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The same strategies that worked for vertical antennas also work for horizontal antennas, although in the horizontal case we are simulating a half wavelength (180 ) balanced antenna rather than a /4 unbalanced antenna Figure 26-3 shows several different shortened, low frequency antennas that are based on the same methods as the verticals shown previously Figures 26-3A through 26-3C show discretely loaded dipole antennas Figures 26-3A and 26-3B are center-loaded versions, and Fig 26-3C is a center (of each element) -loaded version In each case, it is assumed that the radiator elements are the same physical length In the example of Fig 26-3A, the coil is tapped to provide a match to either 52- or 75- transmission line In some variants, the shield of the coaxial-cable transmission line is connected directly to the junction of the coil and one radiator element, and the coax center conductor is connected to the tap that best matches the impedance of the line The impedance-matching problem is solved a little differently in Fig 26-3B In this type of antenna, the coil is used to center-load the dipole, but the transmission line is connected to a link wound on the same form as the loading inductor The turns ratio between the loading inductor and the coupling link determines the impedance match A hairpin linear loading scheme is shown in Fig 26-3D This design is basically the same as for the vertical case, but it is balanced out of respect for the design of the dipole This type of design is used for both the driven and parasitic elements on some commercial 40-m beam antennas In addition, some add-on 40-m dipoles (designed for beam antennas that were intended for operation at frequencies in the 20-m and higher bands) use this method Such antennas are essentially rotatable dipoles The continuously loaded dipole of Fig 26-3E is constructed like the helical vertical (ie, about a half-wavelength of insulated wire is wound over the entire length of an insulated rod or pipe of some sort) The winding can be either broken at its center point to accommodate the feedline, or link-coupled to the transmitter, or receiver, as shown in Fig 26-3F Of the two feed methods, the most popular appears to be the type that breaks the winding into two pieces The form of continuously loaded dipole in Fig 26-3E has a combination of the two methods of feed The distributed loading coil is broken into two sections, as is often done on continuously loaded dipoles But in this case, a portion of the overall inductance is made by using a discrete inductor that is part of a toroidal transformer T1 The length of the wire used for the continuous loading coil is somewhat shorter (find by experimentation) than otherwise would be the case because of the inductance of the transformer secondary Transformer T1 can be wound using the same sort of toroidal ferrite or powdered iron core used for Balun transformers.



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decreases during a collision, as shown in this force-time graph Force (N)

What is the result A count: 33 B count: 40 C count: 45 D count: 65 E Compilation fails F The code runs in an endless loop

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To solve an equation means to find the value of the variable that makes the equation a true statement To solve equations, apply the distributive property and the properties of equality Any properties of equalities that you apply on one side of an equation, you also must apply on the other side Distributive property For any numbers a, b, and c, a(b c) ab ac a(b c) ab ac Example: Use the distributive property to expand the following expression 3(x 2) 3x (3)(2) 3x 6 Addition and subtraction properties of equality If two quantities are equal and the same number is added to (or subtracted from) each, then the resulting quantities also are equal a c b c a c b c Example: Solve x x x 3 3 3 x Example: Solve t t t 2 2 2 t 7 7 10 2 5 5 7 2 5 using the subtraction property 3 3 7 using the addition property

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Multiplication and division properties of equality If two equal quantities each are multiplied by (or divided by) the same number, then the resulting quantities also are equal ac bc a b , for c 0 c c 3 using the multiplication property

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Answer (for Objective 23): D is correct This invocation will run without error A, B, and C are incorrect because the code compiles, and neither assertion is appropriate because ultimately they are testing the args of main() E, F, and G are incorrect Each will throw an AssertionError

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26-3 Inductance loading of a dipole: (A) center loading with impedance tapped coil; (B) center loading with transformer coupling; (C) loading at center of elements; (D) linear loading (hairpin); (E) linear or length loading; (F) transformer coupling

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