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90 A special class of conductors are ionically and electronically conducting polymers (Sections 2.6.4 and 5.5.5). 2.4.2 Conductivity of electrolytes This part will be concerned with the properties of electrolytes (liquid or solid) under ordinary laboratory conditions (i.e. in the absence of strong external electric fields). The electroneutrality condition (Eq. 1.1.1) holds with sufficient accuracy for current flow under these conditions:

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In discussing virtualization, a number of terms (that are often misused) are helpful to define. Although these are not exhaustive definitions, they will explain how these terms are used within the context of this book. Terminology, especially when talking about both physical and virtualized resources, can get quite muddled.

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Bredenbeck J, et al 2003 Transient 2D IR spectroscopy: snapshots of the nonequilibrium ensemble during the picosecond conformational transition of a small peptide J Phys Chem B 107(33):8654 8660 Brown CJ 1966 A re nement of the crystal structure of azobenzene Acta Cryst 21(1): 146 152 Brown D, Natansohn A, Rochon P 1995 Azo polymers for reversible optical storage 5 Orientation and dipolar interactions of azobenzene side groups in copolymers and blends containing methyl methacrylate structural units Macromolecules 28(18):6116 6123 Brown EV, Granneman GR 1975 Cis trans isomerism in pyridyl analogs of azobenzene kinetic and molecular orbital analysis J Am Chem Soc 97(3):621 627 Bublitz D, et al 2000 Photoinduced deformation of azobenzene polyester lms Appl Phys B: Lasers Opt 70(6):863 865 Buffeteau T, Labarthet FL, Pezolet M, Sourisseau C 2001 Dynamics of photoinduced orientation of nonpolar azobenzene groups in polymer lms.

2^, = 0

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Characterization of the cis isomers by visible and FTIR spectroscopies Macromolecules 34(21):7514 7521 Burke SE, Barrett CJ 2003a Acid base equilibria of weak polyelectrolytes in multilayer thin lms Langmuir 19(8):3297 3303 Burke SE, Barrett CJ 2003b pH Responsive properties of multilayered poly(L lysine)/ hyaluronic acid surfaces Biomacromolecules 4(6):1773 1783 Burland DM, Miller RD, Walsh CA 1994 Second order nonlinearity in poled polymer systems Chem Rev 94(1):31 75 Camacho Lopez M, Finkelmann H, Palffy Muhoray P, Shelley M 2004 Fast liquid crystal elastomer swims into the dark Nat Mate 3(5):307 310 Campbell VE, et al 2006 Chromophore orientation dynamics, phase stability, and photorefractive effects in branched azobenzene chromophores Macromolecules 39(3):957 961 Caruso F 2001 Nanoengineering of particle surfaces Adv Mater 13(1):11 22 Caruso F, Mohwald H 1999 Protein multilayer formation on colloids through a stepwise self assembly technique J Am Chem Soc 1212(25):6039 6046 Chen AG, Brady DJ 1993.

When virtualization of physical resources involves combining multiple servers to act as one system, it is also known as aggregation. Clustering (discussed further in 9, Clustering and Blades ) is a way of aggregating systems. Some blade system vendors offer solutions that are specifically designed to aggregate blades and allow them to act as a single entity, with proprietary tools (for example, from Egenera and PANTA Systems) designed to help manage this process.

(2.4.1)

Two wavelength reversible holograms in azo dye doped nematic liquid crystals Appl Phys Lett 62(23):2920 2922 Chen JP, Gao JP, Wang ZY 1997a Preparation and photochemical study of soluble optically active block copolymethacrylates and azo containing random copolymetha crylates J Polym Sci, Part A 35(1):9 16 Chen SH, et al 1995 Novel glass forming organic materials 1 Adamantane with pendant cholesteryl, disperse red 1, and nematogenic groups Macromolecules 28(23):7775 7778 Chen SH, Mastrangelo JC, Shi H, Blanton TN, Bashir Hashemi A 1997b Novel glass forming organic materials 3 Cubane with pendant nematogens, carbazole, and disperse red 1 Macromolecules 30(1):93 97 Chiarelli PA, et al 2001 Controlled fabrication of polyelectrolyte multilayer thin lms using spin assembly Adv Mater 13(15):1167 1171 Cho J, Char K, Hong J D, Lee K B 2001 Fabrication of highly ordered multilayer lms using a spin self assembly method Adv Mater 13(14):1076 1078 Chung AJ, Rubner MF.

where ct are the concentrations of ions / and z, are their charge numbers. The basic equations for the current density (Faraday's law), electrolytic mobility and conductivity are (2.3.14), (2.3.15) and (2.3.17). The conductivity K = ^ z2F2uiCi = 2 N FUiCi

Disaggregation of servers allows multiple independent instances of an operating environment to run on a single server (dividing one physical server into multiple virtual servers). This is the typical usage of the term server virtualization. This type of virtualization allows for the consolidation of multiple, underutilized, physical servers onto one server with higher system utilization reducing management overhead, floor space, power, and cooling requirements. Server virtualization can be implemented in a variety of ways, with pros and cons associated with each. Implementation approaches include emulation, paravirtualization, hypervisors, hosted approach and OS virtualization, which are described later in this chapter. For clarity, in this book, when referring to physical hosts, the term server will be used. When referring to virtual servers, the term virtual machine or VM will be used.

2002 Methods of loading and releasing low molecular weight cationic molecules in weak polyelectrolyte multilayer lms Langmuir 18(4):1176 1183..

(2.4.2)

in dilute solutions is thus a linear function of the concentrations of the components and the proportionality constants are termed the (individual) ionic conductivities: li = zJP2ui = \zi\FUi (2.4.3)

Azo-10

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