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If you are connecting to a SAN, does your environment support boot from SAN, also known as PXE boot (Preboot Execution Environment) This option is generally supported for all Fibre Channel connections and, more recently, for most iSCSI SANs as well (depending on which iSCSI initiator is used). Check with your SAN vendor to confirm any configuration requirements for SAN boot (for example, OS levels, firmware, and so on). If you are connecting to a SAN and don t have a strong requirement for local disk storage on each blade, consider going diskless to simplify reprovisioning and management. Understand bandwidth requirements for your SAN connections. Fibre Channel HBAs are available for most blades in 2Gb and 4Gb options. If you are using iSCSI, would your performance benefit from a TCP Offload Engine (TOE) option on your IP NIC, if one is available

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It follows from Eq. (2.7.29) for / = r, and Eqs (2.7.13), (2.7.27) and (2.7.32) that Sh = 0.62 Re1/2Sc1/3 (2.7.33) When the relationship between the material flux and the parameters of the system can be calculated directly by solution of the appropriate differential equations, the criterion equation (2.7.30) has little significance. However, this is not possible in the great majority of practical systems, and thus the empirically determined criterial equation is of general validity for physically similar systems. It can form a basis for designing larger equipment on the basis of experiments with model systems. References

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, 2004a), an interference pattern of 532-nm visible light is applied to a reactive mixture lled in a 15-mm cell for photopolymerization, the mixture being composed of a diacrylate LC monomer (1,4-phenylene bis{4-[6(acryloyloxy)hexyloxy]benzoate}), a trifunctional monomer (cross-linker), a nematic LC (ML-1009 from Merck), an LC azobenzene compound (4-butyl-4methyoxy-azobenzene), and a photoinitiator (Rose Bengal with n-phenyl glycine) The concentration of azobenzene dopant is 7%, whereas the LC host is the major component (W75%) in the rest of the mixture Similar to the system discussed in Section 1152, the grating structure is formed upon exposure to the visible light interference pattern, since photoinduced polymerization of the monomers in high intensity regions, accompanied by monomer diffusion from dark (low intensity) regions, results in the formation of cross-linked polymer separated from the LCrich phase in dark regions.

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Agar, J. N., Diffusion and convection at electrodes, Faraday Soc. Discussions, 1, 26 (1947). Cussler, E. L., see page 20. Heyrovsky, J., and J. Kuta, Principles of Polarography, Academic Press, New York, 1966. Ibl, N., and O. Dossenbach, Convective mass transport, CTE, 6, 133 (1983). Levich, V. G., see page 20. Rousar, I., K. Micka, and A. Kimla, Electrochemical Engineering, Elsevier, Amsterdam, Vol. 1, 1985, Vol. 2, 1986.

Q Does your chassis support embedded switch modules for your SAN Q Will you be using an embedded switch module or passing through to an external SAN switch

Again, the consideration of the electrical potential in the electrolyte, and especially the consideration of the difference of potential in electrolyte and electrode, involve the consideration of quantities of which we have no apparent means of physical measurement, while the difference of potential in pieces of metal of the same kind attached to the electrodes is exactly one of the things which we can and do measure. J. W. Gibbs, 1899 3.1 Structure and Electrical Properties of Interfacial Regions

By changing the angle of intersection of the two laser beams, the holographic recording technique can control the thickness of the repeated bilayer (alternating polymer-rich and LC-rich regions), which determines the re ected wavelength (Bragg wavelength) The authors prepared a re ection grating with B70 bilayers stacked in the 15-mm cell, each of which has a thickness of 210 nm, corresponding to the selective re ection at 635 nm The mechanism of optical switching is schematized in Fig 1128, supported by experimental date Before UV light exposure, the index modulation is small because all LC components (nematic host, polymer, and azobenzene dopant) are aligned by rubbed cell surfaces and no selective re ection around 635 nm is observed.

In contrast to the previous chapters, dealing with the electrochemical properties of a single phase, this and the next three chapters will be concerned with electrochemical systems consisting of two or more phases in contact, at least one of which is an electronic or electrolytic conductor. The second phase may be either another electrolytic conductor (this case will be considered the most extensively), or another electronic conductor, a dielectric or a vacuum. Two phases in contact are separated by a surface called a phase boundary or interface (Fig. 3.1). The interface is unambiguously defined, for example, in the case of a metal-electrolyte solution interface. Surprisingly enough, even in the case of a liquid-liquid interface where the liquids are partially miscible the transition from one phase to the other is rather sharp. The term 'interface' will be distinguished from a related term, the interfacial region or interphase. This term denotes the region between the two phases where the properties vary markedly in contrast to those in the bulk of the phases. In the case of electrically conducting phases, charge distribution occurs in this region. The main criterion of the electrochemical properties of the interface is whether electric charge can pass sufficiently rapidly across it in both directions, or whether it is impermeable to charge transfer and thus has the 144

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