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Si Slabs

Figure 12.4 shows an example of experimental set up for a classical measurement of heat capacity the sample is glued onto a thin Si support slab. The thermometer is a doped silicon chip and the heater is made by a ( 60 nm thick) gold deposition pattern. Electrical wiring to the connect terminals are of superconductor (NbTi). The thermal conductance to the thermal bath (i.e. mixing chamber of a dilution refrigerator) is made with thin nylon thread. The Si slab, the thermometer and the heater represent the addendum whose heat... [Pg.286]

Figure 2.38 Schematic of the suspended-tube reactor (left and middle) and SEM (right) showing four suspended SiNx tubes connected to the Si reaction zone, Si slabs thermally linking the four tubes and a meandering Ti/Pt resistive heater/temperature sensor [72] (by courtesy of L. R. Arana). Figure 2.38 Schematic of the suspended-tube reactor (left and middle) and SEM (right) showing four suspended SiNx tubes connected to the Si reaction zone, Si slabs thermally linking the four tubes and a meandering Ti/Pt resistive heater/temperature sensor [72] (by courtesy of L. R. Arana).
Fig. 11 Scanning electron microscopy photos of microreactor produced by Jensen et al. for reforming of ammonia showing four freestanding SiN tubes, a suspended Si reaction zone with integrated thin-film platinum heater and temperature sensing resistor (TSR), and Si slabs wrapped around the four tubes. (From Ref.P l)... Fig. 11 Scanning electron microscopy photos of microreactor produced by Jensen et al. for reforming of ammonia showing four freestanding SiN tubes, a suspended Si reaction zone with integrated thin-film platinum heater and temperature sensing resistor (TSR), and Si slabs wrapped around the four tubes. (From Ref.P l)...
Conversion of GS to (GSi)r wiU be carried out for two of the four cases of Table 5-10. Case 1 is an idealization of a metal-heating slab furnace or glass furnace, with its plane sink Ai combining with refractory surface to complete the enclosure. With insertion into Eq. (5-173) of GSi, GS, and S Si after converting each to its gray plus clear form, one obtains... [Pg.586]

Top left Plan view of a slab consisting of cubes and double trigonal prisms in Gd5(Si,Ge)4 with (Si,Ge)2 dumbbells on top the gray square is part of the next slab and shows the mutual stacking of the slabs. Remaining images Side views parallel to the slabs... [Pg.239]

Section 4.8 The reconstructed Si(001) surface was modeled using a c(4 x 4) asymmetric slab with four layers. The bottom two layers were fixed at bulk positions. Reciprocal space was sampled with llxllxllfc points and the vacuum spacing was 17 A. [Pg.112]

The aggregation of the silica species in solution continues upon dilution with water [3], With TPA, the main final products at room temperature are nanoslabs (8), counting 396 Si atoms and composed of twelve precursors (5) (Fig.l). With TPA, it was experienced that the timing of the water addition was not very critical. The yield of Silicalite-1 nanoslabs on silica basis is typically 80% [1]. With TBA, there is a violent hydrolysis and gel formation when the water is added from the beginning. To avoid this, it is preferred to add water after complete hydrolysis. The MEL nanoslabs with occluded TBA rapidly dimerize at room temperature to result in the formation of slabs with dimensions of 1.3 x 4.0 x 8.0 nm [3], The product yield on silica basis is similar to the TPA system. With TEA, the amount of extractable silicate was much smaller. 1R spectra of the extracts recorded after 24 h stirring of the solutions are shown in Fig.3. [Pg.143]

Figure 2.2. Derivation of the standard neutron diffraction expression, Equation (2.SI). It is supposed that neutron plane waves proceed from the left and can be represented by the function eikz and impinge on a slab of material whose faces are defined by z = 0 and z = t. Consider an infinitesimal slice of this material defined by z=u> and z = co + da> and a ring of this slice confined between p and p + Ap where p is the radius of this ring. The wave function at z, a point on the axis of the ring and to the right of the slab will now, using the equations in the text, be given by Equation (2.48). Using the manipulations shown in the text, one then arrives at Equation (2.SI). Figure 2.2. Derivation of the standard neutron diffraction expression, Equation (2.SI). It is supposed that neutron plane waves proceed from the left and can be represented by the function eikz and impinge on a slab of material whose faces are defined by z = 0 and z = t. Consider an infinitesimal slice of this material defined by z=u> and z = co + da> and a ring of this slice confined between p and p + Ap where p is the radius of this ring. The wave function at z, a point on the axis of the ring and to the right of the slab will now, using the equations in the text, be given by Equation (2.48). Using the manipulations shown in the text, one then arrives at Equation (2.SI).

See other pages where Si Slabs is mentioned: [Pg.239]    [Pg.538]    [Pg.262]    [Pg.262]    [Pg.264]    [Pg.265]    [Pg.265]    [Pg.271]    [Pg.1654]    [Pg.22]    [Pg.132]    [Pg.310]    [Pg.314]    [Pg.321]    [Pg.337]    [Pg.344]    [Pg.288]    [Pg.239]    [Pg.538]    [Pg.262]    [Pg.262]    [Pg.264]    [Pg.265]    [Pg.265]    [Pg.271]    [Pg.1654]    [Pg.22]    [Pg.132]    [Pg.310]    [Pg.314]    [Pg.321]    [Pg.337]    [Pg.344]    [Pg.288]    [Pg.466]    [Pg.289]    [Pg.41]    [Pg.239]    [Pg.185]    [Pg.436]    [Pg.243]    [Pg.628]    [Pg.662]    [Pg.724]    [Pg.7]    [Pg.558]    [Pg.93]    [Pg.136]    [Pg.141]    [Pg.466]    [Pg.239]    [Pg.1174]    [Pg.644]    [Pg.100]    [Pg.421]    [Pg.253]   
See also in sourсe #XX -- [ Pg.310 ]




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