By Bassem R. Mahafza
ISBN-10: 1439884951
ISBN-13: 9781439884959
Built from the authors graduate-level classes, the 1st variation of this ebook crammed the necessity for a finished, self-contained, and hands-on remedy of radar structures research and layout. It quick grew to become a bestseller and was once greatly followed by way of many professors. the second one version outfitted in this winning layout by way of rearranging and updating issues and code.
Reorganized, extended, and up to date, Radar structures research and layout utilizing MATLAB®, 3rd variation keeps to assist graduate scholars and engineers comprehend the numerous matters keen on radar structures layout and research. each one bankruptcy contains the mathematical and analytical assurance priceless for acquiring a fantastic knowing of radar idea. also, MATLAB functions/programs in each one bankruptcy additional increase comprehension of the idea and supply a resource for developing radar method layout requirements.
Incorporating suggestions from professors and practising engineers, the 3rd version of this bestselling textual content displays the cutting-edge within the box and restructures the cloth to be less complicated for direction use. It comprises numerous new themes and plenty of new end-of-chapter difficulties. This version additionally takes benefit of the recent good points within the most modern model of MATLAB. up-to-date MATLAB code is accessible for obtain at the books CRC Press website.
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Additional info for Radar Systems Analysis and Design Using MATLAB, Third Edition
Sample text
3 4 4S R kT o FL Eq. m” implements the low PRF radar equation given in Eq. 27). m” computes (SNR)np. 6GHz , antenna gain G = 45dB , radar losses L = 6dB , noise figure F = 3dB . The bandwidth is B = 5MHz . 1m . m” listed in Appendix 2-A. 2a. 2b. 3. High PRF Radar Equation In high PRF radars, the transmitted signal is assumed to be a periodic train of pulses, with pulse width of W and period T . This pulse train can be represented using an exponential Fourier series, where the central power spectrum line (DC component) for this series contains 2 most of the signal’s power.
22) Although Eq. 22) is widely known and used as the Radar Range Equation, it is not quite correct unless the antenna temperature is equal to 290K . In real-world cases, the antenna temperature may vary from a few degrees Kelvin to several thousand degrees. However, the actual error will be small if the radar receiver noise figure is large. In order to accurately account for the radar antenna temperature, one must use Eq. 17) in Eq. 22). Thus, the radar equation is now given by 2 2 Pt G O V SNR o = -----------------------------------.
2 2 T P av G O VW SNR = --- -----------------------------------. W 4S 3 kT FLR 4 o Eq. 35) Define the time it takes the radar to scan a volume defined by the solid angle : as the scan time T sc . The time on target can then be expressed in terms of T sc as T sc T sc -T T . T i = ------ = -----: a e nB Eq. 36) Assume that during a single scan only one pulse per beam per PRI illuminates the target. It follows that T i = T and, thus, Eq. 35) can be written as 2 2 P av G O V T sc ------- T a T e SNR = -----------------------------------3 4 4S kT o FLR : Eq.
Radar Systems Analysis and Design Using MATLAB, Third Edition by Bassem R. Mahafza
by William
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