New PDF release: An introduction to granular flow

By K. Kesava Rao

ISBN-10: 0521571669

ISBN-13: 9780521571661

The circulation of granular fabrics comparable to sand, snow, coal, and catalyst debris is usual prevalence in average and commercial settings. The mechanics of those fabrics isn't really good understood. they're very important due to the fact that a wide fraction of the fabrics dealt with and-processed within the chemical, metallurgical, pharmaceutical, and foodstuff processing industries are granular in nature. This publication describes the theories for granular movement established commonly on continuum versions even if replacement discrete types also are mentioned in short. the extent is suitable for complex undergraduates or starting graduate scholars. The objective is to notify the reader approximately saw phenomena, a few on hand types, and their shortcomings and to go to a few concerns that stay unresolved. there's a number of difficulties on the finish of the chapters to motivate exploration, and large references are given
''This booklet describes the theories for granular move dependent commonly on continuum versions, even supposing replacement discrete types also are mentioned in brief. the extent is suitable for complex undergraduates or starting graduate scholars. The objective is to notify the reader approximately saw phenomena and a few on hand versions and their shortcomings and to go to a few matters that stay unresolved. there's a collection of difficulties on the finish of the chapters to inspire exploration, and large references are given.''--BOOK JACKET.  Read more... conception for sluggish aircraft circulation -- stream via hoppers -- circulation via wedge-shaped bunkers -- conception for sluggish third-dimensional stream -- circulation via axisymmetric hoppers and bunkers -- conception for fast stream of tender, inelastic debris -- research of fast move in easy geometries -- conception for quick move of tough, inelastic debris -- Hybrid theories

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Let us first discuss the case p = 0. The flow rate obtained using the bare hopper, shown by the square in Fig. 10b, is about seven times lower than the value obtained using the hopper–standpipe combination. The reason for the enhanced flow rate in the latter case can be understood by examining the profiles of the pressure of the interstitial air. Fig. 11. Profile of the dimensionless pressure p of the interstitial air for (a) the point on the upper branch of the curve shown in Fig. 4: ◦, data of Chen et al.

10. (a) A standpipe connected to a hopper. The pressure of the air is pa at the top of the hopper and pb at the bottom of the pipe. (b) Variation of the dimensionless mass flow rate V with the dimensionless pressure rise p ≡ pb − pa for the flow of sand: ◦, data of Chen et al. (1984); —, curve drawn to guide the √ eye. Here pa and pb are the dimensionless air pressures. The mass flow rate is scaled by ρp ν0 π r 2p g r p and the pressure by ρp ν0 g L, where ρp is the particle diameter, g is the acceleration due to gravity, r p and L are the inner radius and length of the pipe, respectively, and ν0 is the solids fraction of a moving bed of particles.

Let us select the configuration of the body at some time t0 as a reference configuration. Consider a Cartesian coordinate system in the laboratory frame. With respect to this coordinate system, the material point P in the reference configuration A (Fig. 27) corresponds to the position vector X. The components X 1 , X 2 , and X 3 of X are called the material coordinates of the material point P. Thus material points can be uniquely identified by the corresponding position vectors in the reference configuration or equivalently, by their material coordinates.

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An introduction to granular flow by K. Kesava Rao


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