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Advancements on interferometric radar: studies and applications Coordinatore: Prof. Carlo Atzeni Tutor: Prof. Massimiliano Pieraccini Candidato: Andrea Barucci CorsodiDottorato in IngegneriadeiSistemiElettronici XXIII ciclo

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Ph.D. thesis presentation by Andrea Barucci Advancements on interferometric radar: studies and applications

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Page 1: Phd final slides

Advancements on interferometric radar: studies and applications

Coordinatore: Prof. Carlo Atzeni

Tutor: Prof. Massimiliano Pieraccini

Candidato: Andrea Barucci

CorsodiDottorato

in IngegneriadeiSistemiElettronici

XXIII ciclo

Page 2: Phd final slides

Introduction

Page 3: Phd final slides

Applicationofadvancedmonitoringtechniquesto the monitoring and

characterizationofquarriesfor the profit optimization and for the

safety and environmentalprotectionof the quarrymining

Page 4: Phd final slides

CWSF Ground BasedSynthetic Aperture Interferometric radar

CentralFrequency 16.75 GHz

Banwidth 400 MHz

Tx Power 26 dBm EIRP

SAR scan length 2 m

SAR acquisition time 4 min (minimum)

Power consumption < 40 W

Page 5: Phd final slides

Radar installation

Powersupply system

Wide angle SAR

Page 6: Phd final slides

Start 16 feb 2009

End 25 mar 2009

Days of measurement 39

N. Radar acquisitions about 600 (1 every 2 hours)

Measurementcampaign

Page 7: Phd final slides

RCS SAR image

Range

resolution

0.5 m

Cross

range

resolution

5mrad

Page 8: Phd final slides

Interferograms in scarp area

(m) (m) (m)

(m)(m)(m)

(m)

(m)

(m)

(m)

(m)

(m)

Eachinterferogramrelatesto a timelapseoftwohours

Page 9: Phd final slides

Interferometricanalysisin the wallarea

1. PSsselection

DispersionIndex

2.

Atmosphericmeanphasescreen

removal3. Calculationofdisplacements

About 50.000 PSsselected in

all the area

Page 10: Phd final slides

Interferometricanalysis in the wallarea

cum

ula

ted

dis

pla

cem

ent

Timeperiod: 23 days

Selectionof 50 pixels in the wall

Page 11: Phd final slides

Interferometricanalysis in the wallarea

cum

ula

ted

dis

pla

cem

ent

Timeperiod: 3days

Selectionof 50 pixels in the wall

Page 12: Phd final slides

Validationof the methodby a corner reflector

Distance: 800 m

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Actual

(mm)

Measured

(mm)

Error

(mm)

2.0 2.05 0.05

1.0 0.89 0.11

0.5 0.53 0.03

Page 14: Phd final slides

Interferometric DEM of the quarry

Radar

Laser

Conclusions• A ground based Synthetic Aperture Interferometer was

successfully tested for the first time in a quarry.

• The system showed an accuracy of few tenths of a millimeterin displacement’s measurement, over a long period and at800 meters of distance.

• In short term measurements a simulation showed anaccuracy in measurement of displacements of the order of atenth of a millimeter.

• DEM reconstruction showed some limitations especially inhigh slopes.

Page 15: Phd final slides

S. T. Bramwell, P. C.W. Holdsworth, and J.-F. Pinton,

Universality of rare fluctuations in turbulence and critical

phenomena, Nature 396, 1998

Physical Review Letters [2000, 2005, 2008]

• Long term atmospheric artifacts on GB-SAR are known

• Radar signal propagation through tropospheric turbulence is a new

research topic

Data

Analysis

Classic:Fluctuations of signal

as a function of

turbulence

Modern:Correlated systems,

Gumbel statistics

Experiment

Universal fluctuations in tropospheric radar measurements

Introduction

Page 16: Phd final slides

Firenzuola scenario

Page 17: Phd final slides

Scenario and raw-data

CR distance

Ultrasonic Anemometer / Weather sensor

Radar sampling freq Range Resolution

Observational time

65 m 4/1Hz About 50 Hz 1 m 6 h

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Detrending – High-pass filter

• Turbulent phenomena occur

at the micro scale,

corresponding to distances

shorter than 1 km, which are

the usual working distances for

a GB-SAR.

• We use a moving average to

remove the fluctuations on

temporal scales greater than 30

minutes

Page 19: Phd final slides

Time series data analysis

We use overlapping

temporal windows, with

length of about 30

minutes:

- About 10^5 points ->

rare fluctuations & good

statistics

- Constant Reynolds

number

Turbulent Kinetic

Energy (TKE) is a

measure of the

turbulence

Page 20: Phd final slides

Wind fluctuations dependency

R = 0.98 R = 0.89

Page 21: Phd final slides

Radar signal statistics & Correlated Systems

Correlated

Systems

Turbulence

Ising& 2D XY

Forest fires,

etc.

River water

level

Radar signal through a

turbulent atmosphere

Global quantity

Generalized

Gumbel PDF

Radar Data

statistics?

Page 22: Phd final slides

Generalized Gumbel

• Generalized Gumbel describes the fluctuations in Correlated Systems, its

shape depends on a real parameter a

• As a varies, the shape of the distribution varies from a completely

asymmetric, negatively skewed, distribution to a symmetric one quite similar

to a Gaussian function

• The parameter a has been proposed to be inversely related to the correlation

length of the system

Page 23: Phd final slides

Data distribution

• Fit of the data with the GG(a)

• Amplitude statistic appears to fit with the GG

• Phase statistic doesn’t show the same behaviour

• The radar data distributions calculated over the analysis windows show different means and standard deviations new method from Nature

Amplitude

Phase

Page 24: Phd final slides

• a is determined by the turbulence strength

• In hard windy conditions, a is nearly equal to pi/2 which is the value

for which GGa is approximately the Bramwell-Holdsworth-Pinton

distribution observed in turbulence and critical systems

Andrea Barucci

Page 25: Phd final slides

Conclusions

• The radar signal statistic:

– It is influenced by the turbulence

– It is a global quantity able to measure the “correlation of the

atmosphere” at the micro-scale

• We confirm the adequacy of the Gumbel statistic to describe

highly correlated complex systems

• SAR images - turbulence: work in progress• Paper published by Europhysics Letters: A. Barucci, G. Macaluso, D. Mecatti, L. Noferini, D. Fanelli, A.

Facchini, M. Materassi, M. Pieraccini and C. Atzeni, Universal fluctuations in tropospheric radar

measurements, EPL, 89 (2010) 20006, DOI 10.1209/0295-5075/89/20006