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Titlebook: Integral Methods in Science and Engineering; Analytic Treatment a Christian Constanda,Paul Harris Book 2019 Springer Nature Switzerland AG

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A Stiff Problem: Stationary Waves and Approximations,perator posed in a domain . of .: this domain is composed of two parts in which the stiffness constants are of different order of magnitude, namely, .(.) and .(1), respectively, where . is a parameter . << 1. Here, for each fixed ., we give explicit formulas for the eigenvalues and the eigenfunction
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Modelling Creep in Concrete Under a Variable External Load,eeps by the influence of an external load. The normal stress on the cohesive zone satisfies a history-dependent yield condition, which is represented in the form of a nonlinear Abel-type integral operator in time. The external load will be time dependent in the form of a polynomial function. Initial
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A Combined Boundary Element and Finite Element Model of Cell Motion due to Chemotaxis,e cell is increasing. In some cases of chemotaxis, cells secrete the chemical in order to create a concentration gradient that will attract other nearby cells to form clusters. When the cell secreting the chemical is stationary the linear diffusion equation can be used to model the concentration of
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Shape Optimization for Interior Neumann and Transmission Eigenvalues,e is far from trivial. For example, a concrete maximizer with respect to shapes of fixed area is theoretically established only for the first two non-trivial Neumann eigenvalues. The existence of such a maximizer for higher Neumann eigenvalues is still unknown. Hence, the problem should be addressed
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Periodic Transmission Problems for the Heat Equation,into systems of integral equations. Then we establish the invertibility of the operators appearing in the integral equations and we deduce the unique solvability in parabolic Schauder spaces of the transmission problems.
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On United Boundary-Domain Integro-Differential Equations for Variable Coefficient Dirichlet Problem. The PDE right-hand side belongs to the Sobolev spaces ..(.), when neither classical nor canonical co-normal derivatives are well defined. Using an appropriate parametrix (Levi function) the problem is reduced to a direct boundary-domain integro-differential equation (BDIDE) or to a domain integral
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