity in the ACL-deficient knee, increased valgus laxity indicates a compromised MCL. © 2006 Orthopaedic Research Society. Published by Wiley Periodicals, Inc. J Orthop Res [source] Reconstruction of cracks of different types from far-field measurementsMATHEMATICAL METHODS IN THE APPLIED SCIENCES, Issue 8 2010Jijun Liu Abstract In this paper, we deal with the acoustic inverse scattering problem for reconstructing cracks of possibly different types from the far-field map. The scattering problem models the diffraction of waves by thin two-sided cylindrical screens. The cracks are characterized by their shapes, the type of boundary conditions and the boundary coefficients (surface impedance). We give explicit formulas of the indicator function of the probe method, which can be used to reconstruct the shape of the cracks, distinguish their types of boundary conditions, the two faces of each of them and reconstruct the possible material coefficients on them by using the far-field map. To test the validity of these formulas, we present some numerical implementations for a single crack, which show the efficiency of the proposed method for suitably distributed surface impedances. The difficulties for numerically recovering the properties of the crack in the concave side as well as near the tips are presented and some explanations are given. Copyright © 2009 John Wiley & Sons, Ltd. [source] One-level Newton,Krylov,Schwarz algorithm for unsteady non-linear radiation diffusion problemNUMERICAL LINEAR ALGEBRA WITH APPLICATIONS, Issue 10 2004Serguei Ovtchinnikov Abstract In this paper, we present a parallel Newton,Krylov,Schwarz (NKS)-based non-linearly implicit algorithm for the numerical solution of the unsteady non-linear multimaterial radiation diffusion problem in two-dimensional space. A robust solver technology is required for handling the high non-linearity and large jumps in material coefficients typically associated with simulations of radiation diffusion phenomena. We show numerically that NKS converges well even with rather large inflow flux boundary conditions. We observe that the approach is non-linearly scalable, but not linearly scalable in terms of iteration numbers. However, CPU time is more important than the iteration numbers, and our numerical experiments show that the algorithm is CPU-time-scalable even without a coarse space given that the mesh is fine enough. This makes the algorithm potentially more attractive than multilevel methods, especially on unstructured grids, where course grids are often not easy to construct. Copyright © 2004 John Wiley & Sons, Ltd. [source] A uniform phenomenological constitutive model for glassy and semicrystalline polymersPOLYMER ENGINEERING & SCIENCE, Issue 8 2001Y. Duan A phenomenological constitutive model is proposed on the basis of four models: the Johnson-Cook model, the G'Sell-Jonas model, the Matsuoka model, and the Brooks model. The proposed constitutive model has a concise expression of stress dependence on strain, strain rate and temperature. It is capable of uniformly describing the entire range of deformation behavior of glassy and semicrystalline polymers, especially the intrinsic strain softening and subsequent orientation hardening of glassy polymers. At least three experimental stress-strain curves including variation with strain rate and temperature are needed to calibrate the eight material coefficients. Sequential calibration procedures of the eight material coefficients are given in detail. Predictions from the proposed constitutive model are compared with experimental data of two glassy polymers, polymethyl-methacrylate and polycarbonate under various deformation conditions, and with that of the G'Sell-Jonas model for polyamide 12, a semicrystalline polymer. [source] | ||||||||||