SIGNAL PROCESSING ALGORITHMS FOR HIGH-PRECISION NAVIGATION AND GUIDANCE FOR UNDERWATER AUTONOMOUS SENSING SYSTEMS

Similar documents
Design and Development of a Software-Defined Underwater Acoustic Modem for Sensor Networks for Environmental and Ecological Research

Exploitation of Environmental Complexity in Shallow Water Acoustic Data Communications

Moorea 2007 UCSB UWA Modem Results

Effects of snaking for a towed sonar array on an AUV

Time Reversal Ocean Acoustic Experiments At 3.5 khz: Applications To Active Sonar And Undersea Communications

Shallow Water Fluctuations and Communications

Detection of Multipath Propagation Effects in SAR-Tomography with MIMO Modes

HIGH FREQUENCY INTENSITY FLUCTUATIONS

Broadband Temporal Coherence Results From the June 2003 Panama City Coherence Experiments

SWAMSI: Bistatic CSAS and Target Echo Studies

Exploitation of frequency information in Continuous Active Sonar

Mathematical Modeling of Ultrasonic Phased Array for Obstacle Location for Visually Impaired

Principles of Pulse-Doppler Radar p. 1 Types of Doppler Radar p. 1 Definitions p. 5 Doppler Shift p. 5 Translation to Zero Intermediate Frequency p.

MINE SEARCH MISSION PLANNING FOR HIGH DEFINITION SONAR SYSTEM - SELECTION OF SPACE IMAGING EQUIPMENT FOR A SMALL AUV DOROTA ŁUKASZEWICZ, LECH ROWIŃSKI

Ultrasonic Imaging in Air with a Broadband Inverse Synthetic Aperture Sonar

Penetration-free acoustic data transmission based active noise control

Hydroacoustic Aided Inertial Navigation System - HAIN A New Reference for DP

Company Profile. Facilities

DESIGN OF GLOBAL SAW RFID TAG DEVICES C. S. Hartmann, P. Brown, and J. Bellamy RF SAW, Inc., 900 Alpha Drive Ste 400, Richardson, TX, U.S.A.

Non-Data Aided Doppler Shift Estimation for Underwater Acoustic Communication

Tritech International Vehicle Sonar Developments

BYU SAR: A LOW COST COMPACT SYNTHETIC APERTURE RADAR

Using GPS to Synthesize A Large Antenna Aperture When The Elements Are Mobile

Autonomous Underwater Vehicle Navigation.

Potential interference from spaceborne active sensors into radionavigation-satellite service receivers in the MHz band

Vectrino Micro ADV Comparison

Robust Wideband Waveforms for Synthetic Aperture Radar (SAR) and Ground Moving Target Indication (GMTI) Applications

Robust Wideband Waveforms for Synthetic Aperture Radar (SAR) and Ground Moving Target Indication (GMTI) Applications

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EECS 121 FINAL EXAM

Microwave/Millimeter-wave Antenna Test System

Marine Mammal Acoustic Tracking from Adapting HARP Technologies

Method for the Generation of Broadband Acoustic Signals

Keywords Underwater Acoustic Communication, OFDM, STBC, MIMO

Laboratory Assignment 5 Amplitude Modulation

Microwave/Millimeter-wave Antenna Test System

Shallow Water Array Performance (SWAP): Array Element Localization and Performance Characterization

Implementation of Different Interleaving Techniques for Performance Evaluation of CDMA System

Comparative Analysis of Performance of Phase Coded Pulse Compression Techniques

The Potential of Synthetic Aperture Sonar in seafloor imaging

Waveform Multiplexing using Chirp Rate Diversity for Chirp-Sequence based MIMO Radar Systems

Smart antenna for doa using music and esprit

Implementation of Orthogonal Frequency Coded SAW Devices Using Apodized Reflectors

Acoustic Change Detection Using Sources of Opportunity

FPGA-BASED CONTROL SYSTEM OF AN ULTRASONIC PHASED ARRAY

DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited.

