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Thermal interactions

Emission spectrometry Interaction thermal- radiation energy -species Emitted radiation quanta, hv Photo multiplier tubes, photoplate Spectrum ... [Pg.72]

Common bean protein and procyanidin interactions can be hydrophilic or hydrophobic, depending on the sites on the protein available for interaction. Thermal processing can denature the protein and change the type of interaction possible. Once bean protein is denatured, hydrophobic interactions between the protein and procyanidin are likely. Since the strength of hydrophobic interactions increases with increased in temperature, the interaction between protein and procyanidin will be enhanced during thermal processing. Removal of procyanidin will be easiest prior to thermal processing. [Pg.140]

Maurice, T.J., Slade, L., Page, C., and Sirett, R. (1985). Polysaeeharide-water interactions-Thermal behavior of starch. In D. Simatos and J.L. Multon (Eds.), Properties of Water in Foods. Martinus Nijhoff, Dordrecht, pp. 211-227. [Pg.120]

J. C. Tully, Dynamics of gas-surface interactions Thermal desorption... [Pg.780]

The leading correction to zero-velocity, zero-temperature kinetic friction of the form (7 Inas described in Eq. (28) apparently also applies to more comphcated elastic manifolds. Charitat and Joanny [97] investigated a polymer that was dragged over a surface containing sparsely distributed, trapping sites. They analyzed the competition between the soft elastic, intramolecular interactions, thermal noise, and the tendency of some monomers in the chain... [Pg.217]

Undoubtedly, the realism of any simulation of a protein-solvent system will be further enhanced if all parts of the system experience thermal motion. Because water molecules interact most strongly with polar side chains and because the conformation of long polar side chains may be subject to considerable thermal disorder, flexibility of side chains, in particular, is a major aspect of protein-solvent interaction. Thermal motion of side chains could be provided for rather simply by rigid-body internal rotation of side chains about side-chain single bonds as part of the Monte Carlo process. [Pg.206]

Gemperle et al. (1998) presented an interesting set of guidelines on wearability, covering aspects such as placement, shape, movement, perception of space, sizing, body diversity, attachments, containment, weight accessibility, sensory interaction, thermal. [Pg.173]

Senda, T., He, Y. and Inoue, Y. (2002) Biodegradable blends of poly(E-caprolactone) with o-chitin and chitosan specific interactions, thermal properties and crystallisation behaviour. Polymer International, 51,33-39. [Pg.80]

For a system in which interactions occur, AHm>0, a temperature exists below which complete miscibility is unfavourable. For weak interactions thermal motion may still sufficiently randomize the positions of the components on the lattice to allow the use of the ideal entropy of mixing. This is the basis for the concept of a regular solution. The enthalpy of mixing can be expressed in terms of an exchange energy, a>, given by ... [Pg.244]

Godfrey, W.M., Tagavi, K.A., Cremers, C.J., and Menguc, M.R 1993. Interactive thermal modeling of electronic circuit boards. IEEE Trans. Comp., Hybrids, Manuf. Technol. CHMT-16(8)978-985. [Pg.1350]

Huang JC, He CB, Xiao Y, Mya KY, Dai J, Slow YP. Pol5rtmide/POSS nanocomposites interfacial interaction, thermal properties and mechanical properties. Pol)mer 2003 44 4491-4499. [Pg.195]

PbTlOa Substrate deflection Stress evolution during heating. Effect ot solvent/polymeric network Interaction, thermal expansion mismatch, and crystallization Senguptd(1998)... [Pg.249]

The thermal conductivity of a multicomponent mixture of monatomic species therefore requires a knowledge of the diermal conductivity of the pure components and of three quantities characteristic of the unlike interaction. The final three quantities may be obtained by direct calculation from intermolecular potentials, whereas the interaction thermal conductivity, Xgg, can also be obtained by means of an analysis of viscosity and/or diffusion measurements through equations (4.112) and (4.125) or by the application of equation (4.122) to an analysis of the thermal conductivity data for all possible binary mixtures, or by a combination of both. If experimental data are used in the prediction it may be necessary to estimate both and This is readily done using a realistic model potential or the correlations of the extended law of corresponding states (Maitland et al. 1987). Generally, either of these procedures can be expected to yield thermal conductivity predictions with an accuracy of a few percent for monatomic systems. Naturally, all of the methods of evaluating the properties of the pure components and the quantities characteristic of binary interactions that were discussed in the case of viscosity are available for use here too. [Pg.59]

The first term of equation (4.127) is an approximation to the translational contribution to the thermal conductivity of the mixture. It is obtained by making use of equations (4.122)-(4.125) for the thermal conductivity of a monatomic gas mixture. For this purpose approximate translational contributions to the thermal conductivity of each pure component X, tr and an interaction thermal conductivity for each unlike interaction Xqq are evaluated by the heuristic application of equation (4.125) for monatomic species to polyatomic gases. Thus, the technique requires the availability of experimental viscosity data for pure gases and the interaction viscosity for each binary system or estimates of them. As the discussion of Section 4.2 makes clear, the use of... [Pg.60]

The interaction thermal conductivity A.,y is related to the interaction viscosity rnj. [Pg.267]

In addition, the interaction thermal conductivity Xj is obtained from the interaction viscosity derived in the previous section by means of the equation... [Pg.391]

When membranes fuse, the so-called stalk hypothesis suggests that the intermediate hemifusion state (Fig. 6.4c) comprises a structure in which proximal monolayers layers are connected by a bent stalk and the distal layers are pulled towards each other, thus forming a dimple (see also Fig. 6.5) The stalk model has been supported by theoretical and experimental observations. The fusion of model membranes appears to occur via the same series of fusion intermediates as those in vivo, although the approach of membranes is not Rab/SNARE mediated but is driven by reduced bilayer repulsion forces arising from hydration, electrostatic interactions, thermal fluctuations (Helfrich interaction) or osmotic stress. Membrane fusion is also promoted by defects introduced into the membrane by lateral phase separation (for example of lipid rafts, see above), high spontaneous membrane curvature, or addition of macromolecules or proteins into the membrane. [Pg.281]

PS Tertiary amine (copolymerization) PS/AC Ionic Interaction Thermal 221... [Pg.32]

Changes in enthalpy translating into temperature variations occur during intracellular chemical and biochemical interactions. Thermal imaging becomes then feasible and the commercially available tris(P-diketonate) [Eu(tta)3(H20)2] with temperature-dependent phosphorescence plays the role of a luminescence thermometer [68]. The chelate readily stains biological membranes and while its luminescence in aqueous medium is weak, it is more important and steady in lipophilic environments. The dependence of its emission intensity upon temperature when integrated into liposomal membranes is shown on the left part of Fig. 4.8. Intracellular heat waves in Chinese hamster ovary (CHO) cells were monitored by... [Pg.146]


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See also in sourсe #XX -- [ Pg.11 , Pg.15 , Pg.43 , Pg.45 , Pg.58 , Pg.71 ]

See also in sourсe #XX -- [ Pg.203 , Pg.230 ]




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Thermal gradient interaction chromatography

Thermal gradient interaction chromatography TGIC)

Thermal interaction in furnaces

Thermal interaction with material

Thermal interactions with proteins

Thermal interactions, volatile compounds

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