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Figure 5.18 gives the TEM images of the colloidal spheres after the light irradiation. The TEM images of the colloidal spheres before light irradiation have been given in Fig. 5.8. PEAPE colloids do not show observable deformation after being irradiated for 2 h (Fig. 5.18a). After being irradiated for 20 min, the BP-AZCA colloidal spheres can be signi cantly elongated along the light polarization direction (Fig. 5.18b), which has been discussed in Section 5.4.2. The hybrid colloids show unique morphologies after the light irradiation, which are characterized by the spindlelike or tadpolelike shapes with dark spherical cores (Fig. 5.18c). Figure 5.19 shows the TEM images of the hybrid colloids containing different amounts of BP-AZ-CA before (Fig. 5.19a d) and after the light irradiation of the linearly polarized Ar+ laser beam for 2 h (Fig. 5.19e h). After the light irradiation, the colloids show different deformation degrees related to the BP-AZ-CA content. The hybrid colloids containing 80 wt% of BP-AZ-CA show a similar shape deformation as BP-AZ-CA colloids (Fig. 5.19e), although the degree of deformation is less for the same irradiation time period. The hybrid colloids containing 20 wt% of BP-AZ-CA can only show an insigni cant deformation under the same light irradiation condition (Fig. 5.19h). For the hybrid colloids containing 40% and 60 wt% of BP-AZ-CA (Fig. 5.19f, g), the shape deformation degrees are between the two cases aforementioned. As discussed earlier, the colloidal spheres formed from BP-AZ-CA can exhibit signi cant deformation upon Ar+ laser irradiation, whereas PEAPE colloids do not show such deformation under the same condition. Since every hybrid colloidal sphere shows a very similar deformation upon the light irradiation, it indicates that the colloid spheres are all composed of both BP-AZ-CA and PEAPE components. The fact that the deformation degree is lower than that of the

(6.2.14)

The conjugate driving force is the pressure gradient Ap multiplied by 1. Further, the relative flux of the dissolved substance compared to the flux of the solvent, i.e. the 'exchange' flux / D , is defined by the relationship

organizations. In today s global economy, especially with the amount of outsourcing occurring, being able to share computational as well as data resources worldwide is imperative. By now businesses are all too familiar with the challenges of 24 7 365 requirements. Increasingly, IT organizations are being pushed to leverage all their computing resources together to deliver dynamic computational access across the globe to advance their business objectives. The nomenclature grid computing brings to mind an electrical power grid, where a number of resources contribute to the pool of shared power to be accessed as needed. This is where the name utility computing originated. Although the promise of grid computing has not yet been realized, steady progress is being made. Grid computing is expected to see strong successes in financial services, oil exploration, medical research, security, entertainment, and mechanical engineering. Much like clusters, grid computing doesn t rely on high-powered computational engines; rather, it uses underutilized computational engines (workstations, PCs, mainframes, and so on), located on the network, anywhere in the world. As blade servers meet the criteria of being computational engines located on a network, along with their related blade component technologies, they will certainly see a bright future in grid computing.

Figure 5.18. TEM images of the colloids after they are exposed to a linearly polarized Ar+ laser beam for different time periods: (a) PEAPE, 2 h; (b) BP-AZ-CA, 20 min; (c) PEAPE/BP-AZ-CA (1:1, wt:wt), 2 h. Source: From Deng et al., 2007.

(6.2.15)

Figure 5.19. Typical TEM images of the PEAPE/BP-AZ-CA colloids containing a different percentage of PEAPE before and after the Ar+ laser irradiation for 2 h: (a) 20 wt%, before irradiation; (b) 40 wt%, before irradiation; (c) 60 wt%, before irradiation; (d) 90 wt%, before irradiation; (e) 20 wt%, after irradiation; (f) 40 wt%, after irradiation; (g) 60 wt%, after irradiation; (h) 90 wt%, after irradiation. Source: From Deng et al., 2007.

As decentralized enterprises shifted into the consolidation era and started ramping up centrally located groups of servers, the market was ripe for a more efficient and more cost effective way to store servers. The rack-mounted server market took off in the early 1990s as enterprises created high-end rackmounted server farms, which resided in the data center, under the control of the IT organization. The introduction of rack servers allowed users to configure racks of servers, networking equipment (for example, routers, switches, and firewalls) usually the size of one or two pizza boxes (1U and 2U), and storage devices (usually 9U) potentially from different vendors into a much smaller footprint than with traditional hardware. (See Figure 2.3.) With rack servers, devices are bolted in horizontally, and the user wires everything together behind the rack. Most of the major systems vendors offer rack-mounted versions of their products. Although rack-mounted servers were an improvement over previous hardware options, wiring the components together often created a mess. Furthermore, as the rack-server market grew, the software side lacked maturity in provisioning, virtualization, and systems-management tools. These areas have left opportunities for blade-server technology and server-virtualization software to deliver next-generation data center capabilities for the enterprise space.

where / s and / w are the fluxes of the salt and the solvent, respectively. The conjugate driving force is then the osmotic pressure gradient (multiplied by - 1 ) , since (cf. Eq. 1.1.17)