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Thin functionalization

The Dirac delta function, very often used in quantum mechanics, is an infinitely tall but infinitely thin function, which is anathema to some mathematicians (it is called an improper function). In analogy to what the Kronecker delta does, the Dirac delta function could be called an "integral killer" because... [Pg.105]

Recent development in multilayer sensor architecture using sequential electrochemical polymerization of pyrrole and pyrrole derivatives to entrap enzymes was tested on a tyrosinase-based phenol sensor [127]. A phenothia-zine dye, thionine served as redox mediator and was covalently attached to the thin, functionalized first polypyrrole layer on Platinum disk electrodes. Then, a second layer of polypyrrole with entrapped tyrosinase was electrochemically deposited. The phenol sensor constructed in this manner effectively transferred electron from enz3Tne to the electrode surface. As all steps in preparation, including deposition of the enzyme-containing layer are carried out electrochemically, this technique may prove to be applicable for mass production of miniature sensors. [Pg.362]

In summary, coating the surface of Li jMOy cathode materials by appropriate thin functional layers that form buffer zone on their surface may provide the following advantages [91] (as exhibited in a recent review article) ... [Pg.308]

BouchtaUa SL, Janot JM, Deronzier A, Moutet JC, Seta P (2002) (60)FuUerene immobilized in a thin functionalized polypyrrole film basic principles for the elaboration of an oxygen sensor. Mater Sci Eng C 21 125-129 Boukhvalov DW, Katsnelson MI (2008) Tuning the gap in bilayer graphene using chemical functionalization density functional calculations. Phys Rev B 78 085413... [Pg.30]

Typically nsUho) is a shear thinning function of the Cross or Carreau form and tjuilho) is an extensionally thickening function of the same form (but n > 1). The ratio Wni/S = 1 in simple shear and 0 in pure extension. [Pg.91]

Fink, L. and Mandler, D. (2010) Thin functionalized films on cylindrical microelectrodes for electrochemical determination of Hg(II). /. Electroanal. Chem., 649, 153-158. [Pg.414]

Hence, by the combination of structural and transport properties, LSiF-LSNF nanoeomposite appears to be promising as cathode material for SOFC with apatite-type eleetrolyte provided the sintering temperature is below 1200 °C. The most promising approach consists in application of this composite as thin functional interlayer between the eleetrolyte and thin porous perovskite layer comprised of the same LSNF or other complex perovskite. This will help to mateh the thermal expansion coefficient of cathode and eleetrolyte as well as prevent too strong interaction between perovskite and electrolyte if sintering temperature will be high. [Pg.91]

Using this different cliches, it was possible to gravure print thin functioning layers of P3HT, PMMA, Ag-nanoparticle loaded ink and ITO. [Pg.290]

The best known type of SOFC anode-supported cells consists of a Ni/Zirconia cermet support layer, a thin functional anode, a thin dense yttria doped zirconia electrolyte layer and a thin Strontium doped lanthanum manganite (LSM) cathode layer (material alternatives are given in Fig. 8). Such cells have proved to be stable and durable for thousands of operation hours when operated at relatively mild conditions [9]. The degradation rate increases with increasing cell polarisation and increasing current density. The polarisation-dependent degradation has been identified to mainly originate from the cathode/electrolyte interface. However,... [Pg.213]

O. Wilhehn, Electrohydrodynamic spraying -Transport, mass and heat transfer of charged droplets and their application to the deposition of thin functional films, Swiss Federal Institute of Technology, Zurich, (2004). [Pg.883]

The preceding treatment relates primarily to flocculation rates, while the irreversible aging of emulsions involves the coalescence of droplets, the prelude to which is the thinning of the liquid film separating the droplets. Similar theories were developed by Spielman [54] and by Honig and co-workers [55], which added hydrodynamic considerations to basic DLVO theory. A successful experimental test of these equations was made by Bernstein and co-workers [56] (see also Ref. 57). Coalescence leads eventually to separation of bulk oil phase, and a practical measure of emulsion stability is the rate of increase of the volume of this phase, V, as a function of time. A useful equation is... [Pg.512]

