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Sequence of melting

Amplify DNA for 25 cycles with the appropriate sequence of melting (95°C for 1 min), annealing temperature (to be calculated from the melting temperatures of the primers used), and replication (72°C for 1 min), followed by a final 10 min extension step at 72°C. [Pg.3]

The first thermodynamic expression above states that the intermolecular attraction forces we must overcome to sublime the molecules of a substance are equal to the sum of the forces required to first melt it and then vaporize it. Likewise, the increased randomness obtained as molecules sublime is the same as the sum of entropies associated with the sequence of melting and vaporizing. Consequently, if we can predict such thermodynamic terms for vaporization or melting, we already know the corresponding parameters for sublimation. [Pg.107]

Metallocene isotactic polypropylenes (MET.PP) are accessible with different melting points under the commercial range of melt flow rate (Fig. 11). The variation of melting points in these polymers is linked with the presence of different lengths of isotactic sequences. Mechanical properties of polypropylene... [Pg.161]

Interaction between niobium oxide and fluorides, chlorides or carbonates of alkali metals in an ammonium hydrofluoride melt, yielded monooxyfluoroniobates with different compositions, MxNbOF3+x, where they were subsequently investigated [123-127]. According to DTA patterns of the Nb205 - 6NFL HF2 - 2MF system, (Fig. 18) a rich variety of endothermic effects result from the formation of ammonium monooxyfluoroniobate, its thermal decomposition and its interaction with alkali metal fluorides. The number of effects decreases and separation of ammonium ceases at lower temperatures and when going from lithium to cesium in the sequence of alkali metal fluorides. [Pg.49]

Although there are experimental and interpretative limitations [189, 526] in the kinetic analysis of non-isothermal data, DTA or DSC observations are particularly useful in determining the temperature range of occurrence of one or perhaps a sequence of reactions and also of phase changes including melting. This experimental approach provides, in addition, a useful route to measurements of a in the study of reactions where there is no gas evolution or mass loss. The reliability of conclusions based on non-isothermal data can be increased by quantitatively determining the... [Pg.98]

This sequence of reactions is a useful route to the pure element, but more complex boranes form when the heating is less severe. When diborane is heated to 100°C, for instance, it forms decaborane, B]0H14, a solid that melts at 100°C. Decaborane is stable in air, is oxidized by water only slowly, and is an example of the general rule that heavier boranes are less flammable than boranes of low molar mass. [Pg.723]

Figure 37-2. RNA polymerase (RNAP) catalyzes the polymerization of ribonucleotides into an RNA sequence that is complementary to the template strand of the gene. The RNA transcript has the same polarity (5 to 3 ) as the coding strand but contains L) rather than T. E coli RNAP consists of a core complex of two a subunits and two p subunits (P and p ). The holoen-zyme contains the 0 subunit bound to the ajPP core assembly. The co subunit is not shown. The transcription "bubble" is an approximately 20-bp area of melted DNA, and the entire complex covers 30-75 bp, depending on the conformation of RNAP. Figure 37-2. RNA polymerase (RNAP) catalyzes the polymerization of ribonucleotides into an RNA sequence that is complementary to the template strand of the gene. The RNA transcript has the same polarity (5 to 3 ) as the coding strand but contains L) rather than T. E coli RNAP consists of a core complex of two a subunits and two p subunits (P and p ). The holoen-zyme contains the 0 subunit bound to the ajPP core assembly. The co subunit is not shown. The transcription "bubble" is an approximately 20-bp area of melted DNA, and the entire complex covers 30-75 bp, depending on the conformation of RNAP.
It is now thought that the holes present in the melts are decisive for the conduction in melts. When an electric field is applied, the ion nearest a hole (in the direction of migration) will jump into the hole and leave a hole in its own former place, and thus the next ion can jump into this hole, and so on. Ionic migration thus is not a smooth motion in a viscous medium but, rather, a sequence of ion-hole transitions. [Pg.132]


See other pages where Sequence of melting is mentioned: [Pg.372]    [Pg.872]    [Pg.238]    [Pg.1835]    [Pg.89]    [Pg.283]    [Pg.345]    [Pg.521]    [Pg.411]    [Pg.336]    [Pg.105]    [Pg.195]    [Pg.372]    [Pg.872]    [Pg.238]    [Pg.1835]    [Pg.89]    [Pg.283]    [Pg.345]    [Pg.521]    [Pg.411]    [Pg.336]    [Pg.105]    [Pg.195]    [Pg.2538]    [Pg.157]    [Pg.154]    [Pg.237]    [Pg.419]    [Pg.236]    [Pg.738]    [Pg.318]    [Pg.383]    [Pg.56]    [Pg.280]    [Pg.194]    [Pg.579]    [Pg.236]    [Pg.349]    [Pg.415]    [Pg.415]    [Pg.367]    [Pg.441]    [Pg.442]    [Pg.167]    [Pg.184]    [Pg.144]    [Pg.99]    [Pg.4]    [Pg.399]    [Pg.345]    [Pg.841]    [Pg.444]    [Pg.571]   
See also in sourсe #XX -- [ Pg.105 ]




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