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actual power Prad radiated by the real antenna is used, rather than the power PS supplied to the antenna. These two values are related as Prad APS , where A is the antenna efficiency. Denoting the directivity by d gives G Ad. Often, the directivity is the parameter which can be calculated, and the efficiency is assumed to be equal to unity so that the power gain is also known. Note that A does not include feeder mismatch or polarization losses, which are accounted for separately. The power gain G as defined by Eq. (6.5) is called the isotropic power gain, sometimes denoted by Gi. The power gain of an antenna also may be referred to some standard other than isotropic. For example, the gain of a reflector-type antenna may be stated relative to the antenna illuminating the reflector. Care must be taken therefore to know what reference antenna is being used when gain is stated. The isotropic gain is the most commonly used figure and will be assumed throughout this text (without use of a subscript) unless otherwise noted. 6.7 Radiation Pattern The radiation pattern shows how the gain of an antenna varies with direction. Referring to Fig. 6.3, at a fixed distance r, the gain will vary with and and may be written generally as G( , ). The radiation pattern is the gain normalized to its maximum value. Denoting the maximum value simply by G [as given by Eq. (6.5)] the radiation pattern is g( , ) G( , ) G (6.6)

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Type the program in Fig. 10.7 and see what happens (don t type the line numbers). In Line 15 we calculate an index into the array SomeShape to retrieve the right pair of data. The outcome is that we can now say SomeShape[J] to obtain the command element of the pair and SomeShape[J 1] to retrieve the value element of the pair. Why this formula for J Remember that the rst element of the array is 0. So the elements 0 and 1 are the rst pair, 2 and 3 the second, 4 and 5 the third, and so on. Can you see a pattern We have 0, 2, 4, 6,... for the rst element of the pairs and 0 1, 2 1, 4 1, 6 1,... for the second. So if we are counting using a for-next loop using 1, 2, 3, 4,... then to get 0, 2, 4, 6,... we use the formula in Line 15. The if-then statements (Lines 16 18) are to make sure that the right command is executed. The limit for the for-next loop in Line 14 uses the function MaxDim() allowing the program to determine how many elements there are in the SomeShape array (see Sec. C.8). Since the data is in pairs, we divide the number of elements by two to calculate the number of pairs. If you replace the data in the Data statements on Lines 11 to 13 you can create any shape. You can have as many Data statements as you need to draw the shape, you are not limited to just the three in the program.

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The radiation pattern gives the directional properties of the antenna normalized to the maximum value, in this case the maximum gain. The same function gives the power density normalized to the maximum power density. For most satellite antennas, the three-dimensional plot of the radiation pattern shows a well-defined main lobe, as sketched in Fig. 6.6a. In this diagram, the length of a radius line to any point on the surface of the lobe gives the value of the radiation function at that point. It will be seen that the maximum value is normalized to unity, and for convenience, this is shown pointing along the positive z axis. Be very careful to observe that the axes shown in Fig. 6.6 do not represent distance. The distance r is assumed to be fixed at some value in the far field. What is shown is a plot of normalized gain as a function of angles and . The main lobe represents a beam of radiation, and the beamwidth is specified as the angle subtended by the 3-dB lines. Because in general the beam may not be symmetrical, it is usual practice to give the beamwidth in the H plane ( 0 ), as shown in Fig. 6.6b, and in the E plane ( 90 ), as shown in Fig. 6.6c.

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