Linear Wire Antennas Infinitesimal Dipole From: Balanis, C. A. “Antenna Theory, Analysis and Design” Third Edition. A John Wiley & Sons, Inc.,Publication.

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1 Linear Wire Antennas Infinitesimal Dipole From: Balanis, C. A. “Antenna Theory, Analysis and Design” Third Edition. A John Wiley & Sons, Inc.,Publication. EEUU. 2005. Mg. Ing. Sergio M. Martínez.

2 Wire antennas, linear or curved, are some of the oldest, simplest, cheapest, and in many cases the most versatile for many applications. It should not then come as a surprise to the reader that we begin our analysis of antennas by considering some of the oldest, simplest, and most basic configurations. Initially we will try to minimize the complexity of the antenna structure and geometry to keep the mathematical details to a minimum. An infinitesimal linear wire (l << λ) is positioned symmetrically at the origin of the coordinate system and oriented along the z axis, as shown in Figure 4.1(a). Although infinitesimal dipoles are not very practical, they are used to represent capacitor-plate (also referred to as top-hat-loaded) antennas. In addition, they are utilized as building blocks of more complex geometries. The end plates are used to provide capacitive loading in order to maintain the current on the dipole nearly uniform. Since the end plates are assumed to be small, their radiation is usually negligible. The wire, in addition to being very small (l << λ), is very thin (a << λ). The spatial variation of the current is assumed to be constant and given by where I 0 = constant. Linear Wire Antennas

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4 To find the fields radiated by the current element, the two-step procedure of Figure 3.1 is used. Radiated Fields It will be required to determine first A and F and then find the E and H. The functional relation between A and the source J is given by (3-49), (3-51), or (3-53).

5 Similar relations are available for F and M, as given by (3-50), (3-52), and (3-54). (See Book). R the distance from any point on the source to the observation point. J represent linear densities For electric currents Ie, (3-51) reduce to line integrals of the form:

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8 Geometrical arrangement of an infinitesimal dipole and its associated electric-field components on a spherical surface.

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