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Continuous split fractionation

A number of different driving forces have been used to implement CSF including gravitational sedimentation [113] diffusive transport [114,115] electrically driven transport [116] and hydrodynamic lift forces [117]. [Pg.286]


A System Based on Split-Flow Lateral-Transport Thin (SPLITT) Separation Cells for Rapid and Continuous Particle Fractionation, J. C. Giddings, Sep. Sci. Technol., 20, 749 (1985). [Pg.304]

The column is swept continuously by a carrier gas such as helium, hydrogen, nitrogen or argon. The sample is injected into the head of the column where it is vaporized and picked up by the carrier gas. In packed columns, the injected volume is on the order of a microliter, whereas in a capillary column a flow divider (split) is installed at the head of the column and only a tiny fraction of the volume injected, about one per cent, is carried into the column. The different components migrate through the length of the column by a continuous succession of equilibria between the stationary and mobile phases. The components are held up by their attraction for the stationary phase and their vaporization temperatures. [Pg.20]

Plutonium-239 is a fissile element, and vvill split into fragments when struck by a neutron in the nuclear reactor. This makes Pu-239 similar to U-235, able to produce heat and sustain a controlled nuclear reaction inside the nuclear reactor. Nuclear power plants derive over one-third of their power output from the fission of Pu-239. Most of the uranium inside nuclear fuel is U-238. Only a small fraction is the fissile U-235. Over the life cycle of the nuclear fuel, the U-238 changes into Pu-239, which continues to provide nuclear energy to generate electricity. [Pg.869]

Many interfaces have been developed to meet these demanding challenges. Some of these coupling methods, such as the moving belt or the particle beam interface, are based on the concomitant elimination of the solvent before it enters the mass spectrometer. Other methods such as direct liquid introduction (DLI) or continuous flow FAB rely on splitting the flow of the liquid that is introduced into the interface in order to obtain a flow that can be directly infused into the ionization source. However, these types of interfaces can only handle a fraction of the liquid flow from the LC. [Pg.506]

An early trial sponsored by the National Cancer Institute of Canada failed to establish a significant difference in locoregional control and overall survival when evaluating 212 patients with larnygeal or hypopharyngeal squamous cell carcinoma (SCCA) treated with 50 Gy in 20 fractions over 28 d or split-course radiotherapy of 25 Gy in 10 fractions over 14 d, followed by a 28-d rest and then 25 Gy in 10 fractions over 14 d beginning on d 43 with mitomycin C (10 mg/m2 on d 1 and 43) in combination with continuous infusion 5-FU (1000 mg/m2/d on d 1-4 and 43-46) (48). Nevertheless, this study suggested that the addition of chemotherapy may overcome the decreased activity of split-course radiotherapy. [Pg.154]

Figure 24-16 shows effects of operating parameters in split and splitless injections. Experiment A is a standard split injection with brisk flow through the split vent in Figure 24-15. The column was kept at 75"C. The injection liner was purged rapidly by carrier gas, and peaks are quite sharp. Experiment B shows the same sample injected in the same way, except the split vent was closed. Then the injection liner was purged slowly, and sample was applied to the column over a long time. Peaks are broad, and they tail badly because fresh carrier gas continuously mixes with vapor in the injector, making it more and more dilute but never completely flushing the sample from the injector. Peak areas in B are much greater than those in A because the entire sample reaches the column in B, whereas only a small fraction of sample reaches the column in A. Figure 24-16 shows effects of operating parameters in split and splitless injections. Experiment A is a standard split injection with brisk flow through the split vent in Figure 24-15. The column was kept at 75"C. The injection liner was purged rapidly by carrier gas, and peaks are quite sharp. Experiment B shows the same sample injected in the same way, except the split vent was closed. Then the injection liner was purged slowly, and sample was applied to the column over a long time. Peaks are broad, and they tail badly because fresh carrier gas continuously mixes with vapor in the injector, making it more and more dilute but never completely flushing the sample from the injector. Peak areas in B are much greater than those in A because the entire sample reaches the column in B, whereas only a small fraction of sample reaches the column in A.
This argument is nothing but the additive renormalization discussed in Sect 7.2 in the context of the continuous chain limit, now interpreted on the level of the interaction. From the field theoretic formulation we easily see that it holds to all orders. We thus may split the two-body interaction into a one-body part which effectively takes care of interactions within small fractions of the chains, and a remainder conforming to the estimate (10.1). [Pg.159]

Non-Stop-Flow Mode In the non-stop-flow mode, the LC-ARC system is operated in a similar manner to the conventional continuous-flow analysis. If a mass spectrometer is coupled to the LC-ARC system, the LC effluent is split postcolumn to deliver a fraction to the radiochemical detector and the balance to a mass spectrometer. [Pg.257]

Equation 10.80 assumes spontaneous termination for termination by hydrogeno-lysis, JctTm should be replaced by k timpH2. [The right-hand side of eqn 10.80 also expresses the probability that an adduct will continue to add monomer rather than split off catalyst and produce a dead polymer molecule.] Since all adducts Pj produce polymer Pj with the same rate coefficient klrm, the ratio in eqn 10.80 is also that of the concentrations or mole fractions of the respective polymer molecules Pj+1 and Pj that are formed ... [Pg.337]

We begin the analysis of phase equilibria (for those cases where phase splitting does in fact occur) with the simplest possible case, that of vapor-liquid equilibrium where both the liquid and the vapor phase are ideal, so that Raoult s law applies (Astarita, 1989 Bowman, 1949 Edminster, 1955). In this case the only parameter that completely characterizes every individual component is its vapor pressure b at the temperature considered hence, one begins by using b itself as the (dimensional) component label. Let X (b) and X (fc) be the mole fraction distributions in the liquid and vapor phases, respectively, and let p be the total pressure. Obviously, the zeroth moments of both distributions are unity. The continuous form of Raoult s law is ... [Pg.17]

Uses of Oieochemicais Based on Palm Oil and Palm Kernel Oil. (a) Fatty Acids. The most common method for the production of fatty acids adopted by the oieochemicais industry is high-temperature and high-pressure fat splitting. The fatty acid mixture produced is separated into broad cuts or pure fatty acids by simple or fractional distillations. Tables 50 and 51 list examples of fatty acids derived from palm products. The exact specifications of the various fatty acids produced vary slightly depending on the exact raw materials and process used. The specifications could also change due to continuous upgrading of processes. [Pg.1040]


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Continued fractions

Continuous fractionation

Fractionation split

Split fraction

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