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Circular flat plate

Fractionating Trays Circular flat plates bolted, welded or clamped to rings on the inside of fractionation columns. Used to obtain vapor liquid contact, which results in fractionation. [Pg.458]

Circular flat plate, simply supported around circumference, load applied at the center of the plate. To calculate the maximum deflection for a circular flat plate simply supported around the circumference when a load is applied at the center of the plate, use... [Pg.30]

Referring U Fig. 2..3 and considering it tt> repri sen( a strip in a circular plate, we find that the dishing t f a circular flat plate under unifonn pressure will r ult in curvatures in both the x and z directions. In reference to Etp 2.6 the unit strains niav wfitlen ... [Pg.100]

The maximum l>eudiiig moment occurs at the center of the circular flat plate when r = 0 therefore... [Pg.103]

The sample under test is held in the gap between two identical circular flat plates. The gap between the two plates can be varied, typically up to 5 mm for plates of about 25 mm radius. [Pg.158]

CIRCULAR FLAT PLATES AND HEADS WITH UNIFORM... [Pg.148]

Circular Flat Plates and Heads with Uniform Loading... [Pg.369]

When the circular flat plate is loaded under unifonn pressure p over the entire surface, simplified equations of stress are... [Pg.505]

In order to predict Lhe transition point from stable streamline to stable turbulent flow, it is necessary to define a modified Reynolds number, though it is not clear that the same sharp transition in flow regime always occurs. Particular attention will be paid to flow in pipes of circular cross-section, but the methods are applicable to other geometries (annuli, between flat plates, and so on) as in the case of Newtonian fluids, and the methods described earlier for flow between plates, through an annulus or down a surface can be adapted to take account of non-Newtonian characteristics of the fluid. [Pg.121]

Equation (8.12) is a form of the convective dijfusion equation. More general forms can be found in any good textbook on transport phenomena, but Equation (8.12) is sufficient for many practical situations. It assumes constant diffusivity and constant density. It is written in cylindrical coordinates since we are primarily concerned with reactors that have circular cross sections, but Section 8.4 gives a rectangular-coordinate version applicable to flow between flat plates. [Pg.271]

To ensure an apples-to-apples comparison, reduce kt until aoutlatn matches the value of 0.44321 achieved in the tube. This is found to occur at A t = 0.9311. Diffusion is now added until ,/ ,>, = 0.43849 as in the case of a circular tube with F/7 = 0.003. This is found to occur at about SiaVY = 0.008. Thus, the flat-plate counterpart to the Merrill and Hamrin criterion is... [Pg.287]

Viscometric flows used for measurements include well known flows, such as flow in a narrow gap concentric cylinder device and between a small angle cone and a flat plate. In both of these cases the flows established in these devices approximate almost exactly simple shearing flow. There are other viscometric flows in which the shear rate is not constant throughout, these include the wide gap concentric cylinder flow and flow in a circular pipe, discussed above. [Pg.387]

The average heat-transfer coefficient from horizontal flat plates is calculated with Eq. (7-25) and the constants given in Table 7-1. The characteristic dimension for use with these relations has traditionally [4] been taken as the length of a side for a square, the mean of the two dimensions for a rectangular surface, and 0.9d for a circular disk. References 52 and 53 indicate that better agreement with experimental data can be achieved by calculating the characteristic dimension with... [Pg.342]

Let us therefore discuss about spatial instability of parallel flows, mainly the flow past a flat plate at zero angle of attack- a problem that enjoys a canonical status for instability analyses. For the spatial instability problem associated with two-dimensional disturbance held of two-dimensional primary flows, the disturbance quantities will have the appearance of Eqn. (2.3.28) with /3 = 0. Thus for a fixed Re, one would be looking for complex a when the shear layer is excited by a fixed frequency source of circular frequency, lvq- If we define Re in terms of the displacement thickness S as the length scale, then Re = and the results obtained will be plotted as contours of constant amplification rates Oj in Re — lvo)— plane, as shown in Fig. 2.2. [Pg.43]

Kendall (1987) performed experiments in which a circular cylinder was rotated in a circular trajectory above a flat plate shear layer to create a convecting periodic disturbance source. The speed of convection of these vortices was controlled and it was demonstrated that the underlying shear layer was strongly receptive to imposed disturbances in a narrow range of convecting speed around c = 0.317oo- In the receptive range, the response field consisted of wave packets composed of many TS waves. In this experiment the disturbance (cause) always stayed outside the shear layer. [Pg.99]

Consider the following flow field over a flat plate that is excited simultaneously at the wall y = 0 and at the free stream y = Y) as shown in Fig.2.24, where Y is significantly larger than the boundary layer thickness. At the wall, a time-periodic blowing-suction device is placed at x = xq defined in a coordinate system fixed at the leading edge of the plate. The circular frequency of excitation of the wall device is lvq such that the transverse velocity oscillation at the wall is set up as. [Pg.100]

It is always important to design a laboratory reactor that has the simplest mathematical representation for both the mass and the radiation balance. In this case the work was carried out in a flat plate reactor with circular windows made of quartz. A removable shutter permits to obtain steady-state operation of the whole system (including lamps) before the run commences. The start of the reaction (f = 0) occurs when it is taken off. Other features are described in Figures 11 and 12 and Table 6. Details on all the experimental procedure can be foimd in Labas et al. (2002). [Pg.251]

Flat plate. Batch, with a recycle. Two circular windows made of quartz, Suprasil quality 69.9 cm ... [Pg.253]

The segmental, or chord downcomer, shown in Figure 11.26a is the simplest and cheapest form of construction and is satisfactory for most purposes. The downcomer channel is formed by a flat plate, called an apron, which extends down from the outlet weir. The apron is usually vertical but may be sloped (see Figure 11.26b) to increase the plate area available for perforation. If a more positive seal is required at the downcomer at the outlet, an inlet weir can be fitted (see Figure 11.26c) or a recessed seal pan used (see Figure 11.26d). Circular downcomers (pipes) are sometimes used for small liquid flow rates. [Pg.715]


See other pages where Circular flat plate is mentioned: [Pg.11]    [Pg.11]    [Pg.84]    [Pg.100]    [Pg.231]    [Pg.11]    [Pg.11]    [Pg.84]    [Pg.100]    [Pg.231]    [Pg.233]    [Pg.59]    [Pg.68]    [Pg.408]    [Pg.190]    [Pg.285]    [Pg.564]    [Pg.68]    [Pg.14]    [Pg.113]    [Pg.285]    [Pg.134]    [Pg.111]    [Pg.122]    [Pg.225]    [Pg.35]    [Pg.286]    [Pg.563]    [Pg.348]    [Pg.57]    [Pg.72]   
See also in sourсe #XX -- [ Pg.30 ]




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