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Flip rule

Flip Rule Cross relations can be found in two ways. First, by using energy balances for appropriate cyclic processes and second as a direct result of a mathematical operation we call flipping. Naturally, the flip rule can be derived mathematically (see end of the Chapter), but we will give instructions here in the form of a kind of recipe Take the differential quotient in question (or difference quotient) you wish to transform and... [Pg.257]

Coupling Starting from the main equation (9.4), dW = —pdV + Jd5 — Jid<, we can use the flip rule to convert the temperature coefficient cc of the drive of a reaction or any other type of transformation of substances ... [Pg.260]

An example of coupling in the same direction ( i "T 2) would be a small amount of undissolved PbCl2 in a beaker with water that dissolves when KNO3 is added ( salting-in effect ). The first substance s rise in potential can be used to measure the strength of reciprocal action caused by the second substance. This is the so-called displacement coefficient (9/opposite effect, the displacement of the second substance by the first, which we describe by dpi/dn2)j p is just as great, as we can see by applying the flip rule ... [Pg.263]

We conclude that we can directly obtain all kinds of cross relations by flipping. The flip rule can be considered a memory aid for all such relations. Using it in this way is advantageous ... [Pg.264]

For the mathematically inteiested In order to derive Eq. (12.2), we will refer back to the cross relation discussed in Sect. 9.3 known as n n coupling. When one substance tries to displace (or favor) another one, this happens reciprocally and with equal strength. The corresponding displacement coefficients are equal as can easily be shown by applying the flip rule (main equation dW = —pdV + TdS + ji drif + p dn ) ... [Pg.319]

This same pattern can be used for finding numerous other relations. However, we do not need this method because the flip rule leads directly to the same result without taking the detour over a second derivative of an appropriately chosen thermodynamic function. The relation in the first line, for example, is already well known from Sect. 9.2 [Eq. (9.7)]. [Pg.594]

Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold. Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold.
These results indicate that is it possible to change the fold of a protein by changing a restricted set of residues. They also confirm the validity of the rules for stability of helical folds that have been obtained by analysis of experimentally determined protein structures. One obvious impliction of this work is that it might be possible, by just changing a few residues in Janus, to design a mutant that flip-flops between a helical and p sheet structures. Such a polypeptide would be a very interesting model system for prions and other amyloid proteins. [Pg.370]

What about a microcanonical ensemble based approach The simplest prescription would be to define a rule that flips the spins only at a constant energy that is, for 6H = 0 or Ai = 2. The reader may recall that we have already studied some of the behaviors of this rule in section 3.4 it is, in fact, equal to the Pbedkin-reversible rulq Q2R ([vich84], [vich86aj). Prom the comments made in our earlier discussion, it... [Pg.359]

Another problem with microcononical-based CA simulations, and one which was not entirely circumvented by Hermann, is the lack of ergodicity. Since microcanoriical ensemble averages require summations over a constant energy surface in phase space, correct results are assured only if the trajectory of the evolution is ergodic i.e. only if it covers the whole energy surface. Unfortunately, for low temperatures (T << Tc), microcanonical-based rules such as Q2R tend to induce states in which only the only spins that can flip their values are those that are located within small... [Pg.360]

Within its orbit, which has some of the characteristics of a molecular orbital because it is shared with electrons on the surrounding atoms, the electron has two possible spin multiplicity states. These have different energies, and because of the spin-multiplicity rule, when an (N-V) center emits a photon, the transition is allowed from one of these and forbidden from the other. Moreover, the electron can be flipped from one state to another by using low-energy radio-frequency irradiation. Irradiation with an appropriate laser wavelength will excite the electron and as it returns to the ground state will emit fluorescent radiation. The intensity of the emitted photon beam will depend upon the spin state, which can be changed at will by radio-frequency input. These color centers are under active exploration for use as components for the realization of quantum computers. [Pg.438]

Binding of the tRNA anticodon to the mRNA codon follows the rules of complementary and antiparallel binding, that is, the mRNA codon is "read" 5 ->3 by an anticodon pairing in the "flipped" (3 —>5 ) orientation (Figure 31.9). [Note When writing the sequences of bolh codons and anticodons, the nucleotide sequence must ALWAYS be listed in the 5 —>3 order.]... [Pg.434]

In the first example (top row) the polyhex-like object has a vertex of degree four, which is forbidden. Also the corresponding dualist-like formation is forbidden. In the bottom row the degrees of the vertices are not violated, but yet the systems are obviously not polyhexes. It is not allowed, for instance, to flip naphthalene around the middle edge. In none of the examples above the rules of addition (Fig. 1) have been followed strictly. [Pg.71]

Hip-flop inference rule is simple If a variable is assigned a value under the control of a clock edge, a flip-flop is generated an exception to this rule is when a variable is assigned and used only locally within an always statement as an intermediate variable. [Pg.70]

It is important to understand the flip-flop inference rules of a synthesis tool. These rules may vary from one synthesis tool to another. If the inference rules are not followed, a synthesized netlist may have many more flip-flops than are really necessary. Here is a case in point. [Pg.166]

Only two selection rules can be explained. Absence of transition m = i -> m = — for an energetically isolated term 2P1/2 is due to lack of splitting and failure to build up the 2II1/2 molecular term. Absence of transition m = f - m = — for 2P3/2 under quasidegenerate conditions is due to the impossibility of a Am = 3 transition without spin flip. [Pg.355]

If asked how many transitions are possible among the four spin states, you might be tempted to list all of the following l- 2, l- 3, l- 4, 2->3, 2->4, and 3->4. But there is a selection rule that controls the probability (and hence intensity) of each transition An allowed transition involves only the flip of one nuclear spin all transitions involving more than one flip are forbidden. From the list of transitions we can therefore delete 1—>4 and 2—>3, because these involve the simultaneous flip of both spins. Transitions l- 2 and 3- 4 result from the flip of only the Hb spin and are thus allowed and responsible for the Hb signal. Likewise, transitions 1—>3 and 2—>4 result from the flip of only the Ha spin and give rise to the Ha signal. Further, notice (from symmetry) that transi-... [Pg.132]

In contrast to plastics, rubbers are rarely used in the packaging of food products. Exceptions to this rule are the use of rubber in flip top seals on beer bottles and the seal that is present in food cans. However, in the processing of food, there are a number of situations where significant contact with rubber products can occur. This is due to the fact that the unique properties of rubber lead to it being used in a wide range of products (see Table 12.1). It is also the case that the range of contact conditions encountered (i.e. food type, contact temperature, time and area) mean that a wide variety of rubber compounds are employed (see section 12.2). [Pg.271]


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See also in sourсe #XX -- [ Pg.257 ]




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