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The result of the establishment of phase equilibrium is the formation of differences of inner and outer potentials of both phases. These differences are defined by the equations

450 500 550 Wavelength (nm)

If you require local HDD support, look for redundancy and hot-swap capability to help minimize disruption due to disk failures. If a particular server application requires a large number of directconnect HDDs (for example, 10), blades may not be the right choice.

* -*

450 500 Wavelength (nm)

(3.1.6)

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Figure 11.29. (a) Schematic illustration of the re ection grating prepared with HPDLCs. The azobenzene compound dissolved in the LC droplets changes the LC order state upon UV and visible light irradiation. (b) Transmission spectra of an HPDLC-based re ection grating showing the optically switchable selective re ection in and without the absence of an electric eld. Source: Urbas et al., 2004b. Adapted with permission.

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network and I/O speed. Cheaper is just that less expensive but hopefully not cheaper quality. Blade and virtualization technologies offer these benefits in a variety of ways that are discussed in detail throughout this book. Clearly, the advances in processor chips are allowing more processor power and memory to fit onto circuit boards with greater reliability, yielding bigger, better, faster, and cheaper processor equivalents. Add in the virtualization and software management that enables blades to work together as a unified system, with components provisioned as needed, and the concepts of bigger, better, faster, and cheaper take on a whole new dimension.

(3.1.7)

The as-prepared grating has a high index modulation between polymer regions and the regions containing con ned LC droplets in which LC molecules are aligned; a re ection peak at B530 nm can be observed. In this state, exposure of the grating to UV light induces the nematic isotropic phase transition inside the

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It should be noted that phase equilibrium can be attained for charged species through far smaller transfer of particles from one phase into the other than for uncharged species, as the potential difference formed, 0(/3) 0(ar), decreases the original tendency for transfer between the two phases much faster than the changes in the original chemical potentials. The difference of the inner electrical potentials of the phases, A^0, is also called the Galvani potential difference and the analogous difference of the outer electrical potentials, A^/T/;, is termed the Volta potential difference.

In 1965 Intel s cofounder, Gordon Moore, predicted that the number of transistors on a chip (i.e., density) would double every 18 24 months. This prediction became known as Moore s Law, and has continued to bring processing-performance increases, and decreases in size as well as costs. This law has also been reflected in disk capacity and memory, which now take up less space on a motherboard or in a disk array. Back in the 1970s a single computer filled a room, whereas today we are able to carry a computer in our pocket. Computer memory in the 1970s was counted in bytes, whereas today our computers support terabytes of memory. The size reductions and increased density possible with blade technology come directly from the miniaturization of the components that make up the blade servers. Miniaturization has also had a significant effect on the software. The ability to put more memory and high-performance processors together has meant that software operating systems and programs can be more sophisticated. Most recently, server virtualization software has taken computing to a new level, to create multiple virtual servers where only one physical server used to be.

droplets, and the reduced index modulation results in a decrease in diffraction ef ciency. Subsequent visible light exposure recovers the initial re ection ef ciency. However, the re ection of the as-prepared grating can be turned off by applying an electric eld that aligns LC molecules inside the droplets to change the index modulation. With the grating under a voltage, the re ection can be switched on using UV light and switched off using visible light.

Equations (3.1.5) and (3.1.6) hold for any contact equilibrium of two phases with a common charged species. This species must be exchanged sufficiently rapidly between the two phases, so that the applicability of Eq. (3.1.5) is dependent on species i being transferred very quickly from phase a to phase jS and back again. It should be noted that the Galvani potential difference consists of the contribution of ions g(ion) and of the oriented dipoles g(dipole): A tf> = A^(ion) + Afe(dipole) (3.1.8) In solid-state physics, the electrochemical potential of the electron fie(a) is mostly replaced by the equivalent energy of the Fermi level eF. While the electrochemical potential is usually related to one mole of particles, the Fermi energy is related to a single electron, so that

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