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With the availability of 10Gbps Ethernet, users are questioning the need to implement yet another network for their storage, especially if they are moving to blade systems. Why not just use Ethernet This is a question worth exploring. Several storage protocols use TCP/IP over Ethernet. Two that are addressed in this book are the NAS (NFS and CIFS) and iSCSI protocols. The arguments against using TCP/IP as a storage network protocol involve guaranteeing reliable performance using this chatty network protocol, especially if your applications require a great deal of I/O. What if your TCP/IP network becomes overloaded and I/O requests can t be serviced Most applications do not deal with I/O timeouts or dropped requests very well, even with the advent of SANs. One typical way to get around this is to isolate your storage network from your communications network something you would be doing by default if you were to implement a Fibre Channel SAN. Another aspect of TCP/IP that is less than optimal is that it is most often processed in software as part of the operating system. It is not unheard of for an I/O-intensive application to consume as much as 80% of the CPU in TCP/IP processing only. Obviously, it would be better to have the CPU working on business-related activities rather than OS activities. To address this, TCP Offload Engines (TOEs) implement the TCP/IP protocol in hardware and are placed on NICs. This makes for very efficient and fast processing of all network traffic, including NAS and iSCSI storage traffic.

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Cis form ratio, % 96 94 95 97 87 90 94 93 89 90 90 89 90 90

where ut is the mobility^ of the particle (the velocity of the particle under the influence of unit force, in units of NT1 mol m s"1), zt its charge number and c, its concentration. For the migration flux, the driving force is the molar electric energy gradient multiplied by 1, that is Xmigr=-z,Fgrad0 (2.3.12)

Aspect ratio (L/D) Trans form 5.0 5.1 5.4 4.5 2.6 3.3 3.9 5.2 3.0 4.3 4.4 2.1 2.5 5.4 Cis form 1.3 1.2 1.2 1.3 1.7 1.1 1.1 1.4 2.2 1.8 1.6 3.3 4.5 1.4

The corresponding phenomenological coefficient is then given by the relationship L migr = W/-c, (2.3.13)

The flux of charge, connected with the mass flux of the electrically charged species, is given by Faraday's law for the equivalence of the current density and the material fluxes: j = S^J/ (2.3.14)

33 69 72 83 50 65 79 102 104 127 187 74 51 203 143

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In a blade environment, TOEs are implemented as daughter cards and can be added just as another NIC would be, by connecting it to the I/O expansion adapter on the blade. If you plan to connect blades to an existing SAN, either FC or iSCSI, or if you choose to implement your SAN using specific switches and storage, it is important for you to check with your vendors to verify that the blade I/O expansion adapters and switch modules are interoperable with their hardware.

Thus, in the case of migration material fluxes (Eq. 2.3.11) it holds for the partial current density (the contribution of the ith ion to the overall current density) that j , = -UiZJF2^rgrad 0 (2.3.15)

32.0 28.9 36.6 68.7 44.3 48.4 49.0 10.7 59.9 129 141 4.9 15.6 202 128

tThe term mobility is used to describe the influence of the drag of the medium on the movement of a particle caused by an unspecified force (the unit of w, is, for example, mol. m s ^ N " 1 ) which may be diffusivity (diffusion coefficient) with a chemical potential gradient as the driving force and electrolytic mobility connected with the electric field.

The best way to implement storage with one or many blade systems is highly dependent upon your business goals. This section explains the trade-offs in many of the implementation decisions you will face.

trans-Azo-6

(2.3.16)

cis-Azo-6

(2.3.17)

It s not often you will find a traditional server with no onboard storage, even if it is used only to boot the system. However, with blade servers, there are a number of arguments for using diskless (also called anonymous or stateless) blades:

trans-Azo-10

where K is the conductivity of the system, i.e. this result is identical with Eq. (2.3.7). Fick's first law, J , , d i f f = - A grade, or