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Location correspondence

That means, the input signal u( ) is applied on =0. The output signal y(x) is than given by fthat means by a shifted and scaled version of g(x ). So, the output signal y(x ) at a special location corresponds to the addition of the terms u( )g(x - ) over alt [2,3]. [Pg.367]

Q (4) Represent amplitude and steepness of the arriving surge at different locations corresponding to curves of Figure 17.21. [Pg.582]

On lines 6.2.1 through 6.2.3, report the amount of the chemical transferred to other off-site locations corresponding to those listed in Part II, Sections 2.1 through 2.6, including privately owned wastewater treatment facilities. In the block provided, enterthe numberfrom Part II, Section 2 corresponding to the off-site location to which the transfer is sent For example, if the transfer is sent to the location listed in Part II, Section 2 3. enter 3" in the block provided. (The first digit of this section number has been precoded.) If you need additional space, check the box at the bottom of Section 6 and use the Supplemental Information Sheet (Part IV, Section 6) to report those transfers. [Pg.46]

Notional-particle locations correspond to the grid cells used in the FV code. [Pg.358]

In another study, samples from the Dutch coastal zone of the North Sea were collected in 1999 and 2000 and analysed by LC-ESI-MS [31]. At locations corresponding to those of the 1995/1999 studies, levels (10-30ngNPEOg 1) were observed in close agreement with the ones reported earlier. It can be concluded that, provided careful evaluation of which commercial mixture will be used as a calibrant in LC-FL, the result thus calculated can be similar to those obtained by LC-MS. [Pg.520]

Both practical combustors had pilot streams carr 4ng a fuel-air mixture richer than that of the main flow. These could also serve as a convenient location for the addition of oscillations to the fuel flow to control naturally occurring oscillations. Oscillation of fuel in the main flow will be more effective if it is applied close to the entry to the burner. Hence the present study examined the possibility of control by oscillation of fuel at locations corresponding to both portions of the combustor in-flow. [Pg.296]

The biodistribution of intravenously injected allogeneic MSCs has been recently described [131]. Oxine-labeled MSCs were injected intravenously 72 h after occlusion/reperfusion in seven dogs. Initially, cells were trapped in the lungs within 24 h after injection, they had been redistributed into the liver and spleen. Focal uptake and persistence of the stem cells was observed in a mid anterior wall location corresponding to the infarcted target area. [Pg.111]

Because the Patterson function contains no phases, it can be computed from any raw set of crystallographic data, but what does it tell us A contour map of p(x,y,z) displays areas of high density (peaks) at the locations of atoms. In contrast, a Patterson map, which is a contour map of P(u,v,w), displays peaks at locations corresponding to vectors between atoms. (This is a strange idea at first, but the following example will make it clearer.) Of course, there are more vectors between atoms than there are atoms, so a Patterson map is more complicated than an electron-density map. But if the structure is simple, like that of one or a few heavy atoms in the unit cell, the Patterson map may be simple enough to allow us to locate the atom(s). You can see now that the... [Pg.115]

For the orientation search (often called a rotation search), the computer is looking for large values of the model Patterson function Pmodel( ,v,w) at locations corresponding to peaks in the Patterson map of the desired protein. A powerful and sensitive way to evaluate the model Patterson is to compute the minimum value of Pmodel(w,v,w) at all locations of peaks in the Patterson map of the desired protein. A value of zero for this minimum means that the trial orientation has no peak in at least one location where the desired protein exhibits a peak. A high value for this minimum means that the trial orientation has peaks at all locations of peaks in the Patterson map of the desired protein. [Pg.131]

Auger electron spectroscopy (AES) is particularly suited for surface analysis (depth 0.5-1 nm). AES depth profile analysis was employed to determine the thickness and composition of surface reaction layers formed under test conditions in the Reichert wear apparatus in the presence of four different ZDDPs additives at different applied loads (Schumacher et al., 1980). Using elemental sensitivity factors the concentration of the four elements (S, P, O, C) was determined at three locations corresponding to a depth of 1.8, 4.3, and 17 nm. No significant correlation between wear behavior and carbon or oxygen content of the reaction layer was observed. A steady state sulfur concentration is reached after a very short friction path. Contrary to the behavior of sulfur, phosphorus concentration in the presence of ZDDPs increases steadily with friction path, and no plateau value is reached. [Pg.157]

Figure 3. Model showing how a protein conformational change altering the conductances in access channels may allow the electric field to move past the bound ion (closed circle), which remains stationary. In either conformation the electrical potential gradient is located corresponding to a narrow access channel of low conductance. /(x) indicates electrical potential. Figure 3. Model showing how a protein conformational change altering the conductances in access channels may allow the electric field to move past the bound ion (closed circle), which remains stationary. In either conformation the electrical potential gradient is located corresponding to a narrow access channel of low conductance. /(x) indicates electrical potential.
The graph in Figure 18.19 shows the development of an initially normal distribution of molecules by recombination. As x increases, peaks appear in the distribution at locations corresponding to multiples of the initial average degree of polymerization. [Pg.502]

In Fig. 4.6 we have plotted a typical heat generation expression (curve a) along with the heat removal line, b. In this case the two curves intersect at three locations corresponding to three different reactor conditions that are possible for the same operating parameters and feed conditions. The low-temperature steady state is uneconomical since the feeds are virtually unconverted. The highest-temperature steady state has nearly complete conversion but may be too hot. Under those conditions side reactions may set in or the reactor pressure becomes too high. The middle steady state strikes a good compromise and is where... [Pg.90]


See other pages where Location correspondence is mentioned: [Pg.382]    [Pg.111]    [Pg.126]    [Pg.137]    [Pg.202]    [Pg.684]    [Pg.905]    [Pg.453]    [Pg.341]    [Pg.113]    [Pg.523]    [Pg.770]    [Pg.314]    [Pg.280]    [Pg.244]    [Pg.327]    [Pg.564]    [Pg.68]    [Pg.63]    [Pg.348]    [Pg.354]    [Pg.32]    [Pg.33]    [Pg.7]    [Pg.47]    [Pg.12]    [Pg.940]    [Pg.44]    [Pg.412]    [Pg.583]    [Pg.853]    [Pg.77]    [Pg.39]    [Pg.224]    [Pg.132]    [Pg.382]   
See also in sourсe #XX -- [ Pg.145 ]




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