A common choice of functional relationship between shear viscosity and shear rate, that u.sually gives a good prediction for the shear thinning region in pseudoplastic fluids, is the power law model proposed by de Waele (1923) and Ostwald (1925). This model is written as the following equation... [Pg.6]

Having obtained a mediocre solution to the problem, we now seek to improve it. The next step is to take two Gaussian functions parameterized so that one fits the STO close to the nucleus and the other contributes to the part of the orbital approximation that was too thin in the STO-IG case, the part away from the nucleus. We now have a function... [Pg.245]

Hindered amines, such as 4-(2,2,6,6-tetramethylpiperidinyl) decanedioate, serve as radical scavengers and will protect thin Aims under conditions in which ultraviolet absorbers are ineffective. Metal salts of nickel, such as dibutyldithiocarbamate, are used in polyolefins to quench singlet oxygen or elecbonically excited states of other species in the polymer. Zinc salts function as peroxide decomposers. [Pg.1011]

The steps may be so chosen as to correspond to consecutive points on the experimental isotherm. In practice it is more convenient to divide the desorption process into a number of standard steps, either of relative pressure, or of pore radius, which is of course a function of relative pressure. The amount given up during each step i must be converted into a liquid volume i , (by use of the normal liquid density) in some procedures the conversion is deferred to a late stage in the calculation, but conceptually it is preferable to undertake the conversion at the outset. As indicated earlier, the task then becomes (i) to calculate the contribution dv due to thinning of the adsorbed film, and thus obtain the core volume associated with the mean core radius r by the subtraction = t ... [Pg.134]

Schematic diagram showing how placing a thin layer of highly dispersed carbon onto the surface of a metal filament leads to an induced dipolar field having positive and negative image charges. The positive side is always on the metal, which is much less electronegative than carbon. This positive charge makes it much more difficult to remove electrons from the metal surface. The higher the value of a work function, the more difficult it is to remove an electron. Effectively, the layer of carbon increases the work function of the filament metal. Very finely divided silicon dioxide can be used in place of carbon. Schematic diagram showing how placing a thin layer of highly dispersed carbon onto the surface of a metal filament leads to an induced dipolar field having positive and negative image charges. The positive side is always on the metal, which is much less electronegative than carbon. This positive charge makes it much more difficult to remove electrons from the metal surface. The higher the value of a work function, the more difficult it is to remove an electron. Effectively, the layer of carbon increases the work function of the filament metal. Very finely divided silicon dioxide can be used in place of carbon.
The crack shape is defined by the function -ip. This function is assumed to be fixed. It is noteworthy that the problems of choice of the so-called extreme crack shapes were considered in (Khludnev, 1994 Khludnev, Sokolowski, 1997). We also address this problem in Sections 2.4 and 4.9. The solution regularity for biharmonic variational inequalities was analysed in (Frehse, 1973 Caffarelli et ah, 1979 Schild, 1984). The last paper also contains the results on the solution smoothness in the case of thin obstacles. As for general solution properties for the equilibrium problem of the plates having cracks, one may refer to (Morozov, 1984). Referring to this book, the boundary conditions imposed on crack faces have the equality type. In this case there is no interaction between the crack faces. [Pg.110]

A thin isotropic homogeneous plate is assumed to occupy a bounded domain C with the smooth boundary T. The crack Tc inside 0 is described by a sufficiently smooth function. The chosen direction of the normal n = to Tc defines positive T+ and negative T crack faces. [Pg.159]

Let us consider a thin homogeneous isotropic beam of thickness 2s. We assume that the beam mid-line coincides with the segment (0,1) of the axis X. At the point y = 1/2, the beam has an inclined cut as a segment having the angle a with the vertical line, 0 < tana < 2e). We look for the function % = (W, w) of horizontal displacements W(x) and vertical displacements w(x) provided that the external forces g(x),f(x) are given. The condition of clamped edges... [Pg.229]


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See also in sourсe #XX -- [ Pg.454 ]




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