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Electric field strength vector

It is essential that plasmons are longitudinal electric waves, that is, that the electric field strength vector is parallel to the wave vector q. For a plane wave, the vector potential of electromagnetic field is... [Pg.278]

E = electric field strength vector H = magnetic field strength vector... [Pg.25]

Fig. 1 Setup for electrospinning aligned nanofibers using the (a) rotating mandrel, and the (b) parallel plate techniques, (c) Calculated electric field strength vectors and (d) electrostatic force (F) analysis associated with the parallel plate techniques [62]... Fig. 1 Setup for electrospinning aligned nanofibers using the (a) rotating mandrel, and the (b) parallel plate techniques, (c) Calculated electric field strength vectors and (d) electrostatic force (F) analysis associated with the parallel plate techniques [62]...
The potential of an electric field was determined in Section 12.1 in the form of an infinite series, the convergence rate of which decreases with decreasing clearance between the particles, that is, in the area of greatest interest. For a small gap between the surfaces of spherical particles, the electric field strength vector deviates little from the direction of the surface normal. This allows us to carry out asymptotic analysis in calculating the strength of the electric field near the surface of one of the particles. [Pg.355]

Consider the relative motion of two drops of radii Ri and i 2 under the action of hydrodynamic, electric, and molecular forces. Introduce a spherical system of coordinates (r, 0, ) attached to the center of the larger drop 1, the angle 0 being measured from the direction of the external electric field strength vector The expression (12.46) corresponds to a radial electric force acting on drop 2. If both drops are uncharged, qi = q2 = 0 and... [Pg.451]

Electric field strength vector (absolute value). Maxwell field... [Pg.129]

Let the particle be illuminated by linearly polarized light from negative x values with its plane of polarization matching the plane of scattering (horizontally polarized light) with the electric field strength vector... [Pg.109]

The electric field strength vector of the scattered light at long distances from the oscillating dipole (in the wave zone) is given by (Rayleigh, 1881 Volkcnshtcin, 1051 Fabelinski, 1065 Kerker, 1060 Sivukhin, 1980)... [Pg.109]

Experiment measures the intensity of light, i.c. the radiation energy per unit area per unit time. According to the expression for the Poynting vector, the intensity is proportional to the squared amplitude of the electric field strength vector. As the proportionality coefficient is the same for both the incident and scattered beam, then... [Pg.110]

As in previous chapters we work in the continuum limit employing quantities averaged over macroscopically infinitesimal volume elements and disregarding microscopic local variations associated with the molecular structure (see Brown 1956). These considerations will be limited to processes sufficiently slow to restrict the treatment to time independent or quasistatic fields. The validity of Maxwell s equations of electrostatics is presupposed. The basic electric state variables are the electric field strength vector E, the electric flux density (or electric displacement) vector D, and the electric polarization vector P, related by... [Pg.55]

Assume that electrical conductors, such as aqueous solutions containing charged particles known as ions, exists in a static electrochemical system and that there exists an irrfinitesimal current flow. Thus, an electric field strength vector E at a point P in space and an inner electric potential of the system are defined below, respectively [1]... [Pg.28]

Examining a single component Ei of the electric field strength vector E, it may be described for a linear electric potential distribution between two points with the potentials (pa and ipi, and the distance vector component Si in the regarded direction by... [Pg.31]

The transformation of the volume integral over A into a surface integral over the volume s closed surface dA allows for the application of the surface flux boundary conditions of Eq. (3.35). The virtual electric potential gradient vSif may be represented by the virtual variant SE of the electric field strength vector of Eq. (3.39) ... [Pg.35]

Here is the virtual work of external charges, and the virtual work of internal charges. As the contained virtual electric field strength vector 8E is assembled from derivatives of the virtual electric potential Sip, the latter has to be continuously differentiable. Further on, the virtual electric potential has to comply with the actual conductive boundary conditions of Eq. (3.36). The initial axiom of Remark 3.1 may now be reformulated for the virtual electric potential. [Pg.35]

The electric field strength vector measured in volt per metre... [Pg.1580]

E EMF, electric field strength (vector) V volt, volume... [Pg.226]

Figure 4.1 Force lines of a nonuniform electrostatic field and orientation of an electric field strength vector at a point A. Figure 4.1 Force lines of a nonuniform electrostatic field and orientation of an electric field strength vector at a point A.

See other pages where Electric field strength vector is mentioned: [Pg.14]    [Pg.12]    [Pg.494]    [Pg.330]    [Pg.154]    [Pg.55]    [Pg.840]    [Pg.719]    [Pg.718]    [Pg.110]    [Pg.234]    [Pg.136]    [Pg.100]   
See also in sourсe #XX -- [ Pg.154 ]

See also in sourсe #XX -- [ Pg.55 ]




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