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formulation, no distinction is made between solid or uid phases. Where distinctions do arise, it is in the computation of the material stress and material transport or advection. In the former, the use of a particle description for the solid provides a convenient location upon which to store the material deformation and any relevant history variables required for, say, a plasticity model. Regarding the latter, Eulerian advection schemes are typically quite diffusive, and would lead to an unacceptable smearing of a uid solid interface. Thus, performing advection by moving particles according to the local velocity eld eliminates this concern. At the beginning of each timestep, the particle state is projected rst to the computational nodes and then to the cell centers. This colocates the solid and uid data and allows the multimaterial CFD solution to proceed unaware of the presence of distinct phases. As stated above, the constitutive models for the solid materials are evaluated at the particle locations, and the divergence of the stress at the particles is computed at the cell centers. The Lagrangian phase of the CFD calculation is completed, including exchange of mass, momentum, and enthalpy. At this point, changes to the solid materials state are interpolated back to the particles and their state, including position, is updated. Fluid-phase materials are advected using a compatible advection scheme such as that described in Ref. [35]. Again, a full description can be found in Ref.[11].

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Tip If you re not sure of the command name but you know the menu or toolbar item, execute the command on the menu or toolbar and then press Esc. You see the command name on the command line.

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applications beyond MCE 2005. Like the reference MCE remote from Microsoft, the Firefly also has a home button to take you back to the main menu. Sadly, there are two bugs with the Firefly s software and MCE that keep it from getting a stronger recommendation. You can read more about those issues in the next section.

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In case of an unbound phase conjugate mirror, wPCM becomes in nite, the sin (x)/x function acts as a Dirac-like function, and Eq. (2) simpli es to

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of the output transistor that is to be driven. Moreover, nothing is said about the input network except that the input voltage waveform has to properly drive the device to operate as a switch (i.e. deeply pinched off and saturated). However, if the operating frequency enters the microwave region, both the approaches exhibit a degradation in performances. For instance, actual Class-F ampli ers are usually designed making use of two or three idlers only to control second and third output harmonic impedances. As frequency increases (e.g. >20 GHz), the control of both the second- and third-harmonic output impedances becomes troublesome since the active device output capacitive behaviour practically short-circuit higher components, not allowing the desired wave shaping. Moreover, for low-voltage applications, a Class-F strategy is not the best solution, since different methodologies (based on second-harmonic output impedance tuning) have demonstrated better performances [25]. On the other hand, the switching-mode operation of the active device, necessary to implement Class-E strategy, is not feasible in microwave communication systems since it requires that the power stage operates in saturated conditions, thus often increasing intermodulation distortion levels. As a consequence, while designing high-frequency power ampli ers for communication systems, the number of the voltage harmonics that are effectively controlled is limited to the second and third ones, while the highest are assumed to be short-circuited. With such hypotheses the drain ef ciency becomes = Pout,f Pdiss + Pout,f + Pout,2f + Pout,3f (4.54)

DISTINCT keyword. You also learned how to group results by a specified column or columns through the use of GROUP BY clauses

All performance metrics may be measured as presented in Section 9.3.3 over a period of 1 month. 9.3.5.3 Tra c pro le

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