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Sloping bulk materials

A bulk material which behaves in a fluid manner when very dilated, will flush out to a level surface of fill, as can be seen in Fig. 5.3, and display hydrostatic pressure conditions until settled. Poor flow materials, such as damp and cohesive powders, achieve steep filling repose angles. Therefore, appropriate allowances must be made in calculating holding volumes and fixing the location of level indicators. Coarse, firm, nonadhesive products tend to settle quickly, to form a stable bulk structure, when they come to rest after pouring. Such bulk materials attain consistent density conditions and repeatable angles of repose , virtually independent of the manner in which the slope of the pile is formed. [Pg.92]

Bulk materials that are composed of fine particulate constituents are much more sensitive to the influence of the void gas, as changes of volume are resisted by the rate at which the gas can progress through the interstices of the mass. As a result, the repose conditions are very dependent upon the conditions of slope formation, as is the density condition to which they settle. Such materials do not have a specific angle of repose , either in filling or discharge conditions, and it is misleading to ascribe a definitive... [Pg.92]

To prevent bulk materials from caving in on someone, the materials must have restraints. Options are shoring or sloping back the material to an angle more shallow than the natural... [Pg.214]

The transition to more realistic conditions, near fuel cell environment, is achieved using a thin-film rotating disk electrode with a practical supported catalyst. It allows obtaining kinetic parameters such as the the exchange current density and Tafel slopes, avoiding the use of complex models. This is of fundamental importance, because small catalyst particles having a significant fraction of surface atoms could behave differently compared to bulk materials. [Pg.269]

It must be remembered that the normal inclination of the inner diameter of the flight adjacent to the centre shaft is only about 38 when the screw axis is horizontal, so at 20° slope of the conveyor this surface reduced to about 18° to the horizontal, a slope at which many bulk materials will not slip on metal surfaces, apart from the drag induced by the centre tube and sharp corner between the flight and the tube. This also indicates how surface friction of the material on the flight face is a crucial design parameter, particularly for inclined screw conveyors (Figure 5.5). [Pg.207]

Wj = total weight of bulk material in skirtplale zones = release angle 0 feeder slope angle Fjp = skirtplate resistance. [Pg.220]

A curve relating stress to strain, in the bulk material, is plotted, and from the slope of this curve one obtains the Young s modulus for the material. A typical plot for obtaining the Young s modulus is shown in Fig. 1 ... [Pg.91]

Some typical values of the Young s modulus are shown in Table 1. Note the Young s modulus represents the slope of the stress-strain curve for elastic length deformation of a bulk material. This modulus of elasticity, as can be seen from Table 1, can be considerable, reaching a value in excess of 1.8 TPa for carbon nanotubes [4] ... [Pg.92]

Thus, a plot of ln[— ln(l — x)] versus In t yields a straight line of slope n. The value of n is important not only because it indicates the reaction order, but also because it has some physical interpretation, depending on whether the crystals are growing at the surface of a material or in the bulk (sometimes called volume crystallization). See Table 3.1 for a description of the dimension of the crystals for various values of n. The intercept of this plot gives the rate constant, k. Obtaining k at different... [Pg.221]


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See also in sourсe #XX -- [ Pg.214 ]




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