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T-adapted

Fig. 4-4 The age frequency function j/ x) and the residence time frequency function 4> x) and the corresponding average values and r, for the three cases described in the text (a) ta > t, (b) la = xy, (c) ta > t,. (Adapted from Bolin and Rodhe (1973) with permission from the Swedish Geophysical Society.)... Fig. 4-4 The age frequency function j/ x) and the residence time frequency function 4> x) and the corresponding average values and r, for the three cases described in the text (a) ta > t, (b) la = xy, (c) ta > t,. (Adapted from Bolin and Rodhe (1973) with permission from the Swedish Geophysical Society.)...
Fig. 9 Purification of ELPs by ITC is based on the reversible inverse phase transition. Le/i Protein purification via direct ELP fusions. A soluble ELP fused to a target protein becomes reversibly insoluble upon increasing temperature above 7,. Center Protein purification via ELP coaggregation. An excess of free ELPs enhances the aggregation of trace quantities of ELP-fusions. Right Purification via ELP-mediated affinity capture (EMAC). ELPs are fused to capture proteins, which bind specifically and reversibly to a target protein. This target protein can then be aggregated at temperatures above the T,. Adapted from [38] with permission from Elsevier, copyright 2010... Fig. 9 Purification of ELPs by ITC is based on the reversible inverse phase transition. Le/i Protein purification via direct ELP fusions. A soluble ELP fused to a target protein becomes reversibly insoluble upon increasing temperature above 7,. Center Protein purification via ELP coaggregation. An excess of free ELPs enhances the aggregation of trace quantities of ELP-fusions. Right Purification via ELP-mediated affinity capture (EMAC). ELPs are fused to capture proteins, which bind specifically and reversibly to a target protein. This target protein can then be aggregated at temperatures above the T,. Adapted from [38] with permission from Elsevier, copyright 2010...
Gjessing, D.T., Adaptive techniques for radar detection and identification of objects in an ocean environment , IEEE J. Ocean Engineering, Vol.6, No.l, pp 5-17, 1981. [Pg.186]

TO explain why people s behavior is adapted to their circumstances, one might argue that people who don t adapt don t survive. Selection of the best, rather than rational choice, is what ensures a tight fit between behavior and the demands of the environment. These two mechanisms differ in a number of ways. [Pg.79]

Fig. 2.12 Conductivity of undoped BaTi03 as a function of p0l and T (adapted from Smyth... Fig. 2.12 Conductivity of undoped BaTi03 as a function of p0l and T (adapted from Smyth...
Fig. 20. Experimental setup for applications of the SPECIFIC CP experiment in the context of triple-resonance solid-state NMR experiments. After an initial broadband adiabatic CP step from protons to the I nuclei, SPECIFIC transfer to the observed 5 nucleus occurs during the mixing time tm. The resulting signal represents a dipolar and chemical shift-filtered spectrum and can be controlled by variation of the carrier frequencies and the radiofrequency during the SPECIFIC transfer. A conventional HETCOR experiment is obtained by the introduction of an evolution time t. (Adapted from Baldus et al.215 with permission.)... Fig. 20. Experimental setup for applications of the SPECIFIC CP experiment in the context of triple-resonance solid-state NMR experiments. After an initial broadband adiabatic CP step from protons to the I nuclei, SPECIFIC transfer to the observed 5 nucleus occurs during the mixing time tm. The resulting signal represents a dipolar and chemical shift-filtered spectrum and can be controlled by variation of the carrier frequencies and the radiofrequency during the SPECIFIC transfer. A conventional HETCOR experiment is obtained by the introduction of an evolution time t. (Adapted from Baldus et al.215 with permission.)...
AT T Adapter Cable for Units with Special AT T Video Adapter... [Pg.119]

The Model 480C is fully compatible with IBM PS/2, PC, XT, and AT computer systems, Macintosh D and Mac LC systems, AT T/Olivetti systems, and Apple D systems and DEC VT220 terminals. If the AT T or Olivetti computer has a standard VGA output the Y cable included with Model 480C can be used. However, if they have an AT T display adapter board, then Dukane s accessory AT T adapter cable will be needed. [Pg.120]

If a Firestone valve (Ace Glass Inc., Vineland NJ) is not available, a bubbler connected to the N2 inlet tube via a T-adapter is sufficient. [Pg.272]

Guay M. and Zang T., Adaptive extremum seeking control of nonlinear dynamic systems with parametric uncertainty , Automatica 39 1283-1294, 2003. [Pg.16]

