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Flow through

In situations where a low concentration of suspended solids needs to be separated from a liquid, then cross-flow filtration can be used. The most common design uses a porous tube. The suspension is passed through the tube at high velocity and is concentrated as the liquid flows through the porous medium. The turbulent flow prevents the formation of a filter cake, and the solids are removed as a more concentrated slurry. [Pg.74]

The heat flow through the system can be manipulated by changing the number of stages. Figure 3.13c shows the effect of an increase from three to six stages. [Pg.87]

The grand composite curve is obtained by plotting the problem table cascade. A typical grand composite curve is shown in Fig. 6.24. It shows the heat flow through the process against temperature. It should be noted that the temperature plotted here is shifted temperature T and not actual temperature. Hot streams are represented ATn,in/2 colder and cold streams AT iJ2 hotter than they are in practice. Thus an allowance for ATj in is built into the construction. [Pg.185]

Another design option that can be considered if a column will not fit is use of an intermediate reboiler or condenser. An intermediate condenser is illustrated in Fig. 14.5. The shape of the box is now altered because the intermediate condenser changes the heat flow through the column. The particular design shown in Fig. 14.5 would require that at least part of the heat rejected from the intermediate condenser be passed to the process. An analogous approach can be used to evaluate the possibilities for use of intermediate reboilers. Flower and Jackson," Kayihan, and Dhole and Linnhofl have presented procedures for the location of intermediate reboilers and condensers. [Pg.346]

The viscosity is determined by measuring the time it takes for a crude to flow through a capillary tube of a given length at a precise temperature. This is called the kinematic viscosity, expressed in mm /s. It is defined by the standards, NF T 60-100 or ASTM D 445. Viscosity can also be determined by measuring the time it takes for the oil to flow through a calibrated orifice standard ASTM D 88. It is expressed in Saybolt seconds (SSU). [Pg.318]

The nature of these paraffins and their concentration in diesel fuel affect the three temperatures that characterize the cold behavior. The cloud point is the temperature at which crystals of paraffins appear when the temperature is lowered. The cold filter pluming point is defined as the temperature under which a suspension no ionger flows through a standard filter. Finally, the pour point is the temperature below which the diesel fuel no longer flows by simple gravity in a standard tube. These three temperatures are defined by regulations and the refiner has three types of additives to improve the quality of the diesel fuel of winter. [Pg.353]

The production phase commences with the first commercial quantities of hydrocarbons ( first oil ) flowing through the wellhead. This marks the turning point from a cash flow point of view, since from now on cash is generated and can be used to pay back the prior investments, or may be made available for new projects. Minimising the time between the start of an exploration campaign and first oil is one of the most important goals in any new venture. [Pg.6]

Reservoir rocks are either of clastic or carbonate composition. The former are composed of silicates, usually sandstone, the latter of biogenetically derived detritus, such as coral or shell fragments. There are some important differences between the two rock types which affect the quality of the reservoir and its interaction with fluids which flow through them. [Pg.13]

The pores between the rock components, e.g. the sand grains in a sandstone reservoir, will initially be filled with the pore water. The migrating hydrocarbons will displace the water and thus gradually fill the reservoir. For a reservoir to be effective, the pores need to be in communication to allow migration, and also need to allow flow towards the borehole once a well is drilled into the structure. The pore space is referred to as porosity in oil field terms. Permeability measures the ability of a rock to allow fluid flow through its pore system. A reservoir rock which has some porosity but too low a permeability to allow fluid flow is termed tight . [Pg.13]

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]

For direct measurement from core samples, the samples are mounted in a holder and gas is flowed through the core. The pressure drop across the core and the flowrate are measured. Providing the gas viscosity (ji) and sample dimensions are known the permeability can be calculated using the Darcy equation shown below. [Pg.151]

One of the major differences in fluid flow behaviour for gas fields compared to oil fields is the mobility difference between gas and oil or water. Recall the that mobility is an indicator of how fast fluid will flow through the reservoir, and is defined as... [Pg.196]

Figure 8.14 Single fluid flowing through a section of reservoir rock... Figure 8.14 Single fluid flowing through a section of reservoir rock...
For a single fluid flowing through a section of reservoir rock, Darcy showed that the superficial velocity of the fluid (u) is proportional to the pressure drop applied (the hydrodynamic pressure gradient), and inversely proportional to the viscosity of the fluid. The constant of proportionality is called the absolute permeability which is a rock property, and is dependent upon the pore size distribution. The superficial velocity is the average flowrate... [Pg.202]

It is the indication of a transfer of energy from a distance between the solenoid and the conductor material. The cause of the variation of impedance observed is the modification of the magnetic flow through the solenoid. The flow varies in amplitude and in phase. [Pg.349]

