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The Analogue Solution

Chapter 5 investigates the shape of liquid drops, bubbles, and the liquid surface in the vicinity of a solid surface, using the Laplace-Young equation. The last chapter. Chapter 6, contains a number of interesting properties and applications, such as the vibrational oscillations of soap film membranes and the application of soap films to the analogue solutions of the differential equations of Poisson and Laplace. [Pg.9]

The general ground work required for the understanding of the subsequent chapters is now complete. In the following chapters we shall examine such subjects as the draining processes in soap films, the analogue solutions to minimum area problems, and the shapes of fluid surfaces. [Pg.47]

We shall examine, using soap films, the analogue solutions to some two dimensional mathematical problems. These are problems that are restricted to a surface. [Pg.85]

These minimization problems were first investigated early in the nineteenth century by the mathematician Jacob Steiner They are often known collectively as the Steiner problem. The general problem of linking n points has not been solved analytically. It was the mathematician Richard Cour-anti4 i5 who first popularized the analogue solutions to these problems in the 1940 s. [Pg.97]

This is a simple application of the soap film to solve a problem satisfying the same differential equation. An important application of soap films to the analogue solution of problems occurs when the gradient at any point on the soap film is small. The Laplace-Young equation in Cartesian coordinates, Eq. (5.9), for the soap film surface... [Pg.180]

Isenberg, C. (1976) Soap Films The Analogue Solution to Some Practical Problems, Proc. Roy. Inst. Gt. Brit., 49, 53-75. [Pg.212]

Reversible inhibition is characterized by an equiUbrium between enzyme and inhibitor. Many reversible inhibitors are substrate analogues, and bear a close relationship to the normal substrate. When the inhibitor and the substrate compete for the same site on the enzyme, the inhibition is called competitive inhibition. In addition to the reaction described in equation 1, the competing reaction described in equation 3 proceeds when a competitive inhibitor I is added to the reaction solution. [Pg.288]

Systems that develop contractile forces are very intriguing as analogues of physiological muscles. The idea for gel muscles was based upon the work of Katchalsky and Kuhn. They have prepared polyelectrolyte films or fibers which become elongated or contracted in response to a change in pH of the surrounding solution, and have estimated the induced force and response time. The contraction of gel fibers is also achieved by electric fields. Use of electric fields has the merit that the signals are easily controlled. [Pg.159]

H. B. Gray Work on the excited states of soluble metal oxo species that in a sense are the homogeneous-solution analogues of Ti02-type materials is a promising direction to take, in my view. [Pg.34]

This approximation requires that cos. This behavior in fact follows from a Debye dielectric continuum model of the solvent when it is coupled to the solute nuclear motion [21,22] and then xs would be proportional to the longitudinal dielectric relaxation time of the solvent indeed, in the context of time dependent fluorescence (TDF), the Debye model leads to such an exponential dependence of the analogue... [Pg.242]

When the adsorbent molecides are not independent, we can no longer use the relation (D.2) for the GPF of the system. In this case, we must start from the GPF of the macroscopic system from which we can derive the general form of the BI for any concentration of the adsorbent molecule. The derivation is possible through the McMillan-Mayer theory of solution, but it is long and tedious, even for first-order deviations from an ideal solution. The reason is that, in the general case, the first-order deviations would depend on many second-virial coefficients [the analogue of the quantity B2(T) in Eq. (D.9)]. For each pair of occupancy states, say i and j, there will be a pair potential [/pp(R, i,j), and the corresponding second-virial coefficient... [Pg.319]


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