Opinion - (2023) Volume 12, Issue 3
Received: 01-Mar-2023, Manuscript No. jacm-23-95933;
Editor assigned: 03-Mar-2023, Pre QC No. P-95933;
Reviewed: 15-Mar-2023, QC No. Q-95933;
Revised: 22-Mar-2023, Manuscript No. R-95933;
Published:
28-Mar-2023
, DOI: 10.37421/2168-9679.2023.12.523
Citation: Galli, Cristina. “Two Types of Thermoelastic Contact
Problems and Their Mathematical Theories.” J Appl Computat Math 12 (2023):
523.
Copyright: © 2023 Galli C. This is an open-access article distributed under the
terms of the Creative Commons Attribution License, which permits unrestricted
use, distribution, and reproduction in any medium, provided the original author
and source are credited.
Thermoelastic contact problems involve the study of the interaction between two contacting bodies, where one or both of the bodies are undergoing thermal and mechanical deformation. The mathematical modelling of such problems has been the focus of research for many years, and various mathematical theories have been developed to analyse different aspects of these problems. In this essay, we will discuss mathematical theories for two classes of thermoplastic contact problems. The first class is the non-conforming contact problems, where the contacting bodies do not have the same shape or the same mesh size. The second class is the conforming contact problems, where the contacting bodies have the same shape and mesh size. In non-conforming contact problems, the shape and mesh size of the contacting bodies are not the same. In this case, the mathematical model needs to take into account the deformation of each body separately, and the contact region between the two bodies needs to be determined using appropriate algorithms. One of the most popular mathematical theories used to analyze non-conforming contact problems is the penalty method. The penalty method involves introducing a penalty parameter into the mathematical model to account for the contact forces between the two bodies.
This penalty parameter is typically a very large number, which forces the contact forces to be large and thus ensures that the two bodies do not separate. The penalty method is easy to implement and has been used in many applications, but it has some limitations, such as the dependence on the value of the penalty parameter and the difficulty in determining the correct value of this parameter. Another mathematical theory used to analyze nonconforming contact problems is the augmented Lagrangian method. The augmented Lagrangian method is similar to the penalty method in that it introduces a penalty term into the mathematical model, but it also includes a Lagrange multiplier to enforce the contact constraints. The Lagrange multiplier is updated at each iteration, which allows the method to converge faster than the penalty method. However, the augmented Lagrangian method is more complex than the penalty method and requires more computational resources. In conforming contact problems, the two contacting bodies have the same shape and mesh size.
This simplifies the mathematical modeling of the problem, as both bodies can be treated as a single entity, and the contact region between the two bodies is well-defined. One of the most popular mathematical theories used to analyze conforming contact problems is the finite element method (FEM). The FEM involves dividing the contacting bodies into small elements and approximating the solution of the problem within each element using a set of basis functions. The basis functions are chosen to ensure that the solution satisfies the governing equations and the boundary conditions of the problem. The FEM has been widely used in many applications and is known for its accuracy and flexibility. Another mathematical theory used to analyze conforming contact problems is the boundary element method (BEM). The BEM involves dividing the boundary of the contacting bodies into small elements and approximating the solution of the problem on the boundary using a set of basis functions. The basis functions are chosen to ensure that the solution satisfies the boundary conditions of the problem. The BEM is known for its accuracy and efficiency, as it only requires the discretization of the boundary of the contacting bodies, which reduces the computational cost [1,2].
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