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Directed back-crossing

Most European countries follow the European Directives that list the colorants and specifications for use in foods and drugs in the European Union (EU). The directive that has previously controlled the approved colorants for use in pharmaceuticals in Europe is 78/25/EEC, which refers to a list of colorants from a 1962 directive. " The EC published European Directive 94/36/EC in 1994, which significantly changed the list of approved colorants for use in foods. For example, Allura red AC (FD C red 40) and Brilliant blue FCF (FD C blue 1) were now approved for use in foods, however, these materials did not exist on the list of approved drug colorants because of the cross-referencing of the pharmaceutical directives back to the 1962 list. This has created much confusion throughout industry and the regulatory community. [Pg.660]

Figure 17.5 Suppose a certain number of people are confined to the two buildings connected by this walkway and that people can walk back and forth between the buildings. The number of people in each building will remain constant only if the same number of people cross the bridge in one direction as cross in the opposite direction. [Pg.598]

Quarrie [18] emphasized that in contrast to the lesions in fic and sit other mutations may affect ABA synthesis only indirectly. As mentioned above, the vp mutants in maize are devoid of carotenoids and consequently ABA deficient. Mutations may also occur simultaneously in two different genes, one directly affecting ABA biosynthesis and the other having an unrelated effect. In the case of close linkage, separation of such mutations by back crossing is not always successful. [Pg.25]

If the axial length is closed, the pathway down the screw is divided into a number of isolated areas with no opportunity for flow in the axial direction. Open cross flow allows a material path around the screw, the polymer flows in the radial direction, as it is transfers back and forth between screws. If the cross direction is closed, material cannot flow... [Pg.239]

While evidence for hydration forces date back to early work on clays [1], the understanding of these solvent-induced forces was revolutionized by Horn and Israelachvili using the modem surface force apparatus. Here, for the first time, one had a direct measurement of the oscillatory forces between crossed mica cylinders immersed in a solvent, octamethylcyclotetrasiloxane (OMCTS) [67]. [Pg.243]

Flow behaviour of polymer melts is still difficult to predict in detail. Here, we only mention two aspects. The viscosity of a polymer melt decreases with increasing shear rate. This phenomenon is called shear thinning [48]. Another particularity of the flow of non-Newtonian liquids is the appearance of stress nonnal to the shear direction [48]. This type of stress is responsible for the expansion of a polymer melt at the exit of a tube that it was forced tlirough. Shear thinning and nonnal stress are both due to the change of the chain confonnation under large shear. On the one hand, the compressed coil cross section leads to a smaller viscosity. On the other hand, when the stress is released, as for example at the exit of a tube, the coils fold back to their isotropic confonnation and, thus, give rise to the lateral expansion of the melt. [Pg.2534]

Other types of pressure-relief valves do not depend upon the back pressure for their performances. However, to ensure that the safety valves work at their maximum capacity, back pressure is limited to 50 percent of the relief valve set pressure. In the balanced bellows type valve, the spring does not act directly on the disk. Instead, it serves on a bellows first, which in turn acts on the disk. In case of the piston type, it works on the same principle as the bellows type, except that the bellows is replaced by a piston (see Figure 17B). The cross-sectional area of both the piston and the bellows is the same as the inlet nozzle of the valve and the effect of the back pressure on the top and the bottom of the disk creates equal balancing forces. That is, P,A is always equal to F, as shown in Figure 17B. [Pg.319]

The acetyl-CoA derived from amino acid degradation is normally insufficient for fatty acid biosynthesis, and the acetyl-CoA produced by pyruvate dehydrogenase and by fatty acid oxidation cannot cross the mitochondrial membrane to participate directly in fatty acid synthesis. Instead, acetyl-CoA is linked with oxaloacetate to form citrate, which is transported from the mitochondrial matrix to the cytosol (Figure 25.1). Here it can be converted back into acetyl-CoA and oxaloacetate by ATP-citrate lyase. In this manner, mitochondrial acetyl-CoA becomes the substrate for cytosolic fatty acid synthesis. (Oxaloacetate returns to the mitochondria in the form of either pyruvate or malate, which is then reconverted to acetyl-CoA and oxaloacetate, respectively.)... [Pg.804]

More complex phenomena occur when current crosses interfaces between semiconductors. The most typical example is the rectification produced at interfaces between p- and n-type semiconductors. Electric current freely flows from the former into the latter semiconductor, but an electric field repelling the free carriers from the junction arises when the attempt is made to pass current in the opposite direction Holes are sent back into the p-phase, and electrons are sent back into the n-phase. As a result, the layers adjoining the interface are depleted of free charges, their conductivities drop drastically, and current flow ceases ( blocking the interface). [Pg.13]

Figure 10.1 J. J. Thomson s method for measuring e/m, the mass-to-charge ratio of an electron (Thomson 1897). Electrons (cathode rays) leave the cathode (C) and are accelerated towards the anode (A), passing through a small hole and a further hole in plate (D) to provide a collimated beam. It then passes through crossed electric (E) and magnetic fields (B) which deflect the beam in the same plane but in opposite directions, and strikes the fluorescent screen at the end. In (a) the strengths of E and B are adjusted to bring the spot back to zero deflection (S). In (b), with electric field only, the deflection from S (y ) is measured, and e/m calculated as in the text. Figure 10.1 J. J. Thomson s method for measuring e/m, the mass-to-charge ratio of an electron (Thomson 1897). Electrons (cathode rays) leave the cathode (C) and are accelerated towards the anode (A), passing through a small hole and a further hole in plate (D) to provide a collimated beam. It then passes through crossed electric (E) and magnetic fields (B) which deflect the beam in the same plane but in opposite directions, and strikes the fluorescent screen at the end. In (a) the strengths of E and B are adjusted to bring the spot back to zero deflection (S). In (b), with electric field only, the deflection from S (y ) is measured, and e/m calculated as in the text.

See other pages where Directed back-crossing is mentioned: [Pg.26]    [Pg.262]    [Pg.195]    [Pg.105]    [Pg.160]    [Pg.126]    [Pg.49]    [Pg.55]    [Pg.38]    [Pg.258]    [Pg.24]    [Pg.717]    [Pg.113]    [Pg.316]    [Pg.180]    [Pg.1015]    [Pg.1148]    [Pg.2526]    [Pg.2562]    [Pg.111]    [Pg.459]    [Pg.401]    [Pg.464]    [Pg.74]    [Pg.139]    [Pg.4]    [Pg.103]    [Pg.52]    [Pg.728]    [Pg.602]    [Pg.168]    [Pg.14]    [Pg.86]    [Pg.271]    [Pg.57]    [Pg.275]    [Pg.25]    [Pg.35]    [Pg.4]    [Pg.377]    [Pg.162]   
See also in sourсe #XX -- [ Pg.266 ]




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Direct crossing

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