Griffiths, Introduction to Electrodynamics, 3rd ed., Upper Saddle River, NJ: Prentice Hall, 1999. For example, in this Demonstration, the expansion of dipole has two significant terms, and the computed coefficient for each of these terms should be made to approach the limit rather than. Therefore, coefficients for the and have been divided by two so that the expansion does not duplicate the contributions to the radial component of the electric field. When an expansion includes a term with, it will also include because the real (or imaginary) part of can be expressed as a multiple of the real (or imaginary) part of. Likewise, expansion coefficients for the radial component of electric fields, corresponding to higher-order multipole charge densities, can be computed by summing over a subset of vectors related to the spherical harmonics. Using this quantity as a coefficient for gives an expansion for the monopole electric field: in units of. However, the uniform density in this Demonstration is chosen according to the isotropic spherical harmonic, leading to a computed value of approximately for a point charge. When the subset of vectors is chosen from a distribution such that the sample can be described by one density as a function of solid angle, the computed quantity can equal the electric flux in Gauss's law. This Demonstration computes an electric flux through the surface of a sphere centered at the origin, multiplying a sample density constant by a sum of radial components of the electric field (multiplied by or ) over a subset of all vectors with norm equal to, the radius of the surface of integration. As an approximation to the exact solutions, a multipole expansion can be computed using numerical integration. Each of the monopole, dipole, quadrupole and octupole charge densities belongs to a -dimensional representation of the 3-dimensional rotational group, with their characteristic symmetries. A very useful representation is an expansion of the potential, expressed in terms of spherical harmonics, specifically of the form. Įxact forms for electric potentials can be found by integrating over the charge distribution of the source. The monopole potential (as from a point charge) is spherically symmetrical, varying as. Each of these distributions represents a solution of Poisson's equation. Dipoles, quadrupoles and octupoles all have a unique angular distribution of flux, all of which integrate to zero. Though Gauss's law can facilitate the expression of the electric field of a point charge, expansion of the electric field created by a configuration of point charges requires a sum including higher-order multipole functions. Gauss's law then equates the flux of the electric field through a Gaussian surface to the source density within the boundary of that surface. The gradient of the potential gives the electric field. The contributions from represent monopole, dipole, quadrupole and octupole sources, respectively, and sums of these can generate any realistic potential. In classical electromagnetic theory, the potential of a reasonably localized charge distribution can be represented by a multipole expansion, which is based on a sum of terms of the form.
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