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Head dissociation

Biological [41] and synthetic [42] molecular walkers can often be described in terms of a three-state mechanism shown that involves a mechanical transition L — R along with two energy-driven processes, E L and E R, in which one of the heads dissociates/binds to the molecular track as shown in Fig. 12. This mechanism can also be written as a triangle reaction ... [Pg.311]

In the original presentation of the BFM2 model [23], special attention was paid to computing the degree of dissociation of the sulfonate heads as a function of water content, a( ). However, since i) almost all sulfonate heads dissociate as soon as the water content X exceeds 2 ii) the conductivity vanishes at small values for X and iii) conditioned membranes in fuel cells maintain water contents above X = 2, it is therefore reasonable and expedient to assume a = 1. The model is thus presented here with this simplification. [Pg.138]

Tandem quadrupole and magnetic-sector mass spectrometers as well as FT-ICR and ion trap instruments have been employed in MS/MS experiments involving precursor/product/neutral relationships. Fragmentation can be the result of a metastable decomposition or collision-induced dissociation (CID). The purpose of this type of instrumentation is to identify, qualitatively or quantitatively, specific compounds contained in complex mixtures. This method provides high sensitivity and high specificity. The instrumentation commonly applied in GC/MS is discussed under the MS/MS Instrumentation heading, which appears earlier in this chapter. [Pg.17]

Myosin-I molecules have several IQ sequences on or near the head and have light chains associated with them (Cheney and Mooseker, 1992 Cheney et al., 1993). Frequently, the light chains appear to be calmodulin molecules and some myosin-I molecules can bind three to four molecules of calmodulin at one time. Brush-border and adrenal myosin-I also bind calmodulin. Acanthamoeba myosin-I has a light chain that can be removed, in vitro, without adversely affecting the ATPase activity or the heavy chain phosphorylation (Korn and Hammer, 1988). The role of these calmodulin molecules in regulating myosin-I is complex and poorly understood. One possibility is that the calmodulin molecules dissociate from the heavy chains when calcium binds to the calmodulin, thereby imparting greater flexibility to the head of the myosin-I molecules. [Pg.70]

If intracellular levels of ATP drop (eg, after death), ATP is not available to bind the S-1 head (step 4 above), actin does not dissociate, and relaxation (step 5) does not occur. This is the explanation for r or mortis, the stiffening of the body that occurs after death. [Pg.562]

Figure 13. Action spectrum of the linear He I Cl complex near the He + I Cl(By = 2) dissociation limit obtained by scanning the excitation laser through the ICl B—X, 2-0 region and monitoring the l Cl E—>X fluorescence induced by the temporally delayed probe laser, which was fixed on the l Cl E—B, 11-2 band head, (a). The transition energy is plotted relative to the I Cl B—X, 2-0 band origin, 17,664.08 cm . Panels (b), (c), and (d) are the rotational product state spectra obtained when fixing the excitation laser on the lines denoted with the corresponding panel letter. The probe laser was scanned through the ICl B—X, 11-2 region. Modified with permission from Ref. [51]. Figure 13. Action spectrum of the linear He I Cl complex near the He + I Cl(By = 2) dissociation limit obtained by scanning the excitation laser through the ICl B—X, 2-0 region and monitoring the l Cl E—>X fluorescence induced by the temporally delayed probe laser, which was fixed on the l Cl E—B, 11-2 band head, (a). The transition energy is plotted relative to the I Cl B—X, 2-0 band origin, 17,664.08 cm . Panels (b), (c), and (d) are the rotational product state spectra obtained when fixing the excitation laser on the lines denoted with the corresponding panel letter. The probe laser was scanned through the ICl B—X, 11-2 region. Modified with permission from Ref. [51].
Sucrose changes the dynamic structure of water molecules, which, in turn, affects the manner of aggregation of the DPPE. Citric acid changes the degree of dissociation of the head group of the DPPE molecules. It becomes, therefore, apparent that each chemical species affects the viscoelastic behavior of the lipid thin film in a characteristic manner. [Pg.242]

The bond dissociation energies that follow are taken from the review of McMillan and Golden [Ann. Rev. Phys. Chem. 33, 493 (1982)]. The reader should refer to this publication for the methods of determining the values presented, their uncertainty, and the original sources. In the tables presented, all bond energies and heats of formation are in kJ/mol. The values listed in the first column are the heats of formation at 298 K for the reference radical and those above the column heading for the associated radical. Thus, the tables presented are not only a source of bond energies, but also of heats of formation of radicals. [Pg.693]

Figure 12, Schematic mechanism for impulsive reaction of thermal energy reaction of K with oriented CF3I. The electron is assumed to be transferred at large distance to the molecule irrespective of orientation. The molecular ion is formed in a repulsive state that promptly dissociates, ejecting the T ion in the direction of the molecular axis, and the K is dragged off by the departing T resulting in backward scattering for heads orientation and forward scattering for tails as observed. Figure 12, Schematic mechanism for impulsive reaction of thermal energy reaction of K with oriented CF3I. The electron is assumed to be transferred at large distance to the molecule irrespective of orientation. The molecular ion is formed in a repulsive state that promptly dissociates, ejecting the T ion in the direction of the molecular axis, and the K is dragged off by the departing T resulting in backward scattering for heads orientation and forward scattering for tails as observed.
Figure 14. Schematic illustration of velocity components as the molecular ion dissociates in heads and tails orientations. In the heads orientation, the nascent ions collide head on with a higher relative velocity than in the tails orientation, where one ion must catch up with the other. Figure 14. Schematic illustration of velocity components as the molecular ion dissociates in heads and tails orientations. In the heads orientation, the nascent ions collide head on with a higher relative velocity than in the tails orientation, where one ion must catch up with the other.

See other pages where Head dissociation is mentioned: [Pg.1424]    [Pg.997]    [Pg.12]    [Pg.160]    [Pg.1424]    [Pg.997]    [Pg.12]    [Pg.160]    [Pg.428]    [Pg.296]    [Pg.536]    [Pg.544]    [Pg.552]    [Pg.552]    [Pg.203]    [Pg.23]    [Pg.224]    [Pg.29]    [Pg.32]    [Pg.62]    [Pg.173]    [Pg.495]    [Pg.571]    [Pg.231]    [Pg.233]    [Pg.70]    [Pg.256]    [Pg.130]    [Pg.14]    [Pg.65]    [Pg.97]    [Pg.74]    [Pg.23]    [Pg.416]    [Pg.358]    [Pg.138]    [Pg.173]    [Pg.333]    [Pg.384]    [Pg.296]    [Pg.372]    [Pg.21]    [Pg.314]    [Pg.175]   
See also in sourсe #XX -- [ Pg.3 ]




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