ASU/NASA SPACE GRANT RADAR SYSTEM ANALYSIS & DESIGN Ja’Lon Sisson Mentor: Prof. Daniel W. Bliss TABLE OF CONTENTS General Information & Applications of Radar Electromagnetic Radiation Pulse-Doppler Radar Doppler Effect Simulation Mono-Static – Stationary Mono-Static – Active Bi-Static – Active References GENERAL INFORMATION & APPLICATIONS OF RADAR RAdio Detection And Ranging = RADAR Radar is an object-detection system that uses electromagnetic radiation to determine the range, altitude, direction, or speed of objects . Modern uses of radar include defense systems, outer space surveillance, flight control, anti -collision systems, and many other applications. GENERAL INFORMATION & APPLICATIONS OF RADAR A radar system has a transmitter that emits radio waves in predetermined directions. When these come into contact with an object they are usually reflected or scattered in many directions. Radar signals are reflected especially well by materials of considerable electrical conductivity. Some of the scattered radio waves are reflected back and detected by a receiver. If the object is moving away or toward the receiver, there is a slight change in the frequency, caused by the Doppler effect. Fun Fact: Illumination GENERAL INFORMATION & APPLICATIONS OF RADAR Isotropic Antenna Directional Antenna Pt Pt = 2 (4p )R Pt Gt Pt = 2 (4p )R P t = Transmitter power P t = Transmitter power G t = Gain of the transmitting antenna R= Range from Antenna R= Range from Antenna GENERAL INFORMATION & APPLICATIONS OF RADAR Gain is the radiation intensity relative to a lossless isotropic reference. G= 4p Ae l 2 A e = Ef fective Area (aperture*efficiency) λ= wavelength (c/f) In general, an increase in gain is accompanied by a decrease in beam width. ELECTROMAGNETIC RADIATION Electromagnetic Radiation is emitted and absorbed by charged particles. Radar absorbing materials contain either resistive or magnetic substances to reduce radar reflection PULSE-DOPPLER RADAR A Pulse-Doppler radar is a radar system that determines the range to a target using pulse -timing techniques, and uses the Doppler Shift of the returned signal to determine the target object's velocity. c*t R= 2 DOPPLER EFFECT The Doppler ef fect (or Doppler shift) is the change in frequency of a wave for a target moving relative to an observer. When the object of interest is moving toward the receiver, each successive reflection from the transmitted signal is emitted from a position closer to the receiver than the echo. The time between the arrival of successive wave crests at the receiver is reduced, causing an increase in the frequency. DOPPLER EFFECT 1+ v c) fr = ft ( 1- v c ft fd = fr - ft = 2v (c - v) ft fd » 2v c fd (c) v» 2 ft f r = Shifted Frequency f t = Original Frequency f d = Doppler Frequency c= Speed of light v= Target velocity MONO-STATIC (STATIONARY) Mono-static: The transmitter and receiver are collocated (same antenna is used to transmit/receive). MONO-STATIC (STATIONARY) Multi-Target MONO-STATIC (ACTIVE) Multi-Target BI-STATIC (ACTIVE) Bi-static: The transmitter and receiver are in dif ferent locations. REFERENCES 1 . " R a d a r. " W i k i p e d i a . N . p . , n . d . We b . 3 0 Au g . 2 014 . <http://en.wikipedia.org/wiki/Radar>. 2 . " H o w R a d a r Wo r k s . " I n s t i t u te f o r G e o p hy s i c s . T h e U n i v e r s i t y o f Te x a s a t A u s t i n , n . d . We b . 1 1 J a n . 2 01 5 . < h t t p : / / w w w. i g . u t e x a s . e d u / r e s e a r c h / p r o j e c t s / m a r s / e d u c a t i o n / r a d a r _ wo r k s . h t m > . 3 . " R a d a r Fu n d a m e n t a l s . " R F C a f e . N . p . , n . d . We b . 1 1 J a n . 2 01 5 . < h t t p : / / w w w. r f c a f e . c o m / r e f e r e n c e s / e l e c t r i c a l / N E E T S - M o d u l e s / N E E T S - M o d u l e - 1 8 - 1 - 1 - 1 10 . h t m > . 4 . Pe l l i s s i e r, V i n c e n t . " R a d a r S y s te m D e s i g n a n d A n a l y s i s w i t h M AT L A B . " M a t h Wo r k s . N . p . , n . d . We b . 17 O c t . 2 014 . < h t t p : / / w w w. m a t h w o r k s . c o m / v i d e o s / r a d a r - s y s t e m - d e s i g n and-analysis-with-matlab81 917. h t m l ? f o r m _ s e q = c o n f 1 0 9 2 & c o n f i r m a t i o n _ p a g e & w f s i d = 5 9 6 7 5 8 6 & r e f r e s h = t r u e > . 5 . " S i m u l a t i n g a B i s t a t i c Po l a r i m e t r i c R a d a r. " M a t h Wo r k s . N . p . , n . d . We b . 10 J a n . 2 01 5 . < h t t p : / / w w w. m a t h w o r k s . c o m / h e l p / p h a s e d / e x a m p l e s / s i m u l a t i n g - a - b i s t a t i c - p o l a r i m e t r i c r a d a r. h t m l > . 6 . " A D o p p l e r S h i f t S p e e d G u n . " C F C P Wo r k . U n i v e r s i t y o f C h i c a g o , n . d . We b . 1 2 J a n . 2 01 5 . < h t t p : / / c f c p w o r k . u c h i c a g o . e d u / k i c p - p r o j e c t s / n s t a / 2 0 07 / s h e r m a n / d o p p l e r. h t m > . 7. " E l e c t r o m a g n e t i c r a d i a t i o n . " W i k i p e d i a . N . p . , n . d . We b . 1 3 S e p t . 2 014 . <http://en.wikipedia.org/wiki/Electromagnetic_radiation >. THANK YOU! QUESTIONS?