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The sloping dipole (Fig 6-8) is popular with those operators who need a low angle of radiation, and are not overburdened with a large amount of land to install the antenna This antenna is also called the sloper and the slipole in various texts The author prefers the term slipole, in order to distinguish this antenna from a sloping vertical of the same name Whatever it is called, however, it is a half-wavelength dipole that is built with one end at the top of a support, and the other end close to the

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ground, and being fed in the center by coaxial cable Some of the same comments as obtained for the inverted-vee antenna also apply to the sloping dipole, so please see that section also Some operators like to arrange four sloping dipoles from the same mast such that they point in different directions around the compass (Fig 6-9) A single fourposition coaxial cable switch will allow switching a directional beam around the compass to favor various places in the world

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One of the rarely discussed aspects of antenna construction is that the length/diameter ratio of the conductor used for the antenna element is a factor in determining the bandwidth of the antenna In general, the rule of thumb states that large cross-sectional area makes the antenna more broadbanded In some cases, this rule suggests the use of aluminum tubing instead of copper wire for the antenna radiator On the higher-frequency bands that is a viable solution Aluminum tubing can be purchased for relatively small amounts of money, and is both lightweight and easily worked with ordinary tools But, as the frequency decreases, the weight becomes greater because the tubing is both longer and (for structural strength) must be of greater diameter On 80 m, aluminum tubing is impractical, and at 40 m it is nearly so Yet, 80 m is a significant problem, especially for older transmitters, because the band is 500 kHz wide, and the transmitters often lack the tuning range for the entire band Some other solution is needed Here are three basic solutions to the problem of wide-bandwidth dipole antennas: folded dipole, bowtie dipole, and cage dipole

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One way of visualizing how a waveguide works is to develop the theory of waveguides from the theory of elementary parallel transmission lines (see Chap 3) Figure 19-3A shows the basic parallel transmission line which was introduced in Chap 3 The line

Development of the rectangular waveguide from parallel transmission lines 371 consists of two parallel conductors separated by an air dielectric Because air won t support the conductors, ceramic or other material insulators are used as supports There are several reasons why the parallel transmission line per se is not used at microwave frequencies Skin effect increases ohmic losses to a point that is unacceptable Also, the insulators supporting the two conductors are significantly more

19-2 Rectangular waveguide (end view)

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