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Moving load/mass

Counterbalanced Trucks. The counterbalanced trucks (Fig. 4.42) use their large, carefully positioned weight mass to offset (counterbalance) the moved load mass.These trucks are generally equipped with a tilting mast which will tilt the Ufting mechanism rearward from the vertical Uftog position and further counterbalance the load during movement. The load is positioned fuUy in front of the truck so that the truck structure does not interfere with adjacent stacks of material.This minimizes the aisle widths that are required. [Pg.215]

Typically, rapid repair of main cracks in slabs is realized using bituminous masses covering only the damages. Unfortunately, this kind of protection is ineffective just after few months of exploitation, because the degraded mass (Fig. 2b, 2c) allows for infiltration of water under slabs [8]. The coming into being hydrodynamic pump effect (due to moving loads - Fig. 3a) destructs sealants in joints (Fig. 3b) and causes uneven settlement of concrete slabs (Fig. 3c). The solution of this problem is the use of special polymer flexible joints. [Pg.227]

In (Eqs 23-27), the scalars x and t denote spatial coordinate and time, respectively. The symbols u, M and P signify the transverse displacement, the moment, and the moving load, respectively. Furthermore, m represents the distributed mass of the beam, fx the moving mass, and c t) its prescribed velocity in time. It has been assumed that the motion of the discrete moving mass begins at a zero initial time and from an initial location xq on the beam. Finally, S denotes the spatial Dirac s delta function. In order to deal with inelastic behavior, the set of equations 23-27 is supplemented by the state equations and the flow rule. [Pg.158]

The sediment load of a channel and the sediment yield of its drainage basin are expressed in different ways. The sediment load is the total mass of material moved by the river in a... [Pg.179]

Owing to the high computational load, it is tempting to assume rotational symmetry to reduce to 2D simulations. However, the symmetrical axis is a wall in the simulations that allows slip but no transport across it. The flow in bubble columns or bubbling fluidized beds is never steady, but instead oscillates everywhere, including across the center of the reactor. Consequently, a 2D rotational symmetry representation is never accurate for these reactors. A second problem with axis symmetry is that the bubbles formed in a bubbling fluidized bed are simulated as toroids and the mass balance for the bubble will be problematic when the bubble moves in a radial direction. It is also problematic to calculate the void fraction with these models. [Pg.342]

Move Operations to Balance Mass Load as Evenly as Possible Below the Reuse Only Pinch... [Pg.614]

The technique was then changed to entrap a small mass of water under a molten aluminum surface and simultaneously to overpressure the system. In this manner it was hoped to collapse steam films around the water. The actual procedure employed a small glass sphere containing water. The sphere was moved beneath the aluminum surface and broken by impulsively loading the system from a falling steel cylinder which impacted on a graphite toroid immediately above the molten aluminum. About 0.7 g of water was released into I kg of aluminum at 1170 K and pressurized to about 8 MPa. No explosions were detected. [Pg.168]

Before moving on to true mass transport issues it is worthwhile to point out that the quantity vep(Y - Yp) is in fact the water load per unit of time (whichever units of time v is expressed in.) Further that with an a-priori design process we may not know the required cross sectional area for flow and hence it may be more convenient to multiply the above relationship by and thus obtain the adsorbable contaminant input rate ... [Pg.282]

The first effect may be very serious. Where a balance or dead weight is used to determine the loading press, a rapid ram movement can result in a force due to acceleration of the masses moved which may vary from a substan-tail fraction to several times the force due to gravity. Analyses of some loading operations have revealed that the true loading press was three or four times that intended... [Pg.610]

We first give a rather general mass-transfer model, which is useful for most processes of porous-solid extraction with dense gases. Two cases are possible [43] for a single particle loaded with solute. In (a), the solute is adsorbed over the internal surface of the particle, and is desorbed from the sites and diffuses out to the external surface, (b) The solute fills in the pore-cavities completely, and is dissolved from an inner core that moves progressively to the centre of the particle. [Pg.126]


See other pages where Moving load/mass is mentioned: [Pg.150]    [Pg.150]    [Pg.162]    [Pg.22]    [Pg.149]    [Pg.639]    [Pg.1124]    [Pg.88]    [Pg.328]    [Pg.90]    [Pg.480]    [Pg.161]    [Pg.1922]    [Pg.2042]    [Pg.311]    [Pg.60]    [Pg.129]    [Pg.512]    [Pg.1057]    [Pg.863]    [Pg.80]    [Pg.247]    [Pg.244]    [Pg.245]    [Pg.246]    [Pg.296]    [Pg.297]    [Pg.332]    [Pg.375]    [Pg.181]    [Pg.317]    [Pg.118]    [Pg.119]    [Pg.261]    [Pg.112]    [Pg.222]    [Pg.219]    [Pg.399]    [Pg.605]    [Pg.328]    [Pg.171]   
See also in sourсe #XX -- [ Pg.150 , Pg.158 , Pg.195 ]




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Loading, mass

Moving loads

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