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(A): Infinite domain.
The mechanical behavior of the inhomogeneous body in an infinite domain is very complicated.
Take for example a {P}-structure M with an infinite domain M = {di : i < ω}, where P is unary.
This paper is concerned with the numerical solution to the Schrödinger equation on an infinite domain.
This equation can be solved analytically for an infinite domain region.
To solve the problem numerically, the infinite domain is truncated to finite length.
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Previous models basically focused on numerical and semi-analytical methods for semi-infinite domain.
Semi-infinite domain is mapped into the finite domain using special mapping.
Laplace transformation technique has been used to derive the analytical solution to the problem in a semi-infinite domain.
Two numerical methods were designed to solve the time-dependent, three-dimensional, incompressible Navier-Stokes equations in boundary layers (method A, semi-infinite domain) and mixing layers or wakes (method B, fully-infinite domain).
The semi-infinite domain is then subjected to a moving Hertzian pressure to simulate a load cycle.
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