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81.
Let Hnr be the number of n × n matrices, with nonnegative integer elements, all of whose row and column sums are equal to some prescribed integer r. Similarly, let Anr be the number of n × n (0.1) matrices with common row and column sum r. An asymptotic formula for Hnr is stated and proved, the method of proof being essentially elementary. A simple modification of the proof yields an analogous asymptotic formula for Anr. The latter agrees with a result of O'Neil, obtained by a completely different method. 相似文献
82.
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85.
A circuit space is an independence space (or matroid) in which each basis is contained in a circuit. In this paper we consider various independence spaces associated with a graph and seek to discover for which graphs these spaces are circuit spaces and, in particular, truncated spaces. Some definitive results are obtained and some interesting questions are left open. 相似文献
86.
Prof. Everett C. Dade 《Mathematische Zeitschrift》1971,119(4):345-348
Sans résumé 相似文献
87.
Evidence is presented to show that the gross features of the pion distributions in p and e annihilation are essentially the same. 相似文献
88.
Everett Jones 《Zeitschrift für Angewandte Mathematik und Physik (ZAMP)》1973,24(4):565-580
An existing one-dimensional mathematical model, for the arterial tree was extended to include the effects of radial variation of axial fluid velocity by the application of an integral technique. The resulting formulation reduced to a system of characteristics equations similar, in form to the equations for the onedimensional model and the computer program was modified to accommodate the integral formulation. The need for a kinematic boundary condition on the axial component of wall velocity was demonstrated. Results were obtained for a variety of velocity profiles. It was found that the slope of the front and back of the waves as well as the wave, amplitude are sensitive to changes in the velocity profile and the axial component of wall velocity. The velocity of the waves is also effected but not significantly.
Nomenclature a local internal radius of the vessel - a f , A f constants in the cosine profile - b defined by equation (22) - local normal and tangential unit vectors (see Figure 1) - f(r/a), g (z,t) defined by equation (9) - f R friction factor - local mass flux into the vessel - p local pressure - p c capillary pressure - p o pressure at the terminal end - r, z radial and axial coordinates - S local cross sectional area - t time - flow velocity at the wall interface - u, v, w radial, circumferential and axial components of flow velocity - u w , v w , w w radial, circumferential and axial components of flow velocity at the wall interface - wall velocity at the interface - U w , W w radial and axial components of wall velocity at the interface - W mass average flow velocity defined by equation (13) - w o maximum flow velocity - 0, 1, 2, 3 parameters defined by equation (10) - 4 W w /w w - A , B , C parameters defined by equation (18) - outflow parameter - wave length - L Lagrangian multiplier - viscosity coefficient for the fluid - density of the fluid - kinematic viscosity - ()' nondimensional quantity of order one - ()+, ()– values of () associated with roots of equation (23) This analysis was initiated during the authors appointment as a NASA-ASEE Summer Faculty Fellow to the Stanford-Ames Program and completed through the facilities of the Computer Science Center at the University of Maryland. 相似文献
Zusammenfassung Die eindimensionale Theorie von Anliker et al. (ZAMP22, 217 (1971)) wird in dieser Arbeit dahingehend erweitert, dass der Einfluss des Geschwindigkeitsprofiles mitberücksichtigt wird. Die Navier-Stokes-Gleichungen und die Kontinuitätsgleichung werden mit Hilfe einer Integraltechnik auf ähnliche, für die Rechnung mit dem Computer geeignete Gleichungen zurückgeführt, wie sie von Anliker et al. verwendet wurden. Die charakteristischen Grössen des Geschwindigkeitsprofiles sowie die Geschwindigkeit der Gefässwand gehen als Parameter in die Theorie ein, so dass parametrische Studien durchgeführt werden können.
Nomenclature a local internal radius of the vessel - a f , A f constants in the cosine profile - b defined by equation (22) - local normal and tangential unit vectors (see Figure 1) - f(r/a), g (z,t) defined by equation (9) - f R friction factor - local mass flux into the vessel - p local pressure - p c capillary pressure - p o pressure at the terminal end - r, z radial and axial coordinates - S local cross sectional area - t time - flow velocity at the wall interface - u, v, w radial, circumferential and axial components of flow velocity - u w , v w , w w radial, circumferential and axial components of flow velocity at the wall interface - wall velocity at the interface - U w , W w radial and axial components of wall velocity at the interface - W mass average flow velocity defined by equation (13) - w o maximum flow velocity - 0, 1, 2, 3 parameters defined by equation (10) - 4 W w /w w - A , B , C parameters defined by equation (18) - outflow parameter - wave length - L Lagrangian multiplier - viscosity coefficient for the fluid - density of the fluid - kinematic viscosity - ()' nondimensional quantity of order one - ()+, ()– values of () associated with roots of equation (23) This analysis was initiated during the authors appointment as a NASA-ASEE Summer Faculty Fellow to the Stanford-Ames Program and completed through the facilities of the Computer Science Center at the University of Maryland. 相似文献
89.
Penetration of epidermis by ultraviolet rays 总被引:10,自引:0,他引:10
90.
Prof. Everett C. Dade 《Mathematische Zeitschrift》1970,117(1-4):35-40
Sans résuméDédié au Prof. H. Wielandt à l'occasion de son 60e anniversaire le 19.12.1970 相似文献