Both coils are constructed in the same way, geometry and number of windings are equal. A permanent sinus current flows through these coils and excites an electromagnetic field around each coils. [Pg.368]

The tested blade is flowed through either with hot or cold compressed air with a duration of max. 5 seconds The maximum heat temperature can be adjusted at 250 °C. [Pg.402]

The condition of the magnetic particle suspension is controlled by an automated ASTM-bulb. The bulb is connected to the currently used Magentic particle suspension tank by a bypass, so the suspension in use is flowing through the bulb too. In user defined periods a valve is closed and the Magentic particle suspension remained into the bulb is analysed. The automatic bulb has the ability to measure the extinction and transmission of the suspension related to the time (Figure 1, Figure 2)... [Pg.629]

While adjusting the machine for its job the limits of the current for magnetizing the part have to be fixed as well as the magnetization time. During operation the machine will control for each part that the current-flow through the part and the time will be appropriate for a good magnetization. This is controlled by a hall sensor installed into the switch cabinet. [Pg.630]

The method is based on the international standard ISO 4053/IV. A small amount of the radioactive tracer is injected instantaneously into the flare gas flow through e.g. a valve, representing the only physical interference with the process. Radiation detectors are mounted outside the pipe and the variation of tracer concentration with time is recorded as the tracer moves with the gas stream and passes by the detectors. A control, supply and data registration unit including PC is used for on site data treatment... [Pg.1054]

The measurement of the streaming potential developed when a solution flows through two parallel plates [74-76] allows the characterization of macroscopic surfaces such as mica. [Pg.188]

A simple law, known as Darcy s law (1936), states that the volume flow rate per unit area is proportional to the pressure gradient if applied to the case of viscous flow through a porous medium treated as a bundle of capillaries,... [Pg.580]

Make a numerical estimate, with an explanation of the assumptions involved, of the specific surface area that would be found by (a) a rate of dissolving study, (b) Harkins and Jura, who find that at the adsorption of water vapor is 6.5 cm STP/g (and then proceed with a heat of immersion measurement), and (c) a measurement of the permeability to liquid flow through a compacted plug of the powder. [Pg.593]

Wlien an electrical coimection is made between two metal surfaces, a contact potential difference arises from the transfer of electrons from the metal of lower work function to the second metal until their Femii levels line up. The difference in contact potential between the two metals is just equal to the difference in their respective work fiinctions. In the absence of an applied emf, there is electric field between two parallel metal plates arranged as a capacitor. If a potential is applied, the field can be eliminated and at this point tire potential equals the contact potential difference of tlie two metal plates. If one plate of known work fiinction is used as a reference electrode, the work function of the second plate can be detennined by measuring tliis applied potential between the plates [ ]. One can detemiine the zero-electric-field condition between the two parallel plates by measuring directly the tendency for charge to flow through the external circuit. This is called the static capacitor method [59]. [Pg.1894]

These are databases that provide links to other databases or data sources. In this case, records describe objects that are other databases. The "Gale Directory of Databases" [14] is one of them. The connection between the databases flows through the meta-data of each database. [Pg.240]

When a pure gas flows through a channel the accompanying fall in pressure is accounted for partly by acceleration of the flowing stream and partly by momentum transfer to the stationary walls. Since a porous medium may be regarded as an assembly of channels, similar considerations apply to flow through porous media, but in the diffusional situations of principal interest here accelerational pressure loss can usually be neglected. If more than one molecular species is present, we are also interested in the relative motions of the different species, so momentum transfers by collisions between different types of molecules are also important. [Pg.6]

To appreciate the questions raised by Knudsen s results, consider first the relation between molar flow and pressure gradient for a pure gas flowing through a porous plug, rather than a capillary. The form predicted by the dusty gas model can be obtained by setting = 1, grad = 0 in equation... [Pg.54]

Though by no means a complete theory, this is at least a reasonable explanation of the Knudsen minimum, and it then remains to explain why the minimum is not observed for flow through porous media. Pollard and Present attributed this to the limited length/diameter ratio of the channels in a typical porous medium and gave a plausible argument in favor of this view. [Pg.55]

At very low densities It Is quite easy Co give a theoretical description of thermal transpiration, alnce the classical theory of Knudsen screaming 9] can be extended to account for Che Influence of temperature gradients. For Isothermal flow through a straight capillary of circular cross-section, a well known calculation [9] gives the molar flux per unit cross-sectional area, N, In the form... [Pg.178]


See other pages where Flow through is mentioned: [Pg.87]    [Pg.199]    [Pg.350]    [Pg.359]    [Pg.32]    [Pg.344]    [Pg.40]    [Pg.48]    [Pg.112]    [Pg.204]    [Pg.502]    [Pg.1111]    [Pg.26]    [Pg.399]    [Pg.25]    [Pg.54]    [Pg.90]    [Pg.90]    [Pg.186]    [Pg.444]    [Pg.471]    [Pg.495]   
See also in sourсe #XX -- [ Pg.34 , Pg.51 , Pg.379 ]

