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Rows

Figure 2 shows a typical example of the row data measured by this method The data exhibit a classic curves, namely velocity, contact force and depth of the indenter intrusion, obtained on polyvinyl chloride sample. [Pg.241]

The first equation (1) is the equation of state and the second equation (2) is derived from the measurement process. Finally, G5 (r,r ) is a row-vector that takes the three components of the anomalous ciurent density vector Je (r) = normal component of the induced magnetic field. This system is non hnear (bilinear) because the product of the two unknowns /(r) and E(r) is present. [Pg.328]

By means of a suitable software it is quite possible to qualify each drilling. At first a geometry check examines whether the drillings are present and in that case if they are positioned correctly. Furthermore each hole is examined whether the reached temperature level lies within a given threshhold. A typical error is shown in illustration 7. In both filmcooling rows locked holes are to be recognized. [Pg.404]

The scan area is recognized as a sequence of points set out in rows and columns and detected in a raster-like marmer under adjustable computer control [3]. [Pg.410]

The wall thickness estimation in tangential projection technique is based on the evaluation of profile plots along the pipe diameter as shown in fig. 1 (lowest row). [Pg.519]

Measure Wall Thickness This window is used for the dialog to calibrate the algorithm aceording formula (3) and for point wise measurements after calibration. The row Ideal indicates the nominal wall thickness used, IQI indicates the wall thickness values used for calibration and the detected optical density. Local can be used for noise reduction and compensation of geometric effects. [Pg.564]

The acquisition sequence is as follows a first acquisition calibration enables the acquisition operator to verify the data before storage. The row data, together with calibration files are transferred to the analysis program. The program transforms the row data into calibrated data, which is then analysed. [Pg.1008]

Near drum wastage is the most prevalent type of wastage documented. It cart be found anywhere in the generating bank but is most common on the wall tubes, in tlic row immediately next to soot blower lanes and in the hot and cold row s. Three types of near drum w astagc have been documented. [Pg.1036]

As usual, things become more complicated when studied in detail. Note that for 0/W(l 10) 0 varies with 6 the situation is shown more fully in Fig. XVIII-15. The authors speculate that variations in Dq and E have to do with a p(2 x 1) structure at low oxygen coverage, with O atoms occupying alternate rows of W atoms, the empty rows becoming occupied above 0 = 0.5. The consequence is that O—O interactions shift from being mostly attractive to being in part repulsive. [Pg.711]

Perhaps the most fascinating detail is the surface reconstruction that occurs with CO adsorption (see Refs. 311 and 312 for more general discussions of chemisorption-induced reconstructions of metal surfaces). As shown in Fig. XVI-8, for example, the Pt(lOO) bare surface reconstructs itself to a hexagonal pattern, but on CO adsorption this reconstruction is lifted [306] CO adsorption on Pd( 110) reconstructs the surface to a missing-row pattern [309]. These reconstructions are reversible and as a result, oscillatory behavior can be observed. Returning to the Pt(lOO) case, as CO is adsorbed patches of the simple 1 x 1 structure (the structure of an undistorted (100) face) form. Oxygen adsorbs on any bare 1 x 1 spots, reacts with adjacent CO to remove it as CO2, and at a certain point, the surface reverts to toe hexagonal stmcture. The presumed sequence of events is shown in Fig. XVIII-28. [Pg.737]

Each entry is the product of first applying the permutation at the top of the column and then applying the permutation at the left end of the row. [Pg.144]

Griffiths D 1987 Introduction to Elementary Particles (New York Flarper and Row)... [Pg.183]

Figure A3.10.10 STM image (55 x 55 mn ) of a Si(lOO) surface exposed to molecular bromine at 800 K. The dark areas are etch pits on the terraces, while the bright rows that run perpendicular to the terraces are Si dimer chains. The dimer chains consist of Si atoms released from terraces and step edges during etching [28],... Figure A3.10.10 STM image (55 x 55 mn ) of a Si(lOO) surface exposed to molecular bromine at 800 K. The dark areas are etch pits on the terraces, while the bright rows that run perpendicular to the terraces are Si dimer chains. The dimer chains consist of Si atoms released from terraces and step edges during etching [28],...
Figure A3.10.14 STM image of 0.25 ML Aii vapour-deposited onto Ti02(l 10). Atomie resolution of the substrate is visible as parallel rows. The Au elusters are seen to nueleate preferentially at step edges. Figure A3.10.14 STM image of 0.25 ML Aii vapour-deposited onto Ti02(l 10). Atomie resolution of the substrate is visible as parallel rows. The Au elusters are seen to nueleate preferentially at step edges.
Kuppermann A 1997 Reactive scattering with row-orthonormal hyperspherical coordinates. 2. [Pg.1003]


See other pages where Rows is mentioned: [Pg.151]    [Pg.222]    [Pg.348]    [Pg.429]    [Pg.167]    [Pg.1029]    [Pg.1036]    [Pg.1038]    [Pg.276]    [Pg.304]    [Pg.460]    [Pg.460]    [Pg.460]    [Pg.489]    [Pg.603]    [Pg.32]    [Pg.41]    [Pg.90]    [Pg.159]    [Pg.161]    [Pg.292]    [Pg.299]    [Pg.566]    [Pg.690]    [Pg.825]    [Pg.926]    [Pg.927]    [Pg.935]    [Pg.936]    [Pg.950]    [Pg.1038]    [Pg.1075]   
See also in sourсe #XX -- [ Pg.582 ]




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