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Loops limitations

A switch-clamp-latch mechanism is critical for the quiescent state of c-ABL normally. The switch refers to a flip that occurs in an activation loop from the C-lobe that goes between opened and closed conformations and represent active and inactive states of the enz5mie, respectively (Fig. 2). This clamp or loop limits the access of ATP and other substrates to the active binding site of the ABLl protein. A latch stabilizes... [Pg.130]

Our next-higher value of hf = 0.004552 exhibits a double-loop limit cycle, or a period-two periodic attractor in the phase plot of Figure 4.55. [Pg.238]

Larger-amplitude single period with a one double-loop limit cycle... [Pg.239]

Fig. ni.C.1. The concentrations of Br versus Mn(III) as multiple peak oscillations with looped limit cycles. (After Maselko (1980-1))... [Pg.90]

If variable spin system parameters are used the increment step HS1...32, the start value HV1...32 and the loop limit L0...L31 must be assigned. The range over which a variable parameter is varied depends upon the increment step size and the loop limit. If required by the pulse program these parameters will appear the Go Check Experiment Parameters dialog box. As discussed in previous sections, loop definitions are not only restricted to spin system variable incrementation. [Pg.150]

Table 15.2. Structural families in the basic loop structures. CONFORMATION is the conformation of the loop (0, ((/ angles, see caption of Figure 15.5) NO. is number observed in proteins analyzed SEQUENCE is the sequence template a,, T are used to denote residues favoring a helix, P strand and type I P turn structures respectively i = polar, = hydrophobic - is any amino acid capital letters are one letter amino acid code (G Glycine D Aspartic Acid, N Asparagine, S Serine, T threonine, A Alanine, H Histidine, P Proline) / indicates alternative, blank indicates loop limits... Table 15.2. Structural families in the basic loop structures. CONFORMATION is the conformation of the loop (0, ((/ angles, see caption of Figure 15.5) NO. is number observed in proteins analyzed SEQUENCE is the sequence template a,, T are used to denote residues favoring a helix, P strand and type I P turn structures respectively i = polar, = hydrophobic - is any amino acid capital letters are one letter amino acid code (G Glycine D Aspartic Acid, N Asparagine, S Serine, T threonine, A Alanine, H Histidine, P Proline) / indicates alternative, blank indicates loop limits...
With the existing settings, the control loop limit-cycles at an amplitude of 1.8// and a period of 24.4tj. Reduction of the proportional band by half will change the amplitude only to 2// but will reduce the period to 2Ta-... [Pg.130]

In the region Z i, there are no limit cycles. On the curve L4, upon moving from D towards D2j a stable limit cycle is born from a simple separatrix loop. An imstable double-loop limit cycle bifurcates from a double separatrix loop with (To > 0 on L2. Thus, in the region D3, there are two limit cycles one stable and the other is unstable. The unstable double limit cycle merges with the stable limit cycle on the curve Li. After that only one single-circuit unstable limit cycle remains in region D4. It adheres into the homoclinic loop on the curve L3. [Pg.351]

Attractors can be simple time-independent states (points in F), limit cycles (simple closed loops in F) corresponding to oscillatory variations of tire chemical concentrations with a single amplitude, or chaotic states (complicated trajectories in F) corresponding to aperiodic variations of tire chemical concentrations. To illustrate... [Pg.3055]

In this section, the systematic search for conical intersections based on the Longuet-Higgins phase-change rule is described. For conciseness sake, we limit the present discussion to Hiickel-type systems only, unless specifically noted otherwise. The first step in the antilysis is the determination of the LH loops containing a conical intersection for the reaction of interest. [Pg.347]

A characteristic feature of a Type IV isotherm is its hysteresis loop. The exact shape of the loop varies from one adsorption system to another, but, as indicated in Fig. 3.1, the amount adsorbed is always greater at any given relative pressure along the desorption branch FJD than along the adsorption branch DEF. The loop is reproducible provided that the desorption run is started from a point beyond F which marks the upper limit of the loop. [Pg.111]

