radar signals tutorial 3 lfm, coherent train and frequency coding

24
Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Upload: bruno-mcdonald

Post on 20-Jan-2016

235 views

Category:

Documents


2 download

TRANSCRIPT

Page 1: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Radar Signals

Tutorial 3LFM, Coherent Train and Frequency Coding

Page 2: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

OutlineOutline

More on LFM Range sidelobe reduction

Coherent train of identical pulses Large improvement in Doppler resolution

Frequency-modulated pulse (besides LFM) Costas code Nonlinear FM

Page 3: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

LFM reviewLFM review

Page 4: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

LFM range sidelobe reductionLFM range sidelobe reduction

Amplitude weighting Square-root of Hamming window

Page 5: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

To maintain matched filtering, the weight should be split between the transmitter and receiver

Yet a linear power amplifier is required

Page 6: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

LFM Hamming-weighted LFM

Sidelobe suppression and mainlobe broadening

Page 7: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

A train of pulsesA train of pulses

A coherent train of identical unmodulated pulses Signal

Complex envelop

Unmodulated pulse

Page 8: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

6 pulses and duty cycle = 0.2

Page 9: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Large improvement in Doppler resolution

Page 10: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Resolutions and Ambiguities

Page 11: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Frequency-modulated pulsesFrequency-modulated pulses

Previously discussed LFM The volume of AF concentrates in a slowly decaying

diagonal ridge An advantage when Doppler resolution is not

expected from a single pulse Relatively high autocorrelation sidelobe

Other frequency-modulation schemes Better Doppler resolution Lower autocorrelation sidelobes

Page 12: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Matrix representation of quantized LFMMatrix representation of quantized LFM

M contiguous time slices tb

M f

requ

ency

sli

ces Δ

f There is only one dot in each column and each row.

The AF can be predicted roughly by overlaying a copy of this binary matrix and shifting it to some (delay, Doppler).

A coincidence of N points indicates a peak of N/M

Page 13: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Costas coding (1984)Costas coding (1984)

The number of coinciding dots cannot be larger than one for all but the zero-shift case.

A narrow peak at the origin and low sidelobes elsewhere

Page 14: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding
Page 15: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

A Costas signal Hopping frequency Complex envelope

Page 16: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Check whether CostasCheck whether Costas

If all elements in a row of the difference matrix are different from each other, the signal is Costas.

Page 17: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Peak sidelobe is -13.7 dB

Page 18: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Exhaustive search of Costas codesExhaustive search of Costas codes

Page 19: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Construction of Costas codeConstruction of Costas code

Welch 1 (Golomb & Taylor, 1984) Applicable for M = p – 1 where p can be any prime

number larger than 2. Let α be a primitive element in GF(p) Numbering the columns of the array j = 0,1,...,p-2

and the rows i = 1,2,...,p-1. Then we put a dot in position (i, j) if and only if i = αj

Page 20: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

M = 4 p = M + 1 = 5 GF(5) = {0 1 2 3 4} Use α = 2:

Use α = 3:

{1 2 4 3}

{1 3 4 2}

Page 21: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Nonlinear Frequency ModulationNonlinear Frequency Modulation

Stationary-phase concept The energy spectral density at a certain frequency is

relatively large if the rate of the change of this frequency is relatively small

Design the phase (frequency) to fit a good spectrum

Page 22: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding
Page 23: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Low auto-cor sidelobes

High sidelobes at high Doppler cuts

Page 24: Radar Signals Tutorial 3 LFM, Coherent Train and Frequency Coding

Future talksFuture talks

Phase-coded pulse Barker codes Chirplike phase codes Our codes

Thank youSep. 2009