Lecture 9. Radar Equation. Dr. Aamer Iqbal. Radar Signal Processing Dr. Aamer Iqbal Bhatti

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1 Lecture 9 Radar Equation Dr. Aamer Iqbal 1

2 ystem Losses: Losses within the radar system itself are from many sources. everal are described below. L PL =the plumbing loss. L PO =the polarization loss. L AP =the antenna pattern loss or scan loss. L PW =the pulse width loss. L Q =the squint loss. L LIM =the limiting loss. L C =the collapsing loss. L OP =the operator loss. L NE =the non-ideal equipment loss. 2

3 Plumbing Loss: Caused by the reflections and absorption within transmitter, duplexer, receiver, and other microwave components. Polarization Loss: Caused by the difference in polarization of transmitter and receiver. Transmitter wave polarization not being absorbed completely by receive antenna. Antenna Pattern Loss: Caused by variation in peak gain of multiple echoes returned from a target (Figure on next lide). Pulse Width Loss: Distribution of power over antenna surface from transmission line is call filling the antenna. During fill time antenna does nor radiate efficiently and loss called pulse width loss occurs (Figure on next lide). quint Loss: Caused by the antenna beam displaced from the axis. Antenna gain in the direction of target will be lower than the peak gain. (Figure on next lide). Limiting Loss: If the limiting occurs in receiver, that portion of signal energy above the saturation point is lost. Collapsing Loss: Dropping a dimension (Azimuth, elevation, Doppler etc ) from system degrades IR due to interference from other resolution cells. 3

4 Operator Loss: In manual systems operator can influence many parameters like gain and signal processing. It is difficult to quantify. Non-ideal Equipment Loss: Caused by the aging of system components. 4

5 Absorption by atmospheric gases and scattering by particles in the atmosphere. Absorption occurs at resonant frequencies. cattering of signal by precipitation (rainfall). cattering by particles smaller than the wavelength is sensitive to frequencies. Higher is the frequency more will be the attenuation. 5

6 L rain L rain = the loss due to rainfall. K rain = the rainfall attenuation factor(db/nmi/mm/hr). r = the rainfall rate (mm/hr). Krain R = range in nmi. K f GHz = the frequency in GHz. rain rr(db) fGHz Example 3-5: Estimate tow way attenuation of a 10GHz radar viewing at 20nmi in uniform rainfall of15mm/hr. How it effects the radar s detection capability. K rain will be 0.13 db/nmi/mm/hr. o loss due to rainfall will be 39dB. Maximum detection range halves for every 12dB loss of signal. 39dB loss decreases detection range by a factor of , or a factor of 9.5. o without rain it can be detected at 190 nmi. 6

7 7

8 These losses are caused by multipath either from transmitter-to-target or from target-to-transmitter. These reflections cause phase shift in polarization which is discussed earlier. We can make beam narrower in elevation to avoid these losses. Frequency Agility to force the loss to change rapidly for estimation. 8

9 ignal Processing has an effect of increasing signal to interference ratio. Its effectiveness is measured by Process gain. ignal integration is one method of achieving process gain. It is the summation of signal contents of several samples of same range bin in order to increase the signal to interference ratio. The effective integration number is given by: N eff = N L /L i L i is the integration loss. 9

10 ignal integration can be coherent or non coherent. Coherent integration: ignal and interference phases are considered. Integration takes place at the intermediate frequency and is coherent. Non Coherent integration: ignals and interference phases are ignored this integration takes place after envelop demodulation of the signal. 10

11 More effective than non coherent Loss usually ranges from 1.0 to 1.7 and is rarely larger than 2.0, whereas in non coherent the loss can be as large as square root of the integration number for very large integrations. Coherent integration can be treated by calculating an equivalent integrated NR ratio and applying this /N to single hit process 11

12 12

13 Pulse Compression is the process of transmitting a wide pulse (pulse width τ E ) and processing it into a narrow pulse (pulse width τ C ). The goal is to use the energy in the wide transmitted pulse for detection and the bandwidth of narrow pulse for range resolution. NR for N L pulses processed together with processing loss of L i is repeated here for convenience PT N LG PT N LG N 3 4 ( 4 ) R KT BFL L L L N 3 4 ( 4 ) R KT FL L L o τ = Pulse width without compression. A GP i o A GP L i 13

14 NR for each compressed pulse segment width can be 2 2 defined as. ' PT CG N PC 3 4 ( 4 ) R KTo FL LALGP NR for entire pulse results from summation of Compression Ratio(The number of compressed pulse width in the echo wave). It will improved by CR. N PC PT CR C N 3 4 ( 4 ) R KT FL o L G L 2 A 2 L L GP i CR E C N PC PT E N LG 3 4 ( 4 ) R KT FL o 2 L L 2 A GP L i 14

15 A reciprocal relationship between bandwidth and compressed pulse width can be generated. 2 2 PT N LG N PC 3 4 (4 ) R KTo ( B / CR) FL LALGPLi With pulse compression, detection can be maintained and range resolution can be improved by keeping the same transmitted pulse width but increasing the bandwidth. Range resolution can remain the same and detection can be improved by increasing transmitted pulse width and maintaining bandwidth. 15

16 The last example presented during last lecture. Find the required peak power if the pulse width is increased to 2000µs. Transmitted Power 15MW Type Antenna Monostatic Antenna effective aperture 320 m 2 Antenna Gain Frequency Rx NF ystem Loss Receive Bandwidth Propagation Path Loss Processing Gain to Noise Minimum NR Ground Plane Loss 94-ft diameter array (46.5dB) 1GHz 1.1dB(1.29) 1.0dB(1.26) 1 MHz 1.3dB(1.35) 29dB(800) 14dB(25.1) 0 db(1.0) 16

17 Transmitted pulse width was 1µs with peak power of 1MW. New pulse width is 2000µs, so transmit peak power will be reduced by a factor of Which is 7.5kW. 17

18 earch radars have a limited time-on-target (T OT ). They do not point the peak gain of antenna at targets for all hits in a look. We require minimum scan time along with considerable time-on-target. The scan rate can be set by signal processor so that the number of pulses transmitted as the antenna beam scans past a given point matches the integration number in the signal processor. N 3 / PRF C ( ( AZ ) ) N C = the number of pulses transmitted per antenna beamwidth as the beam scan. 18

19 θ 3(AZ) = the 3dB azimuth beamwidth of the antenna ω = the antenna scan rate in degrees per sec. N (4 ) 3 PT G 4 R KT 2 2 3( AZ ) o BFL L A L GP L PRF i 19

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