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21.
22.
D. Spence 《Colloid and polymer science》1911,9(6):300-306
Ohne Zusammenfassung 相似文献
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Ohne Zusammenfassung 相似文献
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Summary. Let ( real) be a family of real by matrices. A value of is called a Hopf value if has a conjugate pair of purely imaginary eigenvalues , . We describe a technique for detecting Hopf values based on the evolution of the Schur complement of in a bordered extension of where varies along the positive imaginary axis of the complex plane. We compare the efficiency of this method with more obvious
methods such as the use of the QR algorithm and of the determinant function of as well as with recent work on the Cayley transform. In particular, we show the advantages of the Schur complement method
in the case of large sparse matrices arising in dynamical problems by discretizing boundary value problems. The Hopf values
of the Jacobian matrices are important in this setting because they are related to the Hopf bifurcation phenomenon where steady
state solutions bifurcate into periodic solutions.
Received September 15, 1994 / Revised version received July 7, 1995 相似文献
25.
M. Fichtmüller G. Corrigan L. Lauro-Taroni R. Simonini J. Spence E. Springmann A. Taroni 《Czechoslovak Journal of Physics》1998,48(2):25-38
Several attempts to model the entire plasma cross section have been reported in the last few years. Two possibilities are to either couple a core code to a scrape-off layer (SOL) code at a specified interface or to extend the computational region of an SOL-code all the way to the plasma centre. The most advanced global code is the code COCONUT which is based on the former principle and comprises the Monte-Carlo code NIMBUS, the 2D scrape-off layer code EDGE2D, the core transport code JETTO and the core impurity transport code SANCO. A main feature of COCONUT is its modular structure which ensures a high degree of flexibility and the capability to cover a large range of time-scales. The influence of the SOL on the core is lllustrated with a range of global simulations carried out with COCONUT. The simulations show that the primary effect of the SOL is the control of the particle sources and sinks with a secondary effect on plasma dilution, radiation and perhaps pedestal temperatures. 相似文献
26.
MM. P. Duballet A. Godard G. Queguiner P. Pastour 《Journal of heterocyclic chemistry》1973,10(6):1079-1080
This article describes the synthesis of a new heterocycle, pyrido[2,3,f]phtalazine and three new diformylquinolincs. 相似文献
27.
M.G. Brereton R.A. Duckett S.H. Joseph P.J. Spence 《Journal of the mechanics and physics of solids》1977,25(2):127-136
An interpretation of yield behaviour in polymers is given in terms of the stress-activated flow of structural units over an energy barrier together with an additional correlated component to the motion. This correlated contribution takes account, in the simplest way possible, of the state of other conformations, and it is shown to lead to an effective activation-energy barrier which depends in part on the strain present at any time in the material. In this manner, the present work relates to previous work by M.G. Brereton, S.G. Croll, R.A. Duckett and I.M. Ward (1974), who, on purely phenomenological grounds, proposed a relation between stress and strain which had the form of a feedback equation. Specifically, the strain resulting from an applied stress was assumed to modify the material in a way which reduced its resistance to stress. The basic equation obtained here is non-linear and shows a yield-like behaviour resulting from a dynamical (as opposed to a geometrical) instability. Furthermore, it indicates a consistent relation between yield in creep tests and in constant strain-rate tests. 相似文献
28.
The synthesis of two new heterocycles is described: pyrido-[2,3-d]-.s-triazolo[ 3,4-f] pyrimidine and pyrido[3,2-d]-.s-triayzolo-[3,4-f] pyrimidine. 4-[I'-Pyrazolyl]pyrido[2,3-d]pyrimidines and 4-[1′-pyrazoly1] pyrido[ 3,2-d] pyrimidine are obtained by the action of 4-hydrazinopyrido[2,3-d]pyrimidine and 4-hydrazinopyrido-[3,2-d]pyrimidine with several β-diketones. 相似文献
29.
S. El‐Zanati O. Heden G. Seelinger P. Sissokho L. Spence C. Vanden Eynden 《组合设计杂志》2010,18(6):462-474
Let V = V(n, q) denote the vector space of dimension n over GF(q). A set of subspaces of V is called a partition of V if every nonzero vector in V is contained in exactly one subspace of V. Given a partition 𝒫 of V with exactly ai subspaces of dimension i for 1≤i≤n, we have , and we call the n‐tuple (an, an − 1, …, a1) the type of 𝒫. In this article we identify all 8‐tuples (a8, a7, …, a2, 0) that are the types of partitions of V(8, 2). © 2010 Wiley Periodicals, Inc. J Combin Designs 18: 462–474, 2010 相似文献
30.