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Transient field reversals

Electroporation. When bacteria are exposed to an electric field a number of physical and biochemical changes occur. The bacterial membrane becomes polarized at low electric field. When the membrane potential reaches a critical value of 200—300 mV, areas of reversible local disorganization and transient breakdown occur resulting in a permeable membrane. This results in both molecular influx and efflux. The nature of the membrane disturbance is not clearly understood but bacteria, yeast, and fungi are capable of DNA uptake (see Yeasts). This method, called electroporation, has been used to transform a variety of bacterial and yeast strains that are recalcitrant to other methods (2). Apparatus for electroporation is commercially available, and constant improvements in the design are being made. [Pg.247]

Polymer liquid crystal solutions respond in an interesting way to a transient flow field. For example, a damped oscillatory response was observed upon a flow inception or flow reversal [150,156,157], and the strain was recovered to some extent after a creeping flow [158], These phenomena suggest that liquid crystal solutions have some textured structure, i.e., the spatial variation in the... [Pg.147]

This electro-optical effect, commonly observed as transient changes in optical birefringence of a solution following application, removal, or reversal of a biasing electric field E(t), has been used extensively as a probe of dynamics of blopolymer solutions, notably by O Konski, and is a valuable tool because it gives information different in form, but related to, results from conventional dielectric relaxation measurements. The state of the subject to 1975 has been comprehensively presented in two review volumes edited by O Konski (25). The discussion here is confined to an outline of a response theory treatment, to be published in more detail elsewhere, of the quadratic effect. The results are more general than earlier ones obtained from rotational diffusion models and should be a useful basis for further theoretical and experimental developments. [Pg.71]

If a piezoelectric plate (Fig. 6.1), polarized in the direction indicated by P, carries electrodes over its two flat faces, then a compressive stress causes a transient current to flow in the external circuit a tensile stress produces current in the opposite sense (Fig. 6.1(a)). Conversely, the application of an electric field produces strain in the crystal, say a negative strain reversal of the field causes a positive strain (Fig. 6.1(b)). The changes in polarization which accompany the direct piezoelectric effect manifest themselves in the appearance of charges on the crystal surface (see Eq. (2.71)) and, in the case of a closed circuit, in a current. [Pg.340]

By splitting the quasi-steady-state assumption of diffusion of particles under the action of the interaction force field into two parts, kinetic equations which account for accumulation at both the primary and secondary minimum are formulated. Conditions are established under which, after a short transient, reversible adsorption or coagulation can be treated by neglecting accumulation at the secondary minimum. The effect of tangential velocity of particles on the rate of reversible adsorption is analyzed and a criterion established when the effect... [Pg.141]

An aspect of the ES FR that has not been fully exploited as yet is the fact that the dissipation function is sensitive to the choice of the distribution function. Therefore, if a system is presumed to have a particular equilibrium distribution function, with an associated dissipation function, then a field is applied, the transient ES FR should be satisfied for all time. This provides a way of testing if a system is equilibrated, for example. If the FR is not satisfied for the presumed Q, then it indicates that the equilibrium state is not what was expected. This fact has recently been used to establish that domains of the nondissipative, nonequilibrium distributions of glassy systems can be described by Boltzmann weights. Apart from the reversibility of the dynamics, the other key assumption in the derivation of the transient ES FR is that the initial distribution and the dynamics are ergodically consistent. In the same paper, Williams and Evans demonstrated that away from the actual glass... [Pg.186]

Leeuwen theorem. Marathe and Dhar study an Ising spin in a time-varying magnetic field. They verify the Crooks FR and JE, and confirm that time reversibility is required for the transient ES FR. They also observe that the steady state ES FR is not obeyed, confirming that this is an asymptotic result and indicating that observation times were insufficient for convergence. [Pg.194]

Zhdanov, M. S.., and M. A. Frenkel, 1983a, The solution of the inverse problems on the basis of the analytical continuation of the transient electromagnetic field in reverse time J. Geomag. Geoelectr., 35, 747-765. ... [Pg.359]

This is the basic principle of the persistent radical effect. As shown in this review, there are many variants, because there are additional reversible and irreversible reactions of the transient radicals, but these do not alter the essentials. Although it is quite natural, the principle seems somehow paradoxical, and it is not easily accepted on first sight. It took a long time from its first formulation in 19365 and several reinventions612 until it is now clearly recognized that it operates in rather diverse branches of chemistry. This review is a first attempt to cover all major aspects and to illustrate them with examples from different fields. [Pg.303]

Fig. 2. (A) Light-induced EPR transient of P680 in PS-II particles containing 2 mM NH2OH and (B) EPR spectrum constructed from the type of transient signal in (A) (C) Flash-induced EPR transients at 3318 G [trace (b)] and 3330 G [trace (a)] in PS-II particles treated with both acetate and FCCP, and (D) EPR spectra constructed from the transients in (C) (a) and (b) in (D) refer to magnetic fields for traces in (C). See text for discussion. (A, B) from Ghanotakis and Babcock (1983) Hydroxylamine as an inhibitor between Z and P680 in phofosysfem II. FEBS Lett 153 233 (C, D) from Bock, Gerken, Stehlick and Witt (1988) Time resolved EPR on photosystem II particles after irreversible and reversible inhibition of water cleavage with high concentrations of acetate. FEBS Lett 227 143, 144. Fig. 2. (A) Light-induced EPR transient of P680 in PS-II particles containing 2 mM NH2OH and (B) EPR spectrum constructed from the type of transient signal in (A) (C) Flash-induced EPR transients at 3318 G [trace (b)] and 3330 G [trace (a)] in PS-II particles treated with both acetate and FCCP, and (D) EPR spectra constructed from the transients in (C) (a) and (b) in (D) refer to magnetic fields for traces in (C). See text for discussion. (A, B) from Ghanotakis and Babcock (1983) Hydroxylamine as an inhibitor between Z and P680 in phofosysfem II. FEBS Lett 153 233 (C, D) from Bock, Gerken, Stehlick and Witt (1988) Time resolved EPR on photosystem II particles after irreversible and reversible inhibition of water cleavage with high concentrations of acetate. FEBS Lett 227 143, 144.
An example of such a series of transient experiments for a sample of paper without conductive additives (softwood Kraft pulp, 450 CSF, 80 g/m2 basis weight, Sample 1), is shown in Fig. 16. This series of transient currents represents the electric field dependence of charge transport associated with mobile ions within the water associated with the fibrous network of the papor. The initial transient current, labeled (a), corresponds to the first application of an electric field (E = 2.5 x 103 Volts/cm) to the new sample. After reversing the polarity of the power supply an electric field of the same magnitude is applied to the sample which leads to the transient current shown by label (b) in Fig. 16. (N.B. the scale of the ordinate is different for... [Pg.520]

Fig. 16 (a)). Again reversing the polarity of the voltage and maintaining the same value of the electric field leads to the transient current labeled (c). Subsequent experiments, where the magnitude of the electric field was monotonically increased but where the polarity of the power supply was first positive and then negative, results in the transient current pairs (d) and (e), (f) and (g), and (h) and (i), respectively. [Pg.520]


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See also in sourсe #XX -- [ Pg.856 ]




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