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Dynamic pressure static

It is difficult to determine exactly the areas of localized pressure reductions inside the pump, although much research has been focused on this field. It is easy, however, to measure the total fluid pressure (static plus dynamic) at some convenient point, such as pump inlet flange, and adjust it in reference to the pump centerline location. By testing, it is possible to determine the point when the pump loses performance appreciably, such as 3% head drop, and to define the NPSH at that point, which is referred to as a required NPSH (NPSHR). The available NPSH (NPSHA) indicates how much suction head... [Pg.290]

Solid Desiccants. The sohd desiccants used in dynamic appHcations fad into a class caded adsorbents (see Adsorption). Because they are used in large packed beds through which the gas or Hquid to be treated is passed, the adsorbents are formed into soHd shapes that adow them to withstand the static (fluid plus sohd head) and dynamic (pressure drop) forces imposed on them. The most common shapes are granules, extmded pedets, and beads. [Pg.512]

Chile [Prog. Aerosp. Sc7, 16, 147-223 (1975)] reviews the use of the pitot tube and allied pressure probes for impact pressure, static pressure, dynamic pressure, flow direction and local velocity, sldn friction, and flow measurements. [Pg.885]

The effect of different pai ameters such as temperature, pressure, modifier volume, dynamic and static extraction time on the SFE of the plant were investigated. The orthogonal array experimental design method was chosen to determine experimental plan, (5 ). In this design the effect of five parameters and each at five levels were investigated on the extraction efficiency and selectivity [4]. [Pg.365]

Let s consider now a system with dynamic pressures and a constant elevation. A classic example of this would be where a pump feeds a sealed reactor vessel, or boiler. The fluid level in the reactor would be more or less static in relation to the pump. The resistances in the piping, the Hf and Hv, would be mostly static although they would go up with flow. The Hp, pressure head would change with temperature. Consider Figure 8-14. [Pg.113]

When designing air supply through a filter ceiling, one should ensure that the dynamic pressure in the supply air does not affect the static pressure distribution above the filter ceiling too much. [Pg.646]

In such openings, bidirectional flow driven by temperature differences between the two rooms can occur. If a total pressure (static pressure plus dynamic pressure) is specified, this phenomenon can be accounted for. For higher accuracy in the neighborhood of this opening, it is, however, recommended to expand the calculation domain beyond this opening. [Pg.1037]

Static The fan total pressure minus the dynamic pressure corresponding to the mean air velocity at the fan outlet. The fan static pressure is the bursting or collapsing pressure on the enclosure,... [Pg.1439]

Static head The difference between the total fluid pressure and the dynamic pressure. [Pg.1478]

Bernoulli s equation (Equation 2-53), which accounis for static and dynamic pressure losses (due to changes in velocity), but does not account for frictional pressure losses, energ losses due to heat transfer, or work done in an engine. [Pg.171]

Fluid power equipment is designed to reduce friction as much as possible. Since energy cannot be destroyed, some of the energy created by both static pressure and velocity is converted to heat energy as the fluid flows through the piping and components within a hydraulic system. As friction increases, so does the amount of dynamic and static energy that is converted into heat. [Pg.592]

During the second period, the cake grows because of the absence of flow. It may grow to a point at which it locally but completely fills the annulus Bridging takes place and the hydrostatic pressure is no longer transmitted to the deeper zones. From the typical mudcake resistance it can be estimated that under both dynamic and static conditions, the fluid loss could require reduction to an American Petroleum Institutue (API) value lower than what is generally considered a fair control of fluid loss. [Pg.36]

It must be also considered that the reaction rates of different thermal processes which can occur simultaneously are influenced by the treatment conditions (temperature, heating rate, pressure, static or dynamic atmosphere). This will affect the relative quantities of the products formed and in some cases also their nature, when recombination reactions give rise to secondary degradation products. On account of its sensitivity and resolution power Py-GC/MS will also provide useful information on minor components present in a material, including low molecular weight additives and pigments. [Pg.348]