See also in sourсe #XX -- [ Pg.2 , Pg.3 , Pg.32 , Pg.38 , Pg.42 , Pg.43 , Pg.61 , Pg.62 ]




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Accelerating tube flow through

Air flow through ducts

Amperometric detection with flow through electrodes

Amperometric flow-through biosensors

Atmospheric pressure chemical ionization flow rate through

Batch Operation or Flow-through Cells

Blood flow through a vessel

Blood vessels flow through

Bypassing around heat transfer devices up and down (continuous flow through

Calculating the flow pumped through a pipe

Cantilever flow-through system

Capillaries blood flow velocity through

Capillary columns flow rate through

Capillary liquid flow through

Cells, spectroscopic flow-through

Centrifugal pumps minimum flow through

Chamber dynamic flow through

Circulatory system flow through

Columns flow rate through

Compressible flow through nozzles and constrictions

Conductivity flow-through

Constitution flow rate through

Continuous flow-through electrophoresis

Coolers flow through turbine

Curved tube, flow through

Darcy fluid flow through porous media

Darcys law through an analogy with the flow inside a network of capillary tubes

Design flow-through catalytic membrane

Detector flow-through

Directed Assembly of Particles through Convective Flows and Capillary Forces

Dissolution apparatus Flow-through cell

Dissolution testing flow-through systems

Distribution coefficient flow-through method

Dowex flow rate through

Dynamic flow-through system

Electrochemical flow-through immunosensors

Electrode gold flow-through

Electrolytic flow-through cell

Electroosmotic flow through packed columns

Electrostatic precipitators flow through

Emulsion Flow Through an Electric Filter

Entropy production in a flow through an annular packed bed

Enzyme immunosensor, thin-layer flow-through

Equation. d Arcy s. fluid flow through column

Estimation of heat flow through a composite wall with constant thermal conductivities

Example 2-10 Gas Flow Through Sharp-edged Orifice

Example 7-2 Flow through Sharp Edged Vent Orifice

Example Flow Through an Orifice

Example Oblique Transmission through Parallel Plate Flow

Fibre optic-based flow-through optical biosensors

Fibre optic-based flow-through sensors

Filter flow through

Flow Through a Packed Bed

Flow Through a Slit

Flow Through an Annular Die

Flow Through an Assembly of Pipes and Its Permeability

Flow Through the Capillary Fringe

Flow of Gases through Pipes in a Vacuum

Flow of Gases through Porous Plates

Flow of Nascent Hydrogen through Metals

Flow of Water through Schedule 40 Steel Pipe

Flow of fluids through granular beds and packed columns

Flow of polymer melts through narrow tubes and capillaries

Flow through Frictionless Nozzle

Flow through Soils and Rocks

Flow through Variable-Area Conduits

Flow through a Pipe

Flow through a converging nozzle

Flow through a packing

Flow through an annulus

Flow through an open channel

Flow through curved conduit

Flow through curved pipes

Flow through electrode, carbons

Flow through ideal nozzles

Flow through open channel

Flow through packed beds

Flow through regeneration unit

Flow through the accelerating tubes

Flow through the sampling orifice

Flow-Through Microcalorimeters

Flow-Through NMR Probes

Flow-Through PCR

Flow-through Design

Flow-through Tube Banks

Flow-through anodic stripping

Flow-through applications

Flow-through approach, advantages

Flow-through bioassays

Flow-through biochips

Flow-through biosensor

Flow-through calorimetric biosensors

Flow-through catalytic membrane reactors

Flow-through catalytic membrane reactors FTCMRs)

Flow-through catalytic membrane reactors design

Flow-through catalytic membrane reactors operation

Flow-through cell detection

Flow-through cell detection description

Flow-through cells

Flow-through channel

Flow-through chemical sensors

Flow-through chemical sensors reaction-rate

Flow-through chip

Flow-through column measurement

Flow-through column measurement procedure

Flow-through conductivity cell

Flow-through configuration

Flow-through conventional potentiometric cells

Flow-through cyclone

Flow-through diffusion cells, cross-section

Flow-through electrochemical biosensors

Flow-through electrochemical cell

Flow-through electrodes

Flow-through experiment

Flow-through fractionation procedures

Flow-through immunoassay

Flow-through immunosensors

Flow-through ion-selective potentiometric sensors

Flow-through macroscopic experiments

Flow-through method

Flow-through methods with online detection

Flow-through micro reactors

Flow-through microdialysis

Flow-through mode

Flow-through optical biosensors

Flow-through packed columns

Flow-through packed columns equation

Flow-through piezoelectric sensors

Flow-through porosimetry

Flow-through porous electrode

Flow-through potentiometric cells

Flow-through radioactivity detectors

Flow-through reactor system

Flow-through samplers

Flow-through sensor

Flow-through sensors active microzone

Flow-through sensors cells

Flow-through sensors classifications

Flow-through sensors continuous configurations

Flow-through sensors definition

Flow-through sensors features

Flow-through sensors for multideterminations based on integrated retention and detection

