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Unbounded domain
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Part 1 of ebook "Applied partial differential equations (Third edition)" provides readers with contents including: Chapter 1 - The physical origins of partial differential equations; Chapter 2 - Partial differential equations on unbounded domains; Chapter 3 - Orthogonal expansions;...
163p
daonhiennhien
03-07-2024
1
1
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Continued part 1, part 2 of ebook "Complex analysis (Third edition)" has presents the following content: further contour integral techniques; introduction to conformal mapping; the riemann mapping theorem; maximum-modulus theorems for unbounded domains; harmonic functions; different forms of analytic functions; analytic continuation; the gamma and zeta functions; applications to other areas of mathematics;...
165p
dieptieuung
20-07-2023
3
2
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The aim of this paper "Global Attractor for a Semilinear Parabolic System" is to prove the existence of a global attractor of the semigroup generated by the first initial boundary value problem for a semilinear parabolic system in the potential form in an arbitrary (bounded or unbounded) domain.
18p
runordie5
04-07-2022
5
1
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In the paper "The complex Monge–Ampère equation in unbounded hyperconvex domains in Cn", we look for solutions of the complex Monge–Ampère equation with boundary values (ddcu)n = μ in an unbounded hyperconvex domain of Cn.
18p
runordie3
27-06-2022
15
3
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In this paper, we consider the 2D g-Bénard problem in domains satisfying the Poincaré inequality with homogeneous Dirichlet boundary conditions. We show the existence and uniqueness of strong solutions. The obtained results particularly extend previous results for 2D g-Navier-Stokes equations and 2D Bénard problem.
10p
vithales
19-04-2022
17
2
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We consider the 2D g-B´enard problem in domains satisfying the Poincar´e inequality with homogeneous Dirichlet boundary conditions. We prove the existence and uniqueness of global weak solutions. The obtained results particularly extend previous results for 2D g-Navier-Stokes equations and 2D B´enard problem.
9p
koxih_kothogmih5
04-09-2020
15
3
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This paper presents an efficient and accurate numerical technique based upon the scaled boundary finite element method for the analysis of two-dimensional, linear, second-order, boundary value problems with the domain completely described by a circular defining curve. The scaled boundary finite element formulation is established in a general framework allowing single-field and multi-field problems, bounded and unbounded bodies, distributed body source, and general boundary conditions to be treated in a unified fashion.
11p
elandorr
05-12-2019
14
0
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In this paper we continue to develop the method on non-uniform grids for solving a boundary problem for elliptic equation in a semistrip.
5p
vixyliton2711
12-04-2019
13
1
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We propose a syntactic falter for identifying non-coreferential pronoun-NP pairs within a sentence. The filter applies to the output of a Slot Grammar parser and is formulated m terms of the head-argument structures which the parser generates. It liandles control and unbounded dependency constructions without empty categories or binding chains, by virtue of the uniticational nature of the parser. The filter provides constraints for a discourse semantics system, reducing the search domain to which the inference rules of the system's anaphora resolution component apply. ...
8p
bungio_1
03-05-2013
48
2
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Atrial natriuretic peptide (ANP) plays a major role in blood pressure and volume regulation. ANP activities are mediated by a cell surface, single-span transmembrane receptor linked to its intrinsic guanylate cyclase activ-ity. The crystal structures of the dimerized ANP receptor extracellular domain (ECD) with and without ANP have revealed a novel hormone-
9p
vinaphone15
27-02-2013
29
1
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THE FIRST EIGENVALUE OF p-LAPLACIAN SYSTEMS WITH NONLINEAR BOUNDARY CONDITIONS D. A. KANDILAKIS, M. MAGIROPOULOS, AND N. B. ZOGRAPHOPOULOS Received 12 October 2004 and in revised form 21 January 2005 We study the properties of the positive principal eigenvalue and the corresponding eigenspaces of two quasilinear elliptic systems under nonlinear boundary conditions. We prove that this eigenvalue is simple, unique up to positive eigenfunctions for both systems, and isolated for one of them. 1. Introduction Let Ω be an unbounded domain in RN , N ≥ 2, with a noncompact and smooth boundary ∂Ω.
15p
sting12
10-03-2012
49
3
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Tuyển tập báo cáo các nghiên cứu khoa học quốc tế ngành hóa học dành cho các bạn yêu hóa học tham khảo đề tài: NONEXPANSIVE MAPPINGS DEFINED ON UNBOUNDED DOMAINS
13p
dauphong18
09-03-2012
18
2
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Báo cáo hóa học: "Research Article Fixed Points for Pseudocontractive Mappings on Unbounded Domains"
Tuyển tập báo cáo các nghiên cứu khoa học quốc tế ngành hóa học dành cho các bạn yêu hóa học tham khảo đề tài: Research Article Fixed Points for Pseudocontractive Mappings on Unbounded Domains
17p
sting08
18-02-2012
43
3
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Tuyển tập báo cáo các nghiên cứu khoa học quốc tế ngành hóa học dành cho các bạn yêu hóa học tham khảo đề tài: Research Article Multiplicity of Positive and Nodal Solutions for Nonhomogeneous Elliptic Problems in Unbounded Cylinder Domains
20p
dauphong16
18-02-2012
41
2
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Tuyển tập báo cáo các nghiên cứu khoa học quốc tế ngành hóa học dành cho các bạn yêu hóa học tham khảo đề tài: Research Article Multiple Positive Solutions for a Class of Concave-Convex Semilinear Elliptic Equations in Unbounded Domains with Sign-Changing Weights
18p
sting06
13-02-2012
49
4
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Tuyển tập các báo cáo nghiên cứu khoa học ngành toán học được đăng trên tạp chí toán học quốc tế đề tài: Nonexistence of nontrivial solutions for the p(x)-Laplacian equations and systems in unbounded domains of Rn
12p
sting03
04-02-2012
42
3
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Trong bài báo này chúng ta nghiên cứu sự tồn tại của các giải pháp yếu của vấn đề Dirichlet cho một hệ thống phương trình elliptic semilinear trên một miền không bị chặn trong Rn.
9p
phalinh21
01-09-2011
65
3
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This function is defined for all x e (-1. 1). and its range consists of all y. The arctanh x is an odd, nonperiodic. unbounded function that crosses the coordinate axes at the origin x = 0, y = 0. This is an increasing function in its domain with no points ofextremum and an inflection point at the origin. It has two vertical asymptotes: x = ±1. The graph of the function y = arctanh x is given in Fig. 2.20.
7p
phuongthanh3
28-09-2010
48
3
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This function is defined for all x e 11. +3c). and its range consists of y e [0, +30). The arccosh 3; is neither odd nor even; it is nonperiodic and unbounded. It does not cross the axis Oy and crosses the axis Ox at the point j1 = 1. It is an increasing function in its domain with the minimal value y = 0 at x = 1. The graph of the function y = arccosh x is given in Fig. 2.19.
7p
phuongthanh3
28-09-2010
74
3
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