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Figure 6.8. (a) Transmittance vs. water content added to the dioxane solution of P(tBA46-co-AA22)-b-PAzoMA74 (initial concentration, 1 mg mL 1) without and with UV irradiation. (b) Transmittance vs. water content added to the tetrahydrofuran solution of P(tBA46-co-AA22)-b-PAzoMA74 (initial concentration, 1 mg mL 1) without and with UV irradiation. (c) Transmittance vs. water content added to the dioxane solution of P(tBA19-co-AA33)-b-PAzoMA31 (initial concentration, 1 mg mL 1) without and with UV irradiation. Source: Tong et al., 2005.

141 tions in the derivation of Eq. (2.7.16). J. Koutecky gave a rigorous solution for diffusion to a growing sphere in the form of a power series. His solution has the form / = -v/-/ lin (l + 1.04a-lDl/2t1/e) where a = (A0/4JZ)1/2 f=ls. 2.7.3 (2.7.18)

Some blade chassis support add-on cards only as daughter or mezzanine cards to their blades. Some vendors/chassis have standard slots for PCI Express cards for installing special cards to be allocated to a specific blade, or in some cases, shared across blades.

or PEO-b-PAzoMA. Moreover, the effect of BCP composition is related to the used solvent. The more the increase in polarity of the hydrophobic block due to the trans cis isomerization of azobenzene reduces the difference in solubility of the two blocks in a given solvent, the more ef cient the photoinduced dissociation of the micellar aggregates should be.

In hydrodynamic problems it is an advantage to transform all variables into dimensionless parameters by 'scaling' each variable, using constants characterizing the dimensions and other properties of a given system. Thus, in the differential equations describing the systems, these constants are combined into dimensionless numbers or criteria. This formulation of the problem is very convenient because a process may be characterized in a much more general way by using the dimensionless criteria and, furthermore, in more complicated cases it is possible to find the properties of a system using a small model and then to apply the results to a large device keeping the criteria constant. In consideration of the hydrodynamic problem alone, it is usually attempted to characterize the studied system by three quantities, the characteristic length / (e.g. the length of the plate in the direction of the flowing liquid or the radius of a rotating disk), the velocity of the flowing liquid outside the Prandtl layer Vo and the kinematic viscosity v. The Cartesian coordinates of the system, x, y and z, are referred to the characteristic length / and the components of the velocity vx, vy and vz within the Prandtl layer are referred to the characteristic velocity Vo, -t=X, ^=Y, ^=VU y= Z (2.7.19) (2.7.20)

If you have special requirements for cards not available as mezzanine cards and your chassis does not support PCI-E cards, you may not be able to run that application on a blade.

where u = x} y, z. When the first and third terms on the right-hand side of Eq. (2.7.8) are neglected, the Navier-Stokes equation is obtained in Cartesian coordinates as three equations: dX

The interest of using photoswitchable polarity of azobenzene to design lightresponsive polymer micelles goes beyond BCPs A nice example can be found in a study of Liu and Jiang who designed light-controllable, noncovalently connected polymer micelles involving no block copolymers (Liu and Jiang, 2006) They showed that the hydrogen (H)-bonded complex between an azobenzene-containing random copolymer, poly(4-phenylazo-maleinanil-co-4-vinylpyridine) (AzoMIVPy), and carboxy group-terminated polybutadiene (CPB) was soluble in toluene, with azobenzene moieties in the trans form Under UV light irradiation, the increase in polarity with cis azobenzene renders AzoMI-VPy insoluble, leading to the formation of micelles with the AzoMI-VPy core The CPB shell, however, remains soluble in the solvent Upon visible light irradiation, the micelles were dissociated The change between the micellar and soluble polymer complex under UV and visible light was reversible.

The dimensionless number appearing in Eq. (2.7.21), = Re is called the Reynolds number. (2.7.22)

Moreover, when the AzoMI-VPy micelle core was chemically cross-linked to afford the structural integrity, visible light irradiation could no longer dissociate the micelles, instead the core shell micelles (B250 nm) were transformed into larger hollow spheres (B900 nm) due to the solubility of AzoMI-VPy with azobenzene in the trans form As shown in Fig 69, dynamic light scattering (DLS) measurements found that the large change in size between core shell micelles and hollow spheres is also reversible upon alternating UV and visible light irradiation This striking optical switching of selfassembly displayed by H-bonded azobenzene-containing polymers is schematized in Fig 610 Other interesting photoisomerization-induced phenomena were also reported with polymer micellar aggregates formed by azobenzene-containing amphiphilic BCPs Using a diblock copolymer composed of PEO and poly{2-[ethyl(4-(4cyanophenylazo)-phenyl)amino]ethyl methacrylate} (PEO-b-PEPAEMA), Wang et al showed photoinduced deformation of spherical micelles under linearly polarized Ar+ laser irradiation (488 nm) (Wang et al.

Q Will you be running I/O-intensive applications with requirements for a lot of bandwidth Q Is the communication mostly between blades in the chassis or from the blades to other servers/storage outside the chassis Q How many blades will be I/O-heavy Q How many network interfaces or NICS are required per application/ blade