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33 HEMISPHERICAL COVERAGE 331 Introduction Now we consider the three-dimensional case in which the beam is steered over a full hemispherical volume, 2 steradians For our discussion, we think of this as the upper hemisphere with scan angles s from zenith to the horizon and 0 360 in the azimuth (For some applications, the coverage might be oriented differently, as in a nose-mounted radar in an aircraft, where the region would be the forward hemisphere instead) The possible solutions include an arrangement of planar surfaces (pyramids), as discussed in Section 31, and several types of curved surfaces The planar surfaces need not to be connected, since only one surface is used at a time For installations on ships, for instance, two surfaces can be mounted separately to cover the forward region, and two surfaces positioned to cover the aft region.



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The curved surface that first comes to mind is probably a half sphere, matching the shape of the required coverage Many more surfaces can be considered, however, like conical, ellipsoidal, and paraboloidal surfaces Furthermore, the shape within one class of surface depends on one or more parameters, such as eccentricity or focal distance As before, we base our comparison on the effective antenna area To our previous list of assumptions for the analysis, we add the following: The antenna arrangements will fit within a base diameter of 2R The active surface for a curved solution is defined by a maximum local scan angle of 60 All curved alternatives are rotationally symmetric The total antenna area is taken as a measure of cost It turns out that the optimum multisurface solution (for pyramidal shapes) has a maximum scan angle near 60 .

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We, therefore, impose a 60 scan limit also for the curved cases for simplicity With this fixed, we do not need to introduce the parameter (we let = 1) when comparing the different shapes In order to illustrate the concepts of active region and active elements, we take an antenna array with radiating elements on a surface with a paraboloidal shape as an example (see Figure 39) In this example, the antenna has a height-to-diameter ratio of h/D = 05 The radiating element positions are indicated by circles, suggesting circular waveguide apertures as radiators The antenna has 177 elements, of which a certain number can be used (are active), depending on the scan direction..

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In practice, the onset of backstreaming is determined by two techniques. One method is to monitor the increase in the screen power supply current as the magnitude of the accel grid voltage is decreased. Increases in the measured current are due to backstreaming electrons, and a 1% increase is defined as the minimum accel grid voltage to avoid backstreaming: the so-called backstreaming limit. For example, the power supply current from Eq. (5.4-17), normalized to the initial beam current, is plotted in Fig. 5-11 as a function of the accel grid voltage for the NSTAR ion optics [29] for the maximum power throttle point TH15 at the beginning of life (BOL). In this figure, the beam potential and electron temperature were assumed to be 12 V and 2 eV, respectively, consistent with measurements made on this thruster. The onset of backstreaming occurs at about -150 V on the accel grid, which is consistent with the data from tests of this engine [30,3 13.

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FIGURE 10-17: Color Dynamics varies the randomness of the foreground and background color used in the footprint to create a stroke. In this example, the spacing for the tip shape was increased to 100% to amplify the effect.

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