Fig. 6.25. Yield of CO2 as a function of catalyst temperature in the oxidation of trimethylamine over single- and multi-component noble metal catalysts. (A) 2 atm.% Ir/La203 ( ) 2 atm.% Pt/Sn02 ( ) 2 atm.% Au/Fe203 (O) 2 atm.% Au/Fe203-2 atm.% Ir/La203 ( ) mechanical mixture of 2wt% Pt/Sn02 and 2wt% Ir/La203 reactant gas, trimethylamine 100ppm in air SV = 10, OOOmlgJ t (adapted from [516])... Fig. 6.25. Yield of CO2 as a function of catalyst temperature in the oxidation of trimethylamine over single- and multi-component noble metal catalysts. (A) 2 atm.% Ir/La203 ( ) 2 atm.% Pt/Sn02 ( ) 2 atm.% Au/Fe203 (O) 2 atm.% Au/Fe203-2 atm.% Ir/La203 ( ) mechanical mixture of 2wt% Pt/Sn02 and 2wt% Ir/La203 reactant gas, trimethylamine 100ppm in air SV = 10, OOOmlgJ t (adapted from [516])...
Figure 10.2 Normalized gas-solid virial coefficients for a Lennard-Jones potential, as a function of the reduced temperature T/T, for different values of the correlation length Tq and for a given value of the standard deviation of the adsorptive potential kg T,. Adapted from Ref. 25. Figure 10.2 Normalized gas-solid virial coefficients for a Lennard-Jones potential, as a function of the reduced temperature T/T, for different values of the correlation length Tq and for a given value of the standard deviation of the adsorptive potential kg T,. Adapted from Ref. 25.
Figure 3.6. Non-reversing heat flow and change in heat capacity (C ) during cure of an epoxy resin cured with an anhydride at 80 °C. The cure time needed to reach a halving of Cp is marked as t. Adapted from Van Assche et al. (1997). Figure 3.6. Non-reversing heat flow and change in heat capacity (C ) during cure of an epoxy resin cured with an anhydride at 80 °C. The cure time needed to reach a halving of Cp is marked as t. Adapted from Van Assche et al. (1997).
FIGURE 10.34 Values of the surface dilatational modulus ESD of solutions of decanoic acid at two concentrations (indicated) as a function of time scale t. (Adapted from E. H. Lucassen-Reynders. Anionic Surfactants. Surfactant Series Vol. 11. Marcel Dekker, New York, 1981, p. 201.)... [Pg.406]

Figure B2.5.2. Schematic relaxation kinetics in a T-jump experiment, c measures the progress of the reaction, for example the concentration of a reaction product as a function of time t (abscissa with a logarithmic time scale). The reaction starts at (q. (a) Simple relaxation kinetics with a single relaxation time, (b) Complex reaction mechanism with several relaxation times x-. The different relaxation times x. are given by the turning points of c as a function of ln(t). Adapted from [110]. Figure B2.5.2. Schematic relaxation kinetics in a T-jump experiment, c measures the progress of the reaction, for example the concentration of a reaction product as a function of time t (abscissa with a logarithmic time scale). The reaction starts at (q. (a) Simple relaxation kinetics with a single relaxation time, (b) Complex reaction mechanism with several relaxation times x-. The different relaxation times x. are given by the turning points of c as a function of ln(t). Adapted from [110].
After all volatile materials are condensed into trap I, stopcocks B and C are closed, and the cylinder and the pump are removed. By introducing dry nitrogen through stopcock C via a T-adapter, the traps are brought to atmospheric pressure. [Pg.20]

Rg. 2.16 The pulse sequence used to determine spectra under dipolar decoupling conditions. Note that only the envelope curve of the FID is shown, not the high-frequency oscillations within it. This is what is usually recorded Fourier analysis then yields the spectrum as frequency shifts from the irradiating frequency. For all pulse sequences, the recovery time Tr between repeated applications of the sequence must be long compared with T. (Adapted from Nuclear Magnetic Resonance in Solid Polymers by V. J. McBrierty and K. J. Packer. Cambridge University Press, 1993.)... [Pg.51]

FIGURE 4.5 Relative deviation of volume V t) from equilibrium Vi versus time for PVAc following temperature step sequences listed in Table 4.2. (Experiment 1 was a direct downstep from the initial, To, to the final temperature, T.) The abscissa is the time elapsed since the final step was made to T, whether from Tq or from T. (Adapted from Robertson et al. [1988] data from Kovacs [1963].)... [Pg.171]

Figure 8 Determination of optimum ratio of M/T (adapted from Ref 29). Figure 8 Determination of optimum ratio of M/T (adapted from Ref 29).

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See also in sourсe #XX -- [ Pg.117 ]




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