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Particle model experience

How does yield stress depend on the size of particles We have mentioned above that increasing the specific surface, i.e. decreasing an average size of particles of one type, causes an increase in yield stress. This fact was observed in many works (for example [14-16]). Clear model experiments the purpose of which was to reveal the role of a particle s size were carried out in work [8], By an example of suspensions of spherical particles in polystyrene melt it was shown that yield stress of equiconcentrated dispersions may change by a hundred of times according to the diameter d of non-... [Pg.80]

You can appreciate why scientists were puzzled The results of some experiments (the photoelectric effect) compelled them to the view that electromagnetic radiation is particlelike. The results of other experiments (diffraction) compelled them equally firmly to the view that electromagnetic radiation is wavelike. Thus we are brought to the heart of modern physics. Experiments oblige us to accept the wave-particle duality of electromagnetic radiation, in which the concepts of waves and particles blend together. In the wave model, the intensity of the radiation is proportional to the square of the amplitude of the wave. In the particle model, intensity is proportional to the number of photons present at each instant. [Pg.138]

At the time that J. J. Thomson conducted his experiments on cathode rays, the nature of the electron was in doubt. Some considered it to be a form of radiation, like light others believed the electron to be a particle. Some of the observations made on cathode rays were used to advance one view or the other. Explain how each of the following properties of cathode rays supports either the wave or the particle model... [Pg.174]

One of the important elements of the Model of Modelling framework is the consideration of the snbject s previous ideas as one of the experiences needed to support the proposition of the mental model. In this teaching situation, students previous ideas, mainly those related to the kinetic particle model, were essential to the inclusion of fundamental attributes in their models (e.g., the dynamicity of the chemical transformation). [Pg.298]

Summing up this section, we would like to note that understanding size effects in electrocatalysis requires the application of appropriate model systems that on the one hand represent the intrinsic properties of supported metal nanoparticles, such as small size and interaction with their support, and on the other allow straightforward separation between kinetic, ohmic, and mass transport (internal and external) losses and control of readsorption effects. This requirement is met, for example, by metal particles and nanoparticle arrays on flat nonporous supports. Their investigation allows unambiguous access to reaction kinetics and control of catalyst structure. However, in order to understand how catalysts will behave in the fuel cell environment, these studies must be complemented with GDE and MEA tests to account for the presence of aqueous electrolyte in model experiments. [Pg.526]

The computation performed in this study is based on the model equations developed in this study as presented in Sections II.A, III.A, III.B, and III.C These equations are incorporated into a 3-D hydrodynamic solver, CFDLIB, developed by the Los Alamos National Laboratory (Kashiwa et al., 1994). In what follows, simple cases including a single air bubble rising in water, and bubble formation from a single nozzle in bubble columns are first simulated. To verify the accuracy of the model, experiments are also conducted for these cases and the experimental results are compared with the simulation results. Simulations are performed to account for the bubble-rise phenomena in liquid solid suspensions with single nozzles. Finally, the interactive behavior between bubbles and solid particles is examined. The bubble formation and rise from multiple nozzles is simulated, and the limitation of the applicability of the models is discussed. [Pg.16]

Bokkers, G. A., Van Sint Annaland, M., and Kuipers, J. A. M., Comparison of continuum models using kinetic theory of granular flow with discrete particle models and experiments extent of particle mixing induced by bubbles. Proceedings of Fluidization XI, May 9-14, 2004, 187-194, Naples, Italy (2004). [Pg.146]

In Figure 5.23 the velocity of the fluid relative to the particle, as calculated for the model experiments and from equation 5.100, is plotted against voidage. It may be seen that reasonable agreement is obtained at voidages between 0.45 and 0.90, indicating that the model does fairly closely represent the conditions in a suspension. [Pg.281]

The planetary model of the atom was proposed by Rutherford in 1912 following the a particle scattering experiments of Geiger and Marsden, which showed most the mass of an atom to be concentrated in a tiny positive nucleus. The orbiting of light electrons resembles the problem of planetary motion first solved by Newton. [Pg.58]

The most perceptible experimental reason is the evident asymmetry of the Universe. The CP violation alone, on the level allowed by the Standard model, is not sufficient to explain the excess of matter in the Universe [18]. Finding a suitable extension of the Standard Model is not easy not only do the GUT theories tend to violate CPT invariance but they are also difficult to test. Specifically they can not be tested by means of the particle accelerator experiments, which so far have been very successful in extending our knowledge of Physics. This is because the GUT energy is some 1013 times larger than what we can now days produce in the most powerful accelerators. Consequently we must look for the low-energy manifestations of GUT and CPT invariance. Interestingly some possibilities for such tests lie within the realm of atomic and molecular physics. [Pg.191]

A classical dynamics model has been developed to Investigate the Importance of colllslonal processes In heavy particle bombardment experiments. This procedure Is very powerful for describing colllslonal events and provides a working hypothesis against which experimental data can be compared. He have shown numerous examples from SIMS experiments where the calculations have fit experimental data very well. The time has come for the experimentalists to conceive and execute experiments aimed at uncovering the fundamental processes Involved In the SIMS and FABMS procedures. [Pg.53]

The most common form of TOT clathrate crystallises as discrete C2 symmetric cavities in the chiral space group 1, implying that the (—)-(M) and (+)-(/") forms separate spontaneously as crystallisation occurs. This property of TOT has been used in an ambitious model experiment designed to test the theory that the parity-violating energy difference (the violation of parity or symmetry in elementary particles), with autocatalytic amplification (in the case of TOT during crystallisation) is responsible for the observed chirality of modern biomolecules. The experiment did not find any evidence to support the theory, with equal amounts of each enantiomeric crystal being isolated.26... [Pg.445]

Viscometric particle swelling experiments were carried out with a Cannon-Ubbelohde shear-dilution viscometer thermostated at 30 + 0.05°C. The shear rate was approximately 2000 sec-1 with flow times determined to + 0.1 sec. As in the sedimentation method, the model latexes were diluted with distilled water to a concentration of approximately 1 percent. Individual samples were adjusted with sodium hydroxide to various pH values and allowed to equilibrate at least 24 hours before measuring the viscosity. [Pg.266]

For the two-slit experiment, according to standard QM, strict completion of Eq. (7) would make impossible to determine which hole the electron or photon passes through without, at the same time, disturbing the electrons or photons enough to destroy the interference pattern. This is a puzzling situation within the particle model. Somewhere, there is a missing link (see below). [Pg.59]

Consider Ernest Rutherford s alpha-particle bombardment experiment illustrated in Figure 2.11. How did the results of this experiment lead Rutherford away from the plum pudding model of the atom to propose the nuclear model of the atom ... [Pg.46]


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