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Fundamental equations of electrostatics

Unless otherwise stated, we follow here and elsewhere the electrostatic system of units. The electric field at position r associated with a distribution of point charges qt at positions r/ in vacuum is given by the Coulomb law [Pg.45]

Note that taking p to be a distribution of point charges, / ( ) = - u), [Pg.45]

Another expression of the Coulomb law is the Gauss law, which states that the electric field associated with a charge distribution p (r) satisfies the relationship [Pg.46]

212) Q denotes a voliune that is enclosed by the surface S, n is a unit vector at a surface element ds of S in the outward direction and is an integral over the surface [Pg.46]

The Gauss law (1.212) relates the surface-integrated field on the boundary of a volume to the total net charge inside the volume. Using the divergence theorem [Pg.46]


Notes on Three-dimensional Differential Calculus and the Fundamental Equations of Electrostatics... [Pg.180]

The electrostatic field in the stationary state is described by the Poisson-Boltzmann equation. The PB model constitutes the fundamental equation of electrostatics and is based on the differential Poisson equation which describes the electrostatic potential 4>(r) in a medium with a charge density p(r) and a dielectric scalar field e(r) ... [Pg.216]

Here c° is the bulk concentration of a z Z valent electrolyte. However, a fundamental equation of electrostatics (Poisson s equation) relates this density to the way in which ip varies with the distance from the surface ... [Pg.131]

The fundamental equation of electrostatics is Coulomb s law, which gives the electrostatic repulsive force between two point charges of like sign separated by a distance R ... [Pg.80]

There are two important problems with this equation. First, it is a non-linear differential equation because of the exponential terms in d> and therefore cannot be solved in a simple way. The second problem is that the solution of the statistical problem is not consistent with the fundamental laws of electrostatics. These problems were overcome by Debye and Hiickel [17] in a fairly simple way. In the case that the electrostatic energy is small in comparison to the thermal kinetic... [Pg.122]

This equation shows an additive relation between the potentials and therefore fits a fundamental principle of electrostatics the linear superposition of fields. [Pg.364]

In terms of the relationship between voltage V, across the plates of any capacitor and the stored charge density q per cm the capacitance, C, is given by the fundamental equation in electrostatics ... [Pg.472]

The Poisson equation is a fundamental relationship of classical electrostatics and really need not be proved here. However, since we are using it as a starting point, it seems desirable to explore the meaning of this important equation to some extent. [Pg.508]

The passage of electrons or other particles with charge q and mass m through an electrostatic lens system is governed by their motion under the action of the electric field. In the case considered here, cylindrical symmetry around the optical axis (z-axis) and paraxial rays will be assumed. Of the cylindrical coordinates only the transverse radial coordinate p and the distance coordinate z are of relevance, and the electrostatic potential of the lens is given by q>(p, z). As shown in Section 10.3.1, in the paraxial approximation the potential q>(p, z) is fully determined by the potential symmetry axis. Hence, the equations of motion and the fundamental differential equation of an electrostatic lens depend only on this potential. The fundamental lens equation is given by (see equ. (10.38))... [Pg.132]

We turn now to the more recently proposed two-state model of long-range interactions (Magnasco, 2004b). It is of interest in so far as it avoids completely explicit calculation of the matrix elements (Equations 4.12-4.17) occurring in RS perturbation theory, being based only on the fundamental principles of variation theorem and on a classical electrostatic approach. [Pg.157]

This may contradict one of the basic laws of electrostatics, that is the linear superposition of fields. This is a fundamental problem for the theory and to any other theory or development, such as that due to Guggenheim below (Section 10.13.1), which makes use of any such combination. In fact this is one of the big problems in the theory. The other big problem is that the x/tjS in the Poisson equation and in the Maxwell-Boltzmann distribution are different and have a different physical basis (see Section 10.6.5). This is believed by many to be yet another fundamental problem for the theory. [Pg.384]

Coulomb s Law tells us the force experienced by a pair of separated charges. It s a fundamental equation in the study of electrostatics, which is a broad area of physics concerned with the interactions between stationary charges. The equation for this force can be written ... [Pg.27]

Example 4.1 With the help of fundamental equations, show that to acquire a product-ion spectrum, it is necessary to keep ht B/E ratio constant during scanning of the magnetic and electrostatic fields. [Pg.131]

The most fundamental level of modeling of any chemical system employs quantum mechanics. Quantum mechanical (QM) treatments are required to understand many important chemical and biological properties of nucleic acids. Moreover, empirical force-field methods, employed to study the conformations of polynucleotides, rely on quantum calculations to obtain crucial parameters that are difficult to measure experimentally, such as atom-centered charges for calculating electrostatic interactions. The obtain a description of a chemical system using QM one solves the time-independent Schrodinger equation with or without the use of empirical parameters. [Pg.7]

The core of physics. Maxwell s equations are the heart of classical electro-dynamics because they completely model the electrostatic and electromagneto-K static duality together with dynamics, which works between the two domains. S L They rely on the fundamental properties of space-time and they are considered... [Pg.382]

From a more fundamental point of view, the PB equation is not consistent with Maxwell electrostatics (Spitzer 2003). [Pg.30]

Crystal field theory assumes that all M-L interactions are purely electrostatic in nature. More specifically, it considers the electrostatic effect of a field of ligands on the energies of a metals valence-shell orbitals. To discuss CFT, we need only be aware of two fundamental concepts (1) the coulombic theory of electrostatic interactions and (2) the shapes of the valence orbitals of transition metals—that is, the nd orbitals ( = 3 for the first row of transition metals, etc.). The first concept involves only the familiar ideas of the repulsion of like and the attraction of dislike electrical charges. Quantitatively, Coulomb s law states that the potential energy of two charges Qj and Q2 separated by a distance r is given by the formula shown in Equation (4.3) ... [Pg.60]

The flow pattern of the vortex motion of the gas in reverse-flow cyclone is quite complex. First, it is three-dimensional second, the flow is turbulent An exact analysis is therefore difficult Soo (1989) has summarized a fundamental analysis of velocity profiles and pressure drops in such a cyclone. He has also analyzed the governing particle diffusion equation in the presence of electrostatic, gravitational and centrifugal forces. He has then provided an analytical expression for partide collection efficiency under a number of limiting conditions. We wiU, however, opt here for a much simpler model of particle separation in a cyclone developed by Clift et id. (1991). This approach is based on a modification of the original model by Leith and Licht (1972). The model will be... [Pg.627]

The Born-Fajans-Haber cycle uses thermodynamic cycles to determine lattice energy. An alternative to the Born-Fajans-Haber method is one based on fundamental principles. Because the dominant interactions in an ionic crystal are Coulomb interactions, we can use the theory of electrostatics to calculate the lattice energy. Kapustinskii used these ideas and proposed the following equation ... [Pg.577]

Max Born introduced a theoretical approach to the estimation of absolute enthalpies of hydration of ions based on electrostatic theory. Equation (l. 2) is fundamental to electrostatic theory. It may be altered to ... [Pg.31]


See other pages where Fundamental equations of electrostatics is mentioned: [Pg.45]    [Pg.45]    [Pg.45]    [Pg.45]    [Pg.47]    [Pg.300]    [Pg.53]    [Pg.134]    [Pg.387]    [Pg.232]    [Pg.573]    [Pg.134]    [Pg.387]    [Pg.329]    [Pg.543]    [Pg.24]    [Pg.371]    [Pg.4]    [Pg.25]    [Pg.410]    [Pg.323]    [Pg.53]    [Pg.56]    [Pg.308]    [Pg.8]    [Pg.203]   


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