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The previous two problems associated with excessive exibility are likely to result in time and cost overruns. A patchwork deliverable that does not meet customer needs, for example, may result in rejection of the deliverable by the customers and may give rise to demands to redo the project. Clearly, a project that entails rework efforts will pose both time and budget slippages. If excessive exibility causes chaotic planning, this will lead to major inef ciencies in the implementation of the project. We will face false starts and about-faces. Resource utilization will be haphazard, since we will never be quite sure what resources and how many we should be using at any given time. With such inef ciencies, it is unlikely that we will meet our original budget and schedule targets.



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Figure 18.19 (Top) Diamond membrane (bright area) xed in a silicon frame (outer dark area). The image was taken under transmitted light microscopy. The inner dark area represents the eld where a combined mask of Ti/Si3 N4 was used to fabricate a very small hole in its centre. (Bottom) Diagrammatic cross-section





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U ua uw w xa xb xf y Dq DH q n l e ra ma hf hs hwf hws s overall heat transfer coef cient (W m-2 C-1) air ow velocity (m s-1) water ow velocity (m s-1) moisture content (kg/kg) transverse tube spacing (in the direction perpendicular to air- ow direction) (m) longitudinal tube spacing (in the air- ow direction) (m) half width of one n pattern (m) n thickness (m) log mean temperature difference ( C) log mean enthalpy difference (kJ/kg) n pattern angle (rad) kinematic viscosity of air (m2 s-1) under relaxation factor used in numerical solution schemes error or deviation (er relative deviation, ea absolute deviation) air density (kg m-3) air viscosity (kg m-1 s-1) n ef ciency of the dry n surface effectiveness of the dry surface n ef ciency of the wet n surface effectiveness of the wet surface contraction ratio

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Pierre Curie in their studies of tourmaline crystals Materials showing distinctive piezoelectric behaviour are ceramics with the perovskite structure, such as BaTiO3 , SrTiO3 , or Pb(Zr,Ti)O3 labelled as PZT For high temperature applications, materials such as AlN, LiNbO3 , langasite (La3 Ga5 SiO14 ), langanite (La3 Ga55 Nb05 O14 ), or langatite (La3 Ga55 Ta05 O14 ) [75] may be especially suited since they possess high Curie temperatures and a thermal stability of more than 1000 C In these materials the piezo coef cients and the coupling coef cients, which represent the amount of mechanical energy converted into electrical energy and vice versa, are, however, lower as compared with PZT Diamond, because of the symmetry of its lattice, is not piezoelectric and can only be used as a carrier material for this application.

Because piezoceramics are mostly brittle and have low stiffness, diamond is an excellent complementary carrier material and can be employed to develop mechanically stable actuators with high resonance frequencies Bilayers with a piezoelectric overlayer on a mechanical support layer are common in microsystem technologies and are called unimorphs Figure 188 shows calculated, rst order, resonance frequencies of multilayer cantilevers consisting of PZT, NCD, and PZT on NCD Additionally, some FEA data, which take the additional in uence of the metal electrode into account, are also included As can be seen, the resonance behaviour is largely determined by the diamond supporting lm, while the actuation is generated by the PZT overlayer An Al-overlayer electrode will degrade these properties only marginally The prerequisite for piezoelectricity in a material is an asymmetric lattice con guration, which implies spontaneous polarisation.

By applying mechanical loads, the dipole lengths in the crystal are varied, which generates an electrical charge dipole at the surfaces By adding metal electrodes to the surfaces, an electrical voltage can be measured, which is the direct piezoelectric effect Conversely, by applying a potential onto the electrodes the polar crystal can be distorted; this is consequently called inverse piezoelectric effect Both options are used for MEMS transducers either to detect mechanical deformation of.

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