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Communications, Radar & Electronic Warfare (201.. - Index of

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108<strong>Communications</strong>, <strong>Radar</strong> and <strong>Electronic</strong> <strong>Warfare</strong>-- - ----Figure 7.6 Ship radar cross-section illustration before and after a missile holes the ship on the starboardside. <strong>Radar</strong>-guided missiles arriving after this hole has been created will tend to follow the first missile intothe hole.At this point we have not considered the concept that a radar will not illuminate atarget only once during a sweep. The number <strong>of</strong> successive pulses that the target will beilluminated by is dependent on the Pulse Repetition Frequency, the beamwidth in thedirection <strong>of</strong> sweep and the speed at which the antenna rotates or repeats the sweep. Fora mechanically rotating antenna, this can be expressed by:M =cp(PRF)6(RPM)cosOeOr, for a mechanically rotated antenna with a vertical as well as horizontal sweep:M = _ _ -,- F __6w" t,,(RPM)cosOewherePRF =Pulse Repetition Frequency per second.RPM =Rotation rate Per Minute.cp =o =Azimuth beamwidth in degrees.Elevation beam width in degrees.Oe = Target elevation angle.Wv =t,. =Vertical scanning speed in degrees per second.Vertical scan time in seconds (including dead time, if any).This equation is in the direction <strong>of</strong> transmission, and is only valid when cp/cos(Oe) isless than 90 degrees. Both the horizontal (left) and vertical (right) movements areshown in Figure 7.7.When the number <strong>of</strong> pulses arriving at the target is known, it is theoretically possibleto determine the probability <strong>of</strong> receiving a target when looking over the received

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