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(E)GPRS with IR-TU3 3 Ideal FH No FH 2.5 EGPRS IR gain (dB) 2 1.5 1 0.5 0 0 5 10 15 CIR (dB) (a) 20 25 30 0

The technology to create non-spherical lenses was developed to reduce image distortion that is a common characteristic of a spherical lens Aspherical lenses are generally molded out of plastic or the plastic is coated onto the surface of a glass lens chromatic aberration Occurs when light rays travels through glass (or a lens) Each light wave frequency bends (refracts) at a different angle while traveling through the lens Short wavelengths (toward the blue) are refracted more than long wavelengths (toward the red) Thus, different color wavelengths are exposed on different portions of the photosensitive material (film or sensor) Achromatic lenses solve this problem by combining lenses with different refractive indexes color fringing One of the effects of lateral chromatic aberration It appears as magenta and green bands at contrast boundaries Color fringing is always more apparent on the edge of the image than the center because of the lens curvature.

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where we have introduced the shaping parameter [Czarnecki 2001] This parameter allows modifications to the paraboloidal shape, where = 1 gives the normal paraboloid and = 05 gives the equation for a cone Examples of possible cross sections (generating curves) are shown in Figure 318 Thus, the same equation can be used to characterize many typical shapes, from pointed to flat-topped surfaces Similar variations can be applied to hyperboloids and ellipsoids The results for the paraboloid are included in the discussion in the next section, where different shapes are compared The electromagnetic aspects, including mutual coupling and radiating patterns for paraboloidal array antennas, are discussed in detail in s 7 and 8 337 Comparing Shapes The studied shapes differ in curvature and in the slope of the sides This is important in the trade-off of performance versus scan angle.

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It becomes worse at the image corners depth-of-field (DOF) The distance range at which the subject is acceptably sharp is defined as DOF DOF can be changed by changing the size of the aperture A larger aperture (smaller f-number) causes a narrow DOF range A smaller aperture (larger f-number) creates a wide DOF range dispersion The variation in a lens-element s ability to bend light..

We have looked mainly at the minimum effective area within the scan region but, in reality, the requirements are often more detailed and different weights can be given to different regions of the coverage A summary of how different shapes make use of the available size (2R base diameter) is shown in Figure 319, where we have also included a hyperbolic shape and the planar case for reference All cases shown in this figure (except the pyramid and the plane) have h/R = 1 The hyperboloid has an eccentricity e = 11 We see that performance very much depends on the antenna shape The pyramid makes poor use of the available base area (inscribed in the 2R diameter circle) The single plane surface performs well up to the scan limit of 60 , but covers only 50% of the required volume.

Figure 8-11: Break tags, denoted by shield symbols, wrap your lines without the additional line spacing created by <p> tags. You can enable Dreamweaver to mark <br> tags with a symbol: a gold shield with the letters BR and the standard Enter/Return symbol. To make the break symbol visible, you must first choose Edit Preferences (Dreamweaver Preferences) and select the Line Breaks checkbox in the Invisible Elements category. Then show invisible elements by choosing View Visual Aids Invisible Elements.

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