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Shape from physical constants

In this approach no assumption is made about pore structure or particle size or shape. The model is also more advanced than that described above, in that flow at higher Reynolds numbers is taken into account, which allows taking Ccire of fluid circulation within the pores between the particles. Dissipation resulting from hysteresis-induced meniscus expansion or contraction is cdso incorporated. All of this leads to cui extension of d Arcy s law (sec. I.6.4f). The resulting equations contain a number of physical constants, the interpretation of which in terms of the microscopic geometry of the medium is not direct. Nevertheless, theories such as this one provide useful scale laws. [Pg.648]

The physical properties of the micelle, e.g. average aggregation number, shape and formation constant, can be deduced from the chemical-shift data from the mass action model.48 Using the mass action law model for micelle formation, the... [Pg.154]

Looking in on these physics equations as a chemist, 1 am surprised in two different ways. First, the number of fundamental physical constants needed is surprisingly small. For example, the night sky still echoes with light from the Big Bang. The shape of this light can be described with just six numbers. In 2015, four years of data from the Planck satellite were processed and released, and only minor tweaks to those six numbers were needed to explain all that data. Those six numbers work very, very well. [Pg.49]

Ultrasonic Microhardness. A new microhardness test using ultrasonic vibrations has been developed and offers some advantages over conventional microhardness tests that rely on physical measurement of the remaining indentation size (6). The ultrasonic method uses the DPH diamond indenter under a constant load of 7.8 N (800 gf) or less. The hardness number is derived from a comparison of the natural frequency of the diamond indenter when free or loaded. Knowledge of the modulus of elasticity of the material under test and a smooth surface finish is required. The technique is fast and direct-reading, making it useful for production testing of similarly shaped parts. [Pg.466]

The second axiom, which is reminiscent of Mach s principle, also contains the seeds of Leibniz s Monads [reschQl]. All is process. That is to say, there is no thing in the universe. Things, objects, entities, are abstractions of what is relatively constant from a process of movement and transformation. They are like the shapes that children like to see in the clouds. The Einstein-Podolsky-Rosen correlations (see section 12.7.1) remind us that what we empirically accept as fundamental particles - electrons, atoms, molecules, etc. - actually never exist in total isolation. Moreover, recalling von Neumann s uniqueness theorem for canonical commutation relations (which asserts that for locally compact phase spaces all Hilbert-space representations of the canonical commutation relations are physically equivalent), we note that for systems with non-locally-compact phase spaces, the uniqueness theorem fails, and therefore there must be infinitely many physically inequivalent and... [Pg.699]

Equation (17) indicates that the entire distribution may be determined if one parameter, av, is known as a function of the physical properties of the system and the operating variables. It is constant for a particular system under constant operating conditions. This equation has been checked in a batch system of hydrosols coagulating in Brownian motion, where a changes with time due to coalescence and breakup of particles, and in a liquid-liquid dispersion, in which av is not a function of time (B4, G5). The agreement in both cases is good. The deviation in Fig. 2 probably results from the distortion of the bubbles from spherical shape and a departure from random collisions, coalescence, and breakup of bubbles. [Pg.310]

Thus, from the second point, even if the physical properties of a seal material remained totally constant during the service life, the stiffness characteristics of the seal would alter because the shape factor changes—see Figure 23.1. [Pg.628]

The subscript in vessel is for the reactor or building. The subscript experimental applies to data determined in the laboratory using either the vapor or dust explosion apparatus. Equation 6-20 allows the experimental results from the dust and vapor explosion apparatus to be applied to determining the explosive behavior of materials in buildings and process vessels. This is discussed in more detail in chapter 9. The constants KG and KSt are not physical properties of the material because they are dependent on (1) the composition of the mixture, (2) the mixing within the vessel, (3) the shape of the reaction vessel, and (4) the energy of the ignition source. It is therefore necessary to run the experiments as close as possible to the actual conditions under consideration. [Pg.262]

It may seem from the above discussion that it is impossible to use even batch isotherm measurements to design HPLC (or SPE) separations. This is not so, however, at least when the HPLC separation occurs under near-equilibrium conditions. Nonlinear chromatographic peaks can be simulated [38] once the corresponding isotherms have been measured. In this case one does not need a physical interpretation of the isotherm equation s constants they can be regarded merely as interpolation factors. Separately measured isotherms of the two compounds are satisfactory in many cases because - as mentioned above - competition often has only minor influence on the separated peaks position and shape. [Pg.276]


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