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Lorentz rule

This semi-empirical rule tries to account for the influence of differences in size and in ionization potential on the intermolecular potential of the unlike interactions although, as Douslin et aL point out, CF4 and CH4 possess similar ionization potentials and so this is not a significant factor for this particular fluorocarbon -f hydrocarbon pair. The use of equation (6) nevertheless leads to a considerable improvement between the theoretical and experimental values of rPa but there is still an unaccounted weakness in the unlike interactions. The reality of this weakness is further emphasized by the fact that the experimental value of F 2 is 2% larger than the value predicted by the Lorentz rule. [Pg.151]

The first of these relations is the Berthelot rule, and the second is the Lorentz rule. Combining rules are also required for other parameters in the chosen model. For example, the range parameter 2i2 in the unlike hard-core-square-well potential might be estimated as an arithmetic mean of 2n and (Table 3.3)... [Pg.47]

Lorentz-Invariance on a Lattice One of the most obvious shortcomings of a CA-based microphysics has to do with the lack of conventional symmetries. A lattice, by definition, has preferred directions and so is structurally anisotropic. How can we hope to generate symmetries where none fundamentally exist A strong hint comes from our discussion of lattice gases in chapter 9, where we saw that symmetries that do not exist on the microscopic lattice level often emerge on the macroscopic dyneimical level. For example, an appropriate set of microscopic LG rules can spawn circular wavefronts on anisotropic lattices. [Pg.669]

It is easy to invent rules that conserve particle number, energy, momentum and so on, and to smooth out the apparent lack of structural symmetry (although we have cheated a little in our example of a random walk because the circular symmetry in this case is really a statistical phenomenon and not a reflection of the individual particle motion). The more interesting question is whether relativistically correct (i.e. Lorentz invariant) behavior can also be made to emerge on a Cartesian lattice. Toffoli ([toff89], [toffSOb]) showed that this is possible. [Pg.669]

Each side of this rule can be completed to form a Lorentz four-vector by including the following equation ... [Pg.439]

The choice of appropriate potential parameters to use in the study of a certain mixture can be a significant problem. Traditionally the Lorentz Berthelot rules. [Pg.104]

X = 0.5 or so. Such corrections are commonly found in many other applications of the Lorentz-Berthelot mixing rules. [Pg.107]

Fig. 4.17. The Right Hand Rule (I thumb, B index finger, Fl middle finger) to determine the direction of the Lorentz Force (a) the current corresponds to the direction where positive charges move, i.e., the figure directly applies for positive ions, (b) A real magnet yoke without coils and flight tube. With kind permission of Thermo Electron (Bremen) GmbH, (left) and Waters Corporation, MS Technologies, Manchester, UK (right). Fig. 4.17. The Right Hand Rule (I thumb, B index finger, Fl middle finger) to determine the direction of the Lorentz Force (a) the current corresponds to the direction where positive charges move, i.e., the figure directly applies for positive ions, (b) A real magnet yoke without coils and flight tube. With kind permission of Thermo Electron (Bremen) GmbH, (left) and Waters Corporation, MS Technologies, Manchester, UK (right).
One of the main results obtained by Fajans and Joos was the replacement of the old additivity rule for the molar Lorenz-Lorentz refractivity, R, by the following principle R of a given electronic system of an ion, molecule or solvent decreases in the field of adjacent positively charged particles and increases in that of negative particles, i.e. the electronic system becomes tightened in the first case, loosened in the second case. This priciple found innumerable confirmations in a long series of refracto-metric investigations and led to the conclusion that deviations of Rl, l. [Pg.94]

The values of ev and ay are the well depth and size parameters, respectively, for the two interacting atoms i and j. In the case that one of the interacting atoms is a zeolite atom and the other is a sorbate atom, the cross terms ezeo-sorb and o-zeo-Sorb are determined from the Lorentz-Berthelot combination rules (7). When polarization interactions are accounted for, such as those between adsorbates and zeolite extra framework cations, Eq. (2) is written in the form... [Pg.8]

This equation can be deduced from the general Laplace formula that expresses the force exerted on a conductor of length dl, through which a current / passes, in a magnetic field of intensity B. The orientation of the Lorentz force (F = I dl AB) can be found by different approaches such as the right-handed three-finger rule or using the orientations of a direct trihedron. [Pg.293]

For most sets of i-j pairs, the Lorentz-Berthelot combining rules are used. (The only exception being when one molecule is nonpolar and the other is polar that case is also considered below.) The collision diameter Oij is usually estimated from the collision diameter of each molecule through the simple Lorentz-Berthelot combining rule as... [Pg.499]

An additional complication is introduced for the special case that one of the molecules (e.g molecule i) is nonpolar and the other molecule (j) is polar. In this case the simple Lorentz-Berthelot combining rules are modified as follows ... [Pg.500]

This is also the relation obtained in the hypothetical rest frame. Therefore, the B cyclic theorem is Lorentz-invariant in the sense that it is the same in the rest frame and in the light-like condition. This result can be checked by applying the Lorentz transformation rules for magnetic fields term by term [44], The equivalent of the B cyclic theorem in the particle interpretation is a Lorentz-invariant construct for spin angular momentum ... [Pg.140]

The free subindices notation was introduced by Einstein and Lorentz and is commonly called the Einstein notation. This notation is a useful way to collapse the information when dealing with equations in cartesian coordinates, and it is equivalent to subindices used when writing computer code. The Einstein notation has some basic rules that are as follows,... [Pg.645]

It is surprising that the mole refraction of the latter two compounds is not in agreement with the rules of Eisenlohr and Lorenz-Lorentz. No explanation has so far been given for the difference between experimental data and the theory. The Si—Si bond has not been found to have an abnormal increment. [Pg.88]

The Lorentz force encompasses the Lenz75 "right-hand rule" between v, B, and F and also explains how cyclotrons and mass spectrometers work. Practical applications of the Lorentz force are (i) the cyclotron (Problem 2.7.1) with its cyclotron frequency ... [Pg.54]


See other pages where Lorentz rule is mentioned: [Pg.104]    [Pg.89]    [Pg.212]    [Pg.104]    [Pg.89]    [Pg.212]    [Pg.347]    [Pg.228]    [Pg.486]    [Pg.787]    [Pg.666]    [Pg.672]    [Pg.498]    [Pg.562]    [Pg.674]    [Pg.121]    [Pg.232]    [Pg.189]    [Pg.40]    [Pg.165]    [Pg.92]    [Pg.246]    [Pg.713]    [Pg.54]    [Pg.407]    [Pg.336]    [Pg.164]    [Pg.375]    [Pg.497]   
See also in sourсe #XX -- [ Pg.47 , Pg.92 ]




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Lorentz

Lorentz Berthelot rule

Lorentz-Berthelot combination rules

Lorentz-Berthelot combining rules

Lorentz-Berthelot mixing rules

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