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Two-fluid

This method utilizes essentially the concept developed by Fitzer in 1955. According to the principle of three-parameter corresponding states, the compressibility factor z, for a fluid of acentric factor w, is obtained by interpolating between the compressibilities Zj and Z2 for the two fluids having acentric factors w, and (p -... [Pg.119]

Surface sampling involves taking samples of the two phases (gas and liquid) flowing through the surface separators, and recombining the two fluids in an appropriate ratio such that the recombined sample is representative of the reservoir fluid. [Pg.113]

Finally, it is worth remembering the sequence of events which occur during hydrocarbon accumulation. Initially, the pores in the structure are filled with water. As oil migrates into the structure, it displaces water downwards, and starts with the larger pore throats where lower pressures are required to curve the oil-water interface sufficiently for oil to enter the pore throats. As the process of accumulation continues the pressure difference between the oil and water phases increases above the free water level because of the density difference between the two fluids. As this happens the narrower pore throats begin to fill with oil and the smallest pore throats are the last to be filled. [Pg.124]

The above experiment was conducted for a single fluid only. In hydrocarbon reservoirs there is always connate water present, and commonly two fluids are competing for the same pore space (e.g. water and oil in water drive). The permeability of one of the fluids is then described by its relative permeability (k ), which is a function of the saturation of the fluid. Relative permeabilities are measured in the laboratory on reservoir rock samples using reservoir fluids. The following diagram shows an example of a relative permeability curve for oil and water. For example, at a given water saturation (SJ, the permeability... [Pg.202]

When the radial flow of fluid towards the wellbore comes under the localised influence of the well, the shape of the interface between two fluids may be altered. The following diagrams show the phenomena of coning and cuspingoi water, as water is displacing oil towards the well. [Pg.217]

The LMTD, ie, logarithmic mean temperature difference, is an effective overall temperature difference between the two fluids for heat transfer and is a function of the terminal temperature differences at both ends of the heat exchanger. [Pg.486]

Optimum heat-transfer results when the thermal capacity rates of the two fluid streams are balanced, ie, where or = 1.0. [Pg.488]

Direct Contact Heat Exchangers. In a direct contact exchanger, two fluid streams come into direct contact, exchange heat and maybe also mass, and then separate. Very high heat-transfer rates, practically no fouling, lower capital costs, and lower approach temperatures are the principal advantages. [Pg.495]

Fig. 23. Viscosity vs shear rate curves for two fluids showing the fallacy of a single point measurement. Fluid Vl would appear to be more viscous than fluid B if measured only at point X, of the same viscosity if measured at point V, and less viscous if measured only at point Z. Fig. 23. Viscosity vs shear rate curves for two fluids showing the fallacy of a single point measurement. Fluid Vl would appear to be more viscous than fluid B if measured only at point X, of the same viscosity if measured at point V, and less viscous if measured only at point Z.
The Bechtel confined zone dispersion (BCZ) process involves the injection of a fine slurry mist of pressure hydrated dolomitic lime or calcitic lime, using two-fluid atomizing nozzles. A demonstration at the 70 MWe Seward Station of the Pennsylvania Electric Co., performed in 15.2 m of ductwork with a 2.4-m by 3.4-m cross section, achieved a 50% removal of SO2 at a Ca S ratio around 1.1. [Pg.261]

The measurement of level can be defined as the determination of the location of the interface between two fluids, separable by gravity, with respecl to a fixed datum plane. The most common level measurement is that of the interface between a liquid and a gas. Other level mea-... [Pg.763]

Float-Actuated Devices Float-actuated devices are characterized by a buoyant member that floats at the interface between two fluids. Since a significant force is usually required to move the indicating mechanism, float-actuated devices are generally limited to liqiiid-gas interfaces. By properly weighting the float, they can be used to measure hquid-liquid interfaces. Float-actuated devices may be classified on the basis of the method used to couple the float motion to the indicating system as discussed below. [Pg.763]

Thermal Methods Level-measuring systems may be based on the difference in thermal characteristics oetween the fluids, such as temperature or thermal conductivity. A fixed-point level sensor based on the difference in thermal conductivity between two fluids consists of an electrically heated thermistor inserted into the vessel. The temperature of the thermistor and consequently its electrical resistance increase as the thermal conductivity of the fluid in which it is immersed decreases. Since the thermal conductivity of liquids is markedly higher than that of vapors, such a device can be used as a point level detector for liquid-vapor interface. [Pg.764]

