共查询到10条相似文献,搜索用时 109 毫秒
1.
This paper extends the Lagrangian globalization (LG) method to the nonsmooth equation
arising from a nonlinear complementarity problem (NCP) and presents a descent algorithm for the LG phase. The aim of this paper is not to present a new method for solving the NCP, but to find
such that
when the NCP has a solution and
is a stationary point but not a solution. 相似文献
2.
In this paper geodesically corresponding metricsg and
on a manifoldM, dim 5, under the assumption that the tensorsR andS of the metricg satisfyR.R=Q(S, R), are considered. It is stated that the corresponding tensors
and
of
not necessarily must satisfy
. Certain relations between the curvatures ofg and
are obtained.Supported by a post-doctoral fellowship of the researchcouncil of the KU Leuven; Bitnet FGBDA3O at BLEKUL11 相似文献
3.
Ivan Singer 《Mathematical Methods of Operations Research》1996,43(1):35-44
By [6], the dualities between
and
, whereX andW are two sets and
(i.e., the mappings
satisfying
for all
and all index setsI), can be represented with the aid of functions
. Here we show that they can be also represented with the aid of functions
, whereR = (–, +). As an application, we show that every duality
is completely determined by a suitable duality between 2
X ×R
and 2
W ×R
(i.e., a mapping 2
X ×R
2
W ×R
satisfying
for all {M
i}
iI
2
X ×R
and all index setsI), applied to the epigraphs of the functions
. 相似文献
4.
I. M. Longman 《Journal of Optimization Theory and Applications》1976,19(3):487-497
A function
(p) of the Laplace transform operatorp is approximated by a finite linear combination of functions
(p+
r
), where
(p) is a specific function ofp having a known analytic inverse (t), and is chosen in accordance with various considerations. Then parameters
r
,r=1, 2,...,n, and then corresponding coefficientsA
r
of the
(p +
r
) are determined by a least-square procedure. Then, the corresponding approximation to the inversef(t) of
(p) is given by analytic inversion of
r=1
n
A
r
(p+
r
). The method represents a generalization of a method of best rational function approximation due to the author [which corresponds to the particular choice (t)1], but is capable of yielding considerably greater accuracy for givenn.The computations for this paper were carried out on the CDC-6600 computer at the Computation Center of Tel-Aviv University. The author is grateful to Dr. H. Jarosch of the Weizmann Institute of Science Computer Center for use of their Powell minimization subroutine (Ref. 1). 相似文献
5.
In this paper, we suggest a new functional approach to the study of group classes which enables us to describe all formations and Fitting classes of finite groups in the language of functions. The notions of
-fibered formation and of
-fibered Fitting class with direction are introduced. A direction is defined as a mapping of the set
of all primes into the set of all nonempty Fitting formations. The existence of infinitely many mappings of this kind makes it possible to construct new forms of formations and Fitting classes for a given nonempty set
. In particular, an
-local formation is an
-fibered formation with a direction such that
for any prime p. In the paper we study some basic properties of
-fibered formations and of
-fibered Fitting classes with direction and obtain the structure of their minimal satellites for a given . 相似文献
6.
Prof. Dr. E. Binz 《Monatshefte für Mathematik》1980,89(4):275-288
OnE(M,
n
), the Fréchet-manifold of all smooth embeddings of a smooth, compact, closed, orientable manifoldM (of dimensionn-1) into
n
two natural metricsG and
are considered. The metric
plays a central rôle in elasticity theory. Using a generalised notion of the Fréchet derivative their respective spraysS and
and the correspoonding Levi-Civita connections are computed. BothS and
are smooth in a well defined sense. In contrast toS the spray
turns out to be trivial. 相似文献
7.
The following hider-seeker zero-sum game is considered. The hider hides a needle of length
, in the closed unit square, and the seeker tries to locate it by shooting in a straight line across the square. The payoff to the seeker is 1 if he hits the needle and 0 otherwise.A solution of the game is obtained when
or whena lies in either of the intervals
and
; in addition, it is shown that, whenn is a positive integer anda=1/n, the value of the game is 1/2n. The properties of the solutions are in marked contrast to those for the analogous game over the closed unit disc, which the authors solved in a previous paper, and suggest that a complete solution may well be difficult. It is also shown that every member of a whole class of haystack games has a value. 相似文献
8.
Zusammenfassung Es wird die Fortpflanzung elastisch-plastischer Spannungswellen in einem unendlichen Medium betrachtet, welches einer idealen Spannungs-Verformungs-Kurve folgt, Trescas Fliesskriterium unterworfen ist und einen sphärischen Hohlraum enthält, wobei an der Fläche des Hohlraumes ein Stoss
angenommen wird. Ein rechnerisches Verfahren, basiert auf endliche Differenzen, wird entwickelt and ein Beispiel gegeben.
Notation radial stress - tangential stress - K yield stress - rr non-dimensional radial stress ( /K) - non-dimensional tangential stress ( /K) - , Lame's constants - K b Bulk constant (=(3+2)/3) - v Poisson's constant - Material density - C Elastic wave velocity (=((+2)/)1/2) - C p Plastic wave velocity (=(K b /)1/2) - distance from center of cavity - r 0 cavity radius - v non-dimensional radial co-ordinate (= /r 0) - time - t non-dimensional time (=C /r 0) - radial displacement - u non-dimensional radial displacement (=/r 0) - particle velocity - v non-dimensional particle velocity (= /C) - pressure - P(t) non-dimensional pressure (= /K) 相似文献
Notation radial stress - tangential stress - K yield stress - rr non-dimensional radial stress ( /K) - non-dimensional tangential stress ( /K) - , Lame's constants - K b Bulk constant (=(3+2)/3) - v Poisson's constant - Material density - C Elastic wave velocity (=((+2)/)1/2) - C p Plastic wave velocity (=(K b /)1/2) - distance from center of cavity - r 0 cavity radius - v non-dimensional radial co-ordinate (= /r 0) - time - t non-dimensional time (=C /r 0) - radial displacement - u non-dimensional radial displacement (=/r 0) - particle velocity - v non-dimensional particle velocity (= /C) - pressure - P(t) non-dimensional pressure (= /K) 相似文献
9.
T. I. Seidman 《Journal of Optimization Theory and Applications》1980,30(4):535-547
One standard approach to solvingf(x)=b is the minimization of f(x)–b2 overx in
, where
corresponds to a parametric representation providing sufficiently good approximation to the true solutionx*. Call the minimizerx=A(
). Take
=
N
for a sequence {
N
} of subspaces becoming dense, and so determine an approximating sequences {x
N
A (
N
)}. It is shown, withf linear and one-to-one, that one need not havex
Nx* iff
–1 is not continuous.This work was supported by the US Army Research Office under Grant No. DAAG-29-77-G-0061. The author is indebted to the late W. C. Chewning for suggesting the topic in connection with computing optimal boundary controls for the heat equation (Ref. 2). 相似文献
10.
Self-bounded controlled invariant subspaces: A straightforward approach to constrained controllability 总被引:1,自引:0,他引:1
A lattice-type structure is shown to exist in a particular subset of the set of all (A, )-controlled invariants contained in
and containing
, whereA denotes a linear map inR
n
; ,
are arbitrary subspaces ofR
n
; andD is an arbitrary subspace ofJ, the maximum (A, )-controlled invariant contained in
. In linear system theory, this property can be used for a more direct theoretical and algorithmic approach to constrained controllability and disturbance rejection problems. 相似文献