For a fluid having a pressure P and flowing at speed v, the quantity ipv2 is known as the dynamic pressure and P+ipv2 is called the total pressure or the stagnation pressure. The pressure P of the flowing fluid is often called the static pressure, a potentially misleading name because it is not the same as the hydrostatic pressure. [Pg.17]

Dunkle (Ref 40) points out that total pressure is also known as stagnation pressure and is equal to the sum of static pressure and dynamic pressure. Both of these are exerted by gases. More detailed explanation is given in Ref 40, p 32. He also states that in the reaction between A1 K chlorate, mentioned above, the products formed at the temperature of explosion are gaseous KC1, AlO, A O and oxygen. The A Oj does not form until the products cool... [Pg.483]

Autoffettage is a useful measure for statically as well as dynamically pressurized vessels (see section 4.1.5.1). There is also a benifitial impact on the decrease of the rate of crack growth and the increase of the critical crack depth. [Pg.208]

A number of analogous compounds to BA have been reported, including 5,5 -dibenzo-[a]-pyrenyl (BBPY) [116]. These compounds exhibit emission spectra similar to BA. It would be interesting to explore the ultrafast dynamics of BBPY in order to test the generality of the GLE model. It would also be interesting to study the femtosecond dynamics of BA as a function of applied pressure. Static experiments on the emission of BA, reported by Hara et al. [123], demonstrate that in low viscosity solvents an increase of pressure affects the emission similarly to an increase of solvent polarity. As the pressure is increased, however, the LE/CT interconversion is slowed down. It would be interesting to measure C(r) in these environments and compare the solvation dynamics with LE/CT dynamics, in order to test the generality of the GLE dielectric friction model. [Pg.57]

An almost overwhelmingly large number of different techniques for measuring dynamic and static interfacial tension at liquid interfaces is available. Since many of the commercially available instruments are fairly expensive to purchase (see Internet Resources), the appropriate selection of a suitable technique for the desired application is essential. Dukhin et al. (1995) provides a comprehensive overview of currently available measurement methods (also see Table D3.6.1). An important aspect to consider is the time range over which the adsorption kinetics of surface-active substances can be measured (Fig. D3.6.5). For applications in which small surfactant molecules are primarily used, the maximum bubble pressure (MBP) method is ideally suited, since it is the only... [Pg.639]

Klaentschi, K., Brown, J.A., Niblett, P.G., Shore, A.C. and Tooke, J.E. (1998) Pressure-permeability relationships in basement membrane effects of static and dynamic pressures. Am. J. Physiol., 274, H1327-H1334. [Pg.415]

High-pressure static and dynamic light scattering were used to closely examine the behavior of block copolymers of poly(vinyl acetate) (PVAc) and poly(l,l,2,2-tetrahydroperfluoroalkyl acrylate (PTAN) as a function of C02 density (Buhler et al., 1998). The phase diagram for PVAc-6-TAN shows three distinct phases as a function of polymer concentration and C02 density at a fixed temperature of 45 °C (see Figure 9.1). The block copolymer forms a precipitated phase at low C02 densities, spherical micelles at intermediate C02 densities, and unimers, or free polymer chains in solution, at high densities. The micelles-to-unimer transition was found to be very... [Pg.159]

The formula for the pitot tube follows directly from the stagnation-pressure relation. The difference between the stagnation- and the static-pressure heads is seen to be h, which is the dynamic-pressure head. Hence for a pitot tube pointed directly upstream and in a flow without appreciable turbulence, the equation is... [Pg.427]


See other pages where Dynamic pressure static is mentioned: [Pg.23]    [Pg.295]    [Pg.886]    [Pg.75]    [Pg.202]    [Pg.748]    [Pg.428]    [Pg.117]    [Pg.301]    [Pg.296]    [Pg.17]    [Pg.138]    [Pg.181]    [Pg.30]    [Pg.254]    [Pg.11]    [Pg.579]    [Pg.351]    [Pg.673]    [Pg.344]    [Pg.486]    [Pg.60]    [Pg.64]    [Pg.765]    [Pg.428]    [Pg.295]    [Pg.31]    [Pg.673]   
See also in sourсe #XX -- [ Pg.111 ]




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