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Dean numer

Venkatesh P K, Dean A M, Cohen M H and Carr R W 1999 Master equation analysis of intermolecular energy transfer in multiple-well, multiple-channel unimolecular reactions. II. Numerical methods and application to the mechanism of the C. + O2 reaction J. Chem. Phys. Ill 8313... [Pg.1085]

G<3odfeilow has presented numerous courses internationally in the dean air technology field, both for industrial clients and at conferences and icininars. and he has presented and/or published over iOO technical papers. [Pg.1550]

Born in Vienna, Austria, on May 3, 1895, Professor Herman Mark is as vital today as his almost innumerable contributions to polymer science. He continues to maintain an active schedule as a world traveler and lecturer at numerous national and international symposia and seminars. His home base, however, remains at Polytechnic Institute of New York, where he is Dean Emeritus and an emeritus member of the Board of Trustees. [Pg.5]

The point is now to estimate the maximum number of photons that can be detected from a burst. The maximum rate at which a molecule can emit is roughly the reciprocal of the excited-state lifetime. Therefore, the maximum number of photons emitted in a burst is approximately equal to the transit time divided by the excited-state lifetime. For a transit time of 1 ms and a lifetime of 1 ns, the maximum number is 106. However, photobleaching limits this number to about 105 photons for the most stable fluorescent molecules. The detection efficiency of specially designed optical systems with high numerical aperture being about 1%, we cannot expect to detect more than 1000 photons per burst. The background can be minimized by careful dean-up of the solvent and by using small excitation volumes ( 1 pL in hydrodynamically focused sample streams, 1 fL in confocal exdtation and detection with one- and two-photon excitation, and even smaller volumes with near-field excitation). [Pg.372]

The reason for constructing this rather complex model was that even though the mathematical equations may be easily set up using the dispersion model, the numerical solutions are quite involved and time consuming. Deans and Lapidus were actually concerned with the more complicated case of mass and heat dispersion with chemical reactions. For this case, the dispersion model yields a set of coupled nonlinear partial differential equations whose solution is quite formidable. The finite-stage model yields a set of differential-double-difference equations. These are ordinary differential equations, which are easier to solve than the partial differential equations of the dispersion model. The stirred-tank equations are of an initial-value type rather than the boundary-value type given by the dispersion model, and this fact also simplifies the numerical work. [Pg.156]

Membrane-deaning strategies are numerous and generally remain proprietary information. Physical deaning by relaxation or backwashing is used on a frequent basis but the efficiency tends to decrease with filtration time. As irreversible fouling accumulates on the surface, chemical cleanings of various intensities (i.e., cleaner concentration used) can be applied on a weekly to yearly basis [20]. [Pg.130]

Due to the difficulties of getting analytical solutions, many numerical methods were developed to simulate the solute transport and retention processes in the soil. Deane et al. (1999) analyzed the transport and fate of hydrophobic organic chemicals (HOCs) in consolidated sediments and saturated soils. Walter et al. (1994) developed a model for simulating transport of multiple thermodynamically reacting chemical substances in groundwater systems. Islam et al. (1999) presented a modeling... [Pg.63]

Moulin PH, Veyret D, and Charbit F, Dean vortices Comparison of numerical simulation of shear stress and improvement of mass transfer in membrane processes at low permeation fluxes, J. Membr. Sci. 2001 183 148-162. [Pg.229]

Deviations horn straight lines in Mott-Schottky plots are frequently attributed to the influence of potential dependent charging of surface or bulk states. While deviations can also be attributed to nonuniform dopant concentrations, this interpretation is supported by anal3ttic and numerical calculations of the contribution of defects to the space charge as a function of applied potential (see, e.g.. Dean and Stimming ° or Bonham and Orazem ). [Pg.361]

Financial support provided to one of us (M.A.M.) by Dean Otto W. Witzell and Professor Jack Keverian of Drexel University is gratefully acknowledged. Dean Richard E. Woodring has kindly provided us with computer time. Colleagues who have discussed this work are too numerous to name, but comments of all of them are appreciated. [Pg.396]

Brewster et Numerical solution (wide gap theory) Spiral tube Dean vortices in curved the tube were reported... [Pg.1537]

Chung et Finite volume method and nuclear magnetic resonance flow imaging technique Spiral tube Velocity and pressure fields in the curved tube have been reported numerically, and it has been observed that Dean vortices can successfully depolarize solute buildup and fouling... [Pg.1537]

Mallubhotla and Belfort MRI measurement and numerical technique Helical coils Velocity profiles and the dynamic behavior of Dean vortices in the curved tube flow were reported... [Pg.1537]

Chung, K.-Y. Edelstein, W.A. Li, X. Belfort, G. Dean vortices in a curved channel membrane system. 5. Three dimensional magnetic resonance imaging and numerical analysis of the velocity field in a curved impermeable tube. AIChE J. 1993, 39, 1592-1602. [Pg.1547]


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See also in sourсe #XX -- [ Pg.33 ]




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