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排序方式: 共有57条查询结果,搜索用时 15 毫秒
51.
B. Bialecki M. Ganesh K. Mustapha 《Numerical Methods for Partial Differential Equations》2005,21(5):918-937
We propose and analyze an application of a fully discrete C2 spline quadrature Petrov‐Galerkin method for spatial discretization of semi‐linear parabolic initial‐boundary value problems on rectangular domains. We prove second order in time and optimal order H1 norm convergence in space for the extrapolated Crank‐Nicolson quadrature Petrov‐Galerkin scheme. We demonstrate numerically both L2 and H1 norm optimal order convergence of the scheme even if the nonlinear source term is not smooth. © 2005 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq, 2005. 相似文献
52.
G Viesti M Lunardon D Fabris G Nebbia M Cinausero E Fioretto G Prete JB Natowitz K Hagel R Wada 《Pramana》1999,53(3):395-404
The transition of the level density parameter a
off from the low excitation energy value a
off=A/8 MeV−1 to the Fermi gas value a
FG ∼ A/15 MeV−1 was discovered a few years ago studying particle spectra evaporated from hot compound systems of A∼ 160. A number of experiments have been recently performed to confirm the earlier findings and extend the investigation to
other mass regions and to higher excitation energies. Furthermore, precision coincidence experiments have been done in the
lead region in which evaporation residues are tagged by low energy gammarays. Those experiments open the possibility of a
detailed study of the level densities in nuclei where the shell effects are important. 相似文献
53.
Bernard Bialecki & Ryan I. Fernandes 《advances in applied mathematics and mechanics.》2013,5(4):461-476
The alternating direction implicit (ADI) method
is a highly efficient technique for solving multi-dimensional time dependent initial-boundary value problems on
rectangles.
When the ADI technique is coupled with orthogonal spline collocation
(OSC) for discretization in space, we not only obtain the global
solution efficiently, but the discretization error with respect to space
variables can be of an arbitrarily high order. In [2],
we used a Crank Nicolson ADI OSC method for solving general nonlinear parabolic
problems with Robin's boundary conditions on rectangular
polygons and demonstrated numerically the accuracy in various norms.
A natural
question that arises is: Does this method have an extension to non-rectangular regions? In this paper, we present a simple idea of how the
ADI OSC technique can be extended to some such regions. Our approach depends on the
transfer of Dirichlet boundary conditions in the solution of
a two-point boundary value problem (TPBVP).
We illustrate our idea for the solution of the heat equation on the unit disc
using piecewise Hermite cubics. 相似文献
54.
JB Pendry 《Contemporary Physics》2013,54(3):191-202
Light bends the wrong way in materials where both ε and μ are negative as was pointed out in 1968, but the absence of natural materials with this property led to neglect of the subject until 1999 when it was shown how to make artificial materials, metamaterials, with negative μ. The rapid advance of the subject since that date, both in theory and experiment, is reflected in the exponential growth of publications now at the 200 per year level and still growing. This interest is explained by the sudden availability of a qualitatively different class of electromagnetic materials combined with the quite startling properties which these materials appear to have; all of which provokes debate as each new facet of their behaviour is revealed. Experiment has been vital to resolution of controversy and has chiefly been in the microwave region of the spectrum though there is potential in the optical region currently being explored by several groups. 相似文献
55.
Regularity of solutions to a reaction–diffusion equation on the sphere: the Legendre series approach 下载免费PDF全文
Slawomir Bialecki Bogdan Kaźmierczak Dominika Nowicka Je‐Chiang Tsai 《Mathematical Methods in the Applied Sciences》2017,40(14):5349-5369
In the paper, we study some ‘a priori’ properties of mild solutions to a single reaction–diffusion equation with discontinuous nonlinear reaction term on the two‐dimensional sphere close to its poles. This equation is the counterpart of the well‐studied bistable reaction–diffusion equation on the Euclidean plane. The investigation of this equation on the sphere is mainly motivated by the phenomenon of the fertilization of oocytes or recent studies of wave propagation in a model of immune cells activation, in which the cell is modeled by a ball. Because of the discontinuous nature of reaction kinetics, the standard theory cannot guarantee the solution existence and its smoothness properties. Moreover, the singular nature of the diffusion operator near the north/south poles makes the analysis more involved. Unlike the case in the Euclidean plane, the (axially symmetric) Green's function for the heat operator on the sphere can only be represented by an infinite series of the Legendre polynomials. Our approach is to consider a formal series in Legendre polynomials obtained by assuming that the mild solution exists. We show that the solution to the equation subject to the Neumann boundary condition is C1 smooth in the spatial variable up to the north/south poles and Hölder continuous with respect to the time variable. Our results provide also a sort of ‘a priori’ estimates, which can be used in the existence proofs of mild solutions, for example, by means of the iterative methods. Copyright © 2017 John Wiley & Sons, Ltd. 相似文献
56.
Bernard Bialecki 《Numerische Mathematik》1990,57(1):263-269
Summary A Sinc quadrature rule is presented for the evaluation of Hadamard finite-part integrals of analytic functions. Integration over a general are in the complex plane is considered. Special treatment is given to integrals over the interval (–1,1). Theoretical error estimates are derived and numerical examples are included. 相似文献
57.