Two-fluid U tube (Fig. 10-14). This is a highly sensitive device for measuring small gas heads. Let A be the cross-sectional area of each of the resei voirs and a that of the tube forming the U let Pi be... [Pg.890]

Mean Temperature Differenee The temperature difference between the two fluids in the heat exchanger vm, in general, vaiy from point to point. The mean temperature difference (AT, or MTD) can be calculated from the terminal temperatures of the two streams if the following assumptions are valid ... [Pg.1034]

Selection of Flow Path In selecting the flow path for two fluids through an exchanger, several general approaches are used. The tube-side fluid is more corrosive or dirtier or at a higher pressure. The shell-side fluid is a liquid of high viscosity or a gas. [Pg.1065]

As the coiled plate spirals outward, the plate thickness increases from a minimum of 2 mm to a maximum (as required by pressure) up to 10 mm. This means relatively thick material separates the two fluids compared to tubing of conventional exchangers. Pressure vessel code conformance is a common request. [Pg.1085]

Two-fluid nozzles do not operate efficiently at high capacities and consequently are not used widely on plant-size spray diyers. Their chief advantage is that they operate at relatively low pressure, the hq-uid being 0 to 400 kPa/m" pressure, while the atomizing fluid is usually no more than 700 kPa/m" pressure. The atomizing fluid may be steam or air. Two-fluid nozzles nave been employed for the dispersion of thick pastes and filter cakes not previously capable of being handled in ordinaiy atomizers [Baran, Ind. Eng. Chem., 56(10), 34-36 (1964) andTurba, Brit. Chem. Eng., 9(7), 457-460 (1964)]. [Pg.1233]

For proper use of the equations, the chamber shape must conform to the spray pattern. With cocurrent gas-spray flow, the angle of spread of single-fluid pressure nozzles and two-fluid pneumatic nozzles is such that wall impingement wiU occur at a distance approximately four chamber diameters below the nozzle therefore, chambers employing these atomizers should have vertical height-to-diameter ratios of at least 4 and, more usually, 5. The discharge cone below the vertical portion should have a slope of at least 60°, to minimize settling accumulations, and is used entirely to accelerate gas and solids for entty into the exit duct. [Pg.1238]


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See also in sourсe #XX -- [ Pg.169 , Pg.196 , Pg.207 ]

See also in sourсe #XX -- [ Pg.49 , Pg.73 , Pg.97 ]




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Atomization two-fluid

Atomizer two-fluid

Bubbling Bed Reactor Simulations Using Two-Fluid Models

Constants for the Two Reference Fluids Used in Lee-Kesler ethod

Dynamic two-fluid model OLGA

Energy from Earths Two Great Fluids in Motion

Explicit Fractional Step Algorithm for Solving the Two-Fluid Model Equations Applied to Bubble Column Flow

Flow of Two Immiscible Fluids

Fluid Flow in Two and Three Dimensions

Fluid two-phase

Mixing of Two Miscible Fluids

Mixing of two fluids

One- and Two-Dimensional Fluids

Particle on the Interface Between Two Fluids

Pressure Flow of Two Immiscible Fluids with Different Viscosities

Schematic of the batch centrifuge separating two immiscible fluids

Schematic of the continuous gravity separator separating two immiscible fluids

Simulating Bubbling Bed Combustors Using Two-Fluid Models

Sizing for two-phase fluids

Solving the Two-Fluid Model Equations

The Eulerian two-fluid model

The Fluid Dynamic Storage Behaviour at 1 Bar of Two LNG or LPG Layers with Different Density

The Two-Fluid Granular Flow Model

The two-fluid model of Hell

Two-Fluid (Pneumatic) Atomizers

Two-Fluid Cocurrent Flowing Porous Media

Two-Fluid Model with Kinetic Theory of Granular Flow Closures

Two-Fluid Simulation of Gas Fluidized Beds

Two-Phase Flow Models and Computational Fluid Dynamics

Two-Phase Fluid Flow Energy Balance

Two-component Fluid

Two-dimensional fluid

Two-dimensional hard-sphere fluid

Two-fluid Model Formulation and Closure Limitations

Two-fluid equations

Two-fluid model

Two-fluid nozzles

Two-fluid reactor, design

Two-fluid systems

Two-phase fluid flow Lockhart-Martinelli method

Two-phase fluid flow correlations

Two-phase fluid flow granular beds

Two-phase fluid flow homogeneous model

Two-phase fluid flow patterns

Two-phase fluid flow pressure drop, calculation example

Two-phase fluid flow void fraction

Two-phase fluid system

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