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Normal interface level

Assume 20% cross-sectional area is occupied by an emulsion and is recognized as a dead volume. This is actually the height over which the interface level wdll vary during normal operations [26]. [Pg.241]

In the LPG contactor the amine is normally the continuous phase with the amine-hydrocarbon interface at the top of the contactor. This interface level controls the amine flow out of the contactor. (Some liquid/liquid contactors are operated with the hydrocarbon as the continuous phase. In this case, the interface is controlled at the bottom of the contactor.) The treated C3/C4 stream leaves the top of the contactor. A final coalescer is often installed to recover the carry-over amine. [Pg.36]

Fig- 2—Typical configuration of a three-phase horizontal separator. Interface level control maintains water level, weir maintains oil level. Vessels may be equipped with sand jets If sand production is a problem. jets are designed for 20 fps velocity, and produced water normally is used for backwashing. [Pg.98]

Horizontal treaters. Multiwell installations normally require horizontal treaters. Fig 2 shows a typical design. Flow enters the front section of the tteatei where gas is flushed. Liq uid falls to the vicinity of the oil-water interface where it is water washed and freewater separated Oil and emulsion rise past the lire tubes and are. skimmed into the oil surge i Irani -her. "Fhe oil-water interface in the inlet section is controlled by an interface level controller that operates a dump valve for the freewater... [Pg.144]

Figure 3 shows the eomparison of the normalized bed height from the H-Oil reactor data and ANN model predicted values after two millions training events. The maximum ARD% is 13.8% with an AAD% of 1.92% for the 85 sets of input data employed. However, if only data with bed height values below the allowable upper level are considered, the max. ARD% and AAD% reduce to 10.7% and 1.43% respectively. It is clearly demonstrated the predicted results from the ANN ebullated-bed expansion model are very close to the literature values. This model by no mean limits its applications just to predict the interface level. It can be extended to eover heat generation in terms of exotherms, spread temperature and/or catalyst average temperature (CAT) from data recorded in the technieal report [15]. [Pg.287]

There are a number of hybrid techniques which integrate different methodologies. These include (a) coupled level set-volume of fluid (CLSVOF) which combines mass-conserving properties with accurate normal and curvature calculation of level set (b) particle level set which uses particles to enhance mass conservation (c) mixed markers and volume of fluid with which one obtains a smooth motion of the interface, typical of the marker approach, with a good volume conservation, as in standard VOF methods and (d) hybrid immersed interface-level set which, instead of tracking the interface explicitly, captures the interface similar to level set method (purely Eulerian technique). There are a number of other hybrid techniques which have been less widely used. [Pg.2477]

Fig. 12 HOMO and LUMO levels for different locations in the CuPc/PTCBI interface system. The normal interface cell dashed) shows some changes in the HOMO energies near the interface, while the pulled interface cell (solid) has much larger HOMO and LUMO changes near the interface. Reprinted with permission from [138], Copyright 2013 American Chemical Society... Fig. 12 HOMO and LUMO levels for different locations in the CuPc/PTCBI interface system. The normal interface cell dashed) shows some changes in the HOMO energies near the interface, while the pulled interface cell (solid) has much larger HOMO and LUMO changes near the interface. Reprinted with permission from [138], Copyright 2013 American Chemical Society...
Amine entrainment in the LPG is minimized by providing adequate LPG residence time above the normal LPG/amine interface level. Tse and Santos (1993) cite a case where the LPG residence time, as measured from the interface to the top of the contactor, was 8 to 10 minutes. This is quite conservative. A more reasonable criterion is believed to be the greater of 8 feet or 5 minutes LPG residence time as measured from the LPG/amine interface to the LPG contactor top tangent line. This assumes that an external grasity settler or coalescer is provided for the LPG product stream as shown in Figure 2-96. [Pg.169]

A cyclone installed to separate liquid from a carrier gas is normally equipped with a liquid drain pipe that is submerged at its bottom end in a pool of liquid. This type of seal is very similar to that shown in Fig. ll.l.le. The drain pipe must be of sufficient height above the gas-liquid interface level to overcome the suction created by the cyclone. In systems where foaming is possible, such an underflow seal must also take into consideration the decrease in liquid density brought about by foaming. [Pg.239]

Elevation of low interface level shutdown (LILSD) is normally set at 150 mm from the bottom of the vessel however, it is always advisable to check the liquid residence time for LILSD. A too short liquid residence time will increase the chances of a gas breakthrough from the separator. Generally, 1 to 3 min residence time is adequate for the shutdown level. The same principle can be used to set the low liquid level shutdown (LLLSD). This setting also depends on tire type of separator being used. For the flooded weir separator, this level can be set either above or below the weir level, depending on the residence time requirement. [Pg.220]

For mixture.s the picture is different. Unless the mixture is to be examined by MS/MS methods, usually it will be necessary to separate it into its individual components. This separation is most often done by gas or liquid chromatography. In the latter, small quantities of emerging mixture components dissolved in elution solvent would be laborious to deal with if each component had to be first isolated by evaporation of solvent before its introduction into the mass spectrometer. In such circumstances, the direct introduction, removal of solvent, and ionization provided by electrospray is a boon and puts LC/MS on a level with GC/MS for mixture analysis. Further, GC is normally concerned with volatile, relatively low-molecular-weight compounds and is of little or no use for the many polar, water soluble, high-molecular-mass substances such as the peptides, proteins, carbohydrates, nucleotides, and similar substances found in biological systems. LC/MS with an electrospray interface is frequently used in biochemical research and medical analysis. [Pg.59]

VOF or level-set models are used for stratified flows where the phases are separated and one objective is to calculate the location of the interface. In these models, the momentum equations are solved for the separated phases and only at the interface are additional models used. Additional variables, such as the volume fraction of each phase, are used to identify the phases. The simplest model uses a weight average of the viscosity and density in the computational cells that are shared between the phases. Very fine resolution is, however, required for systems when surface tension is important, since an accurate estimation of the curvature of the interface is required to calculate the normal force arising from the surface tension. Usually, VOF models simulate the surface position accurately, but the space resolution is not sufficient to simulate mass transfer in liquids. [Pg.341]

The Vacuum Reference The first reference in the double-reference method enables the surface potential of the metal slab to be related to the vacuum scale. This relationship is determined by calculating the workfunction of the model metal/water/adsorbate interface, including a few layers of water molecules. The workfunction, — < ermi. is then used to calibrate the system Fermi level to an electrochemical reference electrode. It is convenient to choose the normal hydrogen electrode (NHE), as it has been experimentally and theoretically determined that the NHE potential is —4.8 V with respect to the free electron in a vacuum [Wagner, 1993]. We therefore apply the relationship... [Pg.101]


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