Fig. 3.28 The Kiselev method for calculation of specific surface from the Type IV isotherm of a compact of alumina powder prepared at 64 ton in". (a) Plot of log, (p7p) against n (showing the upper (n,) and lower (n,) limits of the hysteresis loop) for (i) the desorption branch, and (ii) the adsorption branch of the loop. Values of. 4(des) and /4(ads) are obtained from the area under curves (i) or (ii) respectively, between the limits II, and n,. (6) The relevant part of the isotherm. Fig. 3.28 The Kiselev method for calculation of specific surface from the Type IV isotherm of a compact of alumina powder prepared at 64 ton in". (a) Plot of log, (p7p) against n (showing the upper (n,) and lower (n,) limits of the hysteresis loop) for (i) the desorption branch, and (ii) the adsorption branch of the loop. Values of. 4(des) and /4(ads) are obtained from the area under curves (i) or (ii) respectively, between the limits II, and n,. (6) The relevant part of the isotherm.
Perhaps the most serious limitation, however, arises from the fact neither branch of the hysteresis loop corresponds to thermodynamic reversibility. The value of the integral J Va(p°jp)dn = /, say, differs considerably for the two branches of the loop. In fact... [Pg.173]

The limits of pore size corresponding to each process will, of course, depend both on the pore geometry and the size of the adsorbate molecule. For slit-shaped pores the primary process will be expected to be limited to widths below la, and the secondary to widths between 2a and 5ff. For more complicated shapes such as interstices between small spheres, the equivalent diameter will be somewhat higher, because of the more effective overlap of adsorption fields from neighbouring parts of the pore walls. The tertiary process—the reversible capillary condensation—will not be able to occur at all in slits if the walls are exactly parallel in other pores, this condensation will take place in the region between 5hysteresis loop and in a pore system containing a variety of pore shapes, reversible capillary condensation occurs in such pores as have a suitable shape alongside the irreversible condensation in the main body of pores. [Pg.244]

Methanol Synthesis. AH commercial methanol processes employ a synthesis loop, and Figure 6 shows a typical example as part of the overall process flow sheet. This configuration overcomes equiUbtium conversion limitations at typical catalyst operating conditions as shown in Figure 1. A recycle system that gives high overall conversions is feasible because product methanol and water can be removed from the loop by condensation. [Pg.278]

Solids. Increasing use of bulk cars, especially of covered hopper cars, has accompanied the expansion of the tank-car fleet. The principal drawback of bulk cars is the requirement for limited use, specialized cars, which necessitates a large investment. However, if such investment can be justified, the cost of transportation for dry bulk materials ia hopper cars usually is less than those for goods ia shipping containers. In many instances, such cars are used in closed-loop service that is, they shuttle in unit trains between filling and discharge points. Similar equipment is also used in specialized highway vehicles whose tmck bodies can incorporate dump hoppers and built-in conveyors. [Pg.512]

The simplest method of reduciag stresses and reactions is to provide additional pipe ia the system ia the form of loops or offset-bonds. When physical limitations restrict the use of additional bends, a multiple arrangement of several small-size pipe mns may sometimes be used. Owiag to stress intensification, the maximum stress generally occurs at elbows, bends, and Ts. Thus, heavier-walled fittings may reduce the stress without significantly impairing flexibiUty. FiaaHy, effectively located restraints can reduce thermal effects on the equipment. [Pg.64]


See other pages where Loops limitations is mentioned: [Pg.903]    [Pg.238]    [Pg.14]    [Pg.903]    [Pg.215]    [Pg.233]    [Pg.702]    [Pg.702]    [Pg.125]    [Pg.856]    [Pg.857]    [Pg.1238]    [Pg.862]    [Pg.200]    [Pg.34]    [Pg.260]    [Pg.903]    [Pg.238]    [Pg.14]    [Pg.903]    [Pg.215]    [Pg.233]    [Pg.702]    [Pg.702]    [Pg.125]    [Pg.856]    [Pg.857]    [Pg.1238]    [Pg.862]    [Pg.200]    [Pg.34]    [Pg.260]    [Pg.1677]    [Pg.2268]    [Pg.2277]    [Pg.122]    [Pg.479]    [Pg.205]    [Pg.51]    [Pg.100]    [Pg.113]    [Pg.260]    [Pg.589]    [Pg.243]    [Pg.337]    [Pg.190]    [Pg.211]    [Pg.371]    [Pg.138]   
See also in sourсe #XX -- [ Pg.200 ]




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