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Chips geometry

The type of constitutive material law model strongly influences the flow stress in FE simula-ti(Mis and thereby the computed forces, temperatures, and chip geometries. Results from different workpiece materials AISI1045 and AISI52100 are compared in Fig. 6 (Denkena et al. 2006). [Pg.639]

However, these favorable properties also result in a challenging machinability, which is reflected by high tool wear rates, unfavorable chip geometries, and rough surface qualities. In order to design stable cutting operations, one has to consider the complex interaction of alloying elements, tool materials, and process parameters. [Pg.788]

Considering the original tool geometry, the model is able to calculate the undeformed chip geometry, the geometry and surface roughness of the machined workpiece, and the cutting forces. [Pg.890]

Illustration of undeformed chip geometry. (From Hwang, T.W. and Malkin, S., ASME J. Manuf. Sci. Eng., 121, 623. With permission.)... [Pg.74]

Direct current (DC) dielectrophoresis (DEP) is an efficient means to move and thus separate particles or cells with the force of a stationary electric field. This is accomplished with a spatially nonuniform electric field shaped around insulative objects as obstacles in the path of the DC field. DC-DEP is then the induced motion of polarizable, dielectric objects of micron and smaller size, in a DC electric field that is modified by lab-on-a-chip geometry (or other means) to be spatially nonuniform. [Pg.529]

An alternative version of extension occurs when the dimensions change in one direction and are constrained to be constant in the two mutually perpendicular directions. This is achieved by placing a thin flat sample, whose faces are bonded to rigid members, under tension or compression in the thin direction, colloquially termed poker chip geometry (Fig. 1-15), or by axial compression of a cylinder confined by a rigid cylindrical wall. Under these conditions, 722 = 7j3 = 0. If a sudden tensile strain e = 1 is accomplished and the stress relaxation is followed... [Pg.25]

A plasma etcher has a number of MVs that can be adjusted in order to achieve the desired chip geometry. By applying Guidelines 6 and 8, several input variables can be selected from the four possible MVs etch time. [Pg.248]

Thus, the difference in the output power for m-plane and -plane LED for drive currents in excess of 100 mA is owing to the difference in the operating temperature of the device. Higher temperature results in the decrease of radiative recombination efficiency, thereby resulting in the drop of the optical output power [35]. The efficiency of the nonpolar LED can be improved by adopting a flip-chip geometry. [Pg.351]

Because of the possibility of focusing laser beams, thin films can be produced at precisely defined locations. Using a microscope train of lenses to focus a laser beam makes possible the production of microregions suitable for application in computer chip production. The photolytic process produces islands of product nuclei, which act as preferential nucleation sites for further deposition, and thus to some unevenness in the product film. This is because the substrate is relatively cool, and therefore the surface mobility of the deposited atoms is low. In pyrolytic decomposition, the region over which deposition occurs depends on the thermal conductivity of the substrate, being wider the lower the thermal conductivity. For example, the surface area of a deposit of silicon on silicon is narrower than the deposition of silicon on silica, or on a surface-oxidized silicon sample, using the same beam geometry. [Pg.83]

We have shown that antiresonant dielectric layers can be used to design low-loss liquid-core waveguides that are suitable for implementing planar sensor device geometries. The following sections will describe in more detail how the design principles laid out here were implemented in silicon-based LC-ARROW chips and used for optical sensing and detection of a wide variety of substances. [Pg.494]

Fig. 18.9 Single molecule fluorescence detection in LC ARROW chip, (a) Top view of experi mental beam geometry of dye molecule in sub picoliter excitation volume (dotted ellipse) (2exc excitation beam, dF fluorescence signal) (b) fluorescence signal as function of molecules in excitation volume symbols, different experimental runs, dashed line linear fit... Fig. 18.9 Single molecule fluorescence detection in LC ARROW chip, (a) Top view of experi mental beam geometry of dye molecule in sub picoliter excitation volume (dotted ellipse) (2exc excitation beam, dF fluorescence signal) (b) fluorescence signal as function of molecules in excitation volume symbols, different experimental runs, dashed line linear fit...

See other pages where Chips geometry is mentioned: [Pg.119]    [Pg.122]    [Pg.122]    [Pg.423]    [Pg.484]    [Pg.257]    [Pg.1097]    [Pg.327]    [Pg.413]    [Pg.414]    [Pg.642]    [Pg.890]    [Pg.1294]    [Pg.787]    [Pg.27]    [Pg.512]    [Pg.119]    [Pg.122]    [Pg.122]    [Pg.423]    [Pg.484]    [Pg.257]    [Pg.1097]    [Pg.327]    [Pg.413]    [Pg.414]    [Pg.642]    [Pg.890]    [Pg.1294]    [Pg.787]    [Pg.27]    [Pg.512]    [Pg.344]    [Pg.345]    [Pg.116]    [Pg.194]    [Pg.195]    [Pg.207]    [Pg.207]    [Pg.210]    [Pg.211]    [Pg.215]    [Pg.220]    [Pg.328]    [Pg.126]    [Pg.374]    [Pg.243]    [Pg.67]    [Pg.106]    [Pg.266]    [Pg.130]    [Pg.247]    [Pg.247]    [Pg.508]   
See also in sourсe #XX -- [ Pg.512 , Pg.522 ]




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