The ion and polymer content of polyelectrolyte multilayers constructed via layer-by-layer deposition
have been directly probed using radioanalytical methods. Multilayers were fabricated using salt-containing or
salt-free solutions. Charges on polyions quantitatively balance each other. As-deposited multilayers contain
no salt ions within a limit of detection of a few ppm. All excess charge, which is reversed on each deposition
step, resides at the surface. Surface charge controls the amount of polymer deposited and represents, on average,
one-half of the charge within a single molecular layer. Internal charge can be regulated following deposition
if one of the polyelectrolytes employed is redox-active, such as a polyviologen. Under electrochemical reduction,
bulk charge compensation in a polyviologen/poly(styrene sulfonate) multilayer is preserved mainly by cation
influx. Residual salt ions accumulate as conformational changes occur during repeated electrochemical cycling.
When a thermally labile precursor to poly(p-phenylene vinylene) is incorporated as polycation, salt cation
uptake is observed when positive charge is thermally eliminated from the multilayer. Evidence for disruption
of this structure is observed when the charge density on one of the constituents approaches zero. For typical
deposition times, usually up to 1 h, polymer deposition is kinetically irreversible, and the top layer is not
stripped from the surface on exposure to its oppositely charged counterpart. These results provide further
confirmation of extensive interpenetration and disorder as well as limited mobility within polyelectrolyte
multilayers.
In this study, we have demonstrated a simple ionic polymerization route for the fabrication of a magnetically separable adsorbent, that is, activated carbon/cobalt ferrite/alginate composite beads, for effective dye removal from aqueous solution. Adsorption characteristics of the as-fabricated magnetic beads were assessed by using methylene blue (MB) as an adsorbate. The isotherms, kinetics, and thermodynamics of the adsorption of MB onto the magnetic beads have been studied at various experimental conditions (initial dye concentration, contact time, solution pH, and temperature). The kinetics of the adsorption process was found to follow the pseudosecond-order kinetics. The equilibrium data fitted well to both the Langmuir and the Freundlich models. Various thermodynamic parameters such as the standard Gibbs energy (ΔG°), standard enthalpy (ΔH°), and standard entropy (ΔS°) changes were calculated. The prepared magnetic beads had a high magnetic sensitivity under an external magnetic field, which provides an easy and efficient way to separate the beads from aqueous solution.
This paper asks a new question: how can we control the collective behavior of self-organized multi-agent systems? We try to answer the question by proposing a new notion called 'Soft Control', which keeps the local rule of the existing agents in the system. We show the feasibility of soft control by a case study. Consider the simple but typical distributed multi-agent model proposed by Vicsek et al. for flocking of birds: each agent moves with the same speed but with different headings which are updated using a local rule based on the average of its own heading and the headings of its neighbors.Most studies of this model are about the self-organized collective behavior, such as synchronization of headings. We want to intervene in the collective behavior (headings) of the group by soft control. A specified method is to add a special agent, called a 'Shill', which can be controlled by us but is treated as an ordinary agent by other agents. We construct a control law for the shill so that it can synchronize the whole group to an objective heading. This control law is proved to be effective analytically and numerically. Note that soft control is different from the approach of distributed control. It is a natural way to intervene in the distributed systems. It may bring out many interesting issues and challenges on the control of complex systems.
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