Flow-through sensors integrated detection-reaction

Flow-through sensors integrated detection-separation

Flow-through sensors measurement modes

Flow-through sensors transient signals

Flow-through spectrophotometer

Flow-through spring reliefs

Flow-through synthesis

Flow-through system

Flow-through systems, definition

Flow-through tactics

Flow-through test methodology

Flow-through tests

Flow-through thin layer technique

Flow-through voltammetry

Flow-through, description

Flow-through-screen pressure drop

Flow-through-screen tests

Fluid Flow Through a Packed Bed of Particles

Fluid flow pressure loss through tubes

Fluid flow through packed beds

Fluid flow through porous media

Fluid flow through solid beds

Fluidization fluid flow through solid beds

Forced Flow of Fluids through Tubes (Conduits)

Forced flow through catalyst

Forced flow-through type capillary

Forced flow-through type capillary viscometer

Friction in Flow through Beds of Solids

Frictionally resisted, incompressible flow through a real pipe

Fuel Flow-Through

Fuel Flow-Through System

Fuel cell flow-through

Gas Flow through Metals

Gas flow through an installed valve - Average Specific Volume Approximation Method (ASVAM)

Gas flow through the installed control valve

Gravitational flow through system

Heart blood flow through

Heat transfer between fluid flowing through fixed

INDEX flow-through configurations

Imaging flow-through chip

Instabilities During Flow Through Spinneret

Integrated flow-through optical biosensors

Integrated flow-through sensors

Isothermal reactors flow through packed beds

Knudsen (Intermediate) Flow Through a Tube

Laminar flow through packed beds

Laminar flow-through design

Light transmission through flow cell

Liquid flow through an installed valve

Liquid flow through polyhedral foams

Liquid flow through the valve

Liquids pipes, flow through

Mass flow rate through packed

Maxwell-Stefan equations, flow-through

Mean potential flows through groups of fixed bodies

Measurement by flow through a constriction

Measurement of current flowing through

Melt spinning flow through packs

Membrane flow-through multistage

Membrane flow-through sensors

Methods flow-through micro reactors

Methods flow-through reactor

Micromachined flow-through device

Minimum flow through pumps

Model Parameters and Flow-Through-Screen Experiment

Models flow-through

Molecular flow through components

Monolithic columns flow rate through

Newtonian Flow through a Capillary

Optical flow-through immunosensors

Optical flow-through sensors based on a non-regenerable immobilized reagent

Optimization of Pumping Rates in the Through-Flow System

Orifices, flow through

Overpumping Policy The Through-Flow Systems

Packings fluid flow through

Piezoelectric flow-through immunosensors

Piezoelectric flow-through sensors based on a non-regenerable immobilized reagent

Pipes gases, flow through

Poiseuille constant, flow-through

Polarographic through-flow analyzer

Pores forced flow through

Porosity fluid flow through porous media

Porous media flow through

Potentiometric flow-through biosensors

Prediction of pressure gradient for flow through packed beds

Pressure drop flow through packed beds

Pressure fluid flow through porous media

Probe flow-through probes

Process Intensification Achieved Through the Use of Flow Reactors

Process optical flow-through cell

Reactor flow-through

Recirculation through a Plug-Flow Batch Reactor

Regulation of blood flow through tissues

Reservoir through-flow

Reverse flow through pumps

Sedimentation tanks, flow-through

Semi-Fluidization through Oscillatory Flow

Solution sequence for compressible flow through a pipe

Steady-state flow through a nozzle with constant specific volume

Synthesis of Low Molecular Weight Compounds through Fast Reactions in Turbulent Flows

Thin-layer flow-through enzyme

Through-Flow Filtration Applications

Through-Flow Systems Unconfined and Confined

Through-flow filtration

Transport mechanisms, flow-through

Turbulent flow through packed beds

Two-Dimensional Flow Through Porous Media

Two-Phase Flow Through Porous Media

Upward Flow of Fluid Through Solid Particles (-AP) Regimes

Validation of Flow-Through Microcalorimeters

Vapor flow through trays

Water Flow through the Unsaturated Zone

Water flow through aquaporin channels

Woven fabrics, flow through

Zones through-flow

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