Text Book: Simon Haykin & Michael Moher,

Mobile Communications TCS 455

EVALUATION OF BINARY PHASE CODED PULSE COMPRESSION SCHEMES USING AND TIME-SERIES WEATHER RADAR SIMULATOR

UTILIZATION OF AN IEEE 1588 TIMING REFERENCE SOURCE IN THE inet RF TRANSCEIVER

Oceanographic Variability and the Performance of Passive and Active Sonars in the Philippine Sea


UWB for Lunar Surface Tracking. Richard J. Barton ERC, Inc. NASA JSC

Subsystems of Radar and Signal Processing and ST Radar

Sensor and Simulation Notes Note 548 October 2009

MULTI-CHANNEL SAR EXPERIMENTS FROM THE SPACE AND FROM GROUND: POTENTIAL EVOLUTION OF PRESENT GENERATION SPACEBORNE SAR

ADAPTIVE EQUALISATION FOR CONTINUOUS ACTIVE SONAR?

Phased Array Velocity Sensor Operational Advantages and Data Analysis

SPREAD SPECTRUM CHANNEL MEASUREMENT INSTRUMENT

A Modified Single Phase Inverter Topology with Active Common Mode Voltage Cancellation

Proceedings of Meetings on Acoustics

EC 2301 Digital communication Question bank

- 1 - Rap. UIT-R BS Rep. ITU-R BS.2004 DIGITAL BROADCASTING SYSTEMS INTENDED FOR AM BANDS

A High-Resolution, Four-Band SAR Testbed with Real-Time Image Formation

A New Scheme for Acoustical Tomography of the Ocean

Chapter 0. Overview. 0.1 Digital communication systems

Advanced Communication Systems -Wireless Communication Technology

Real Time Deconvolution of In-Vivo Ultrasound Images

Mutual Coupling Estimation for GPS Antenna Arrays in the Presence of Multipath

March, 2003 IEEE P /131r0. IEEE P Wireless Personal Area Networks

A Novel Transform for Ultra-Wideband Multi-Static Imaging Radar

TEST RESULTS OF A DIGITAL BEAMFORMING GPS RECEIVER FOR MOBILE APPLICATIONS

International Research Journal of Engineering and Technology (IRJET) e-issn: Volume: 03 Issue: 12 Dec p-issn:

Performance Analysis of Different Ultra Wideband Planar Monopole Antennas as EMI sensors

Progress Report. Mohammadtaghi G. Poshtmashhadi. Supervisor: Professor António M. Pascoal

3. Sound source location by difference of phase, on a hydrophone array with small dimensions. Abstract

Null-steering GPS dual-polarised antenna arrays

Noise Reduction for L-3 Nautronix Receivers

Rev 2.0 September 2010 Copyright Lecoeur Electronique corporation all rights reserved -

Practical Considerations for Radiated Immunities Measurement using ETS-Lindgren EMC Probes

Enhancing the capability of primary calibration system for shock acceleration in NML

Pulse Compression. Since each part of the pulse has unique frequency, the returns can be completely separated.

Radiation Analysis of Phased Antenna Arrays with Differentially Feeding Networks towards Better Directivity

Three-dimensional investigation of buried structures with multi-transducer parametric sub-bottom profiler as part of hydrographical applications

A NOVEL DIGITAL BEAMFORMER WITH LOW ANGLE RESOLUTION FOR VEHICLE TRACKING RADAR

QUESTION BANK EC 1351 DIGITAL COMMUNICATION YEAR / SEM : III / VI UNIT I- PULSE MODULATION PART-A (2 Marks) 1. What is the purpose of sample and hold

Research Article A Design of Wide Band and Wide Beam Cavity-Backed Slot Antenna Array with Slant Polarization

Chapter 4 Results. 4.1 Pattern recognition algorithm performance

(i) Determine the admittance parameters of the network of Fig 1 (f) and draw its - equivalent circuit.

3D radar imaging based on frequency-scanned antenna

DESIGN AND IMPLEMENTATION OF AN ALGORITHM FOR MODULATION IDENTIFICATION OF ANALOG AND DIGITAL SIGNALS

PLazeR. a planar laser rangefinder. Robert Ying (ry2242) Derek Xingzhou He (xh2187) Peiqian Li (pl2521) Minh Trang Nguyen (mnn2108)

A Prototype Wire Position Monitoring System

Passive Localization of Multiple Sources Using Widely-Spaced Arrays with Application to Marine Mammals

Keysight Technologies Pulsed Antenna Measurements Using PNA Network Analyzers

Simulating and Testing of Signal Processing Methods for Frequency Stepped Chirp Radar

Implementation of Adaptive and Synthetic-Aperture Processing Schemes in Integrated Active Passive Sonar Systems

Abstract. 1. Introduction

Passive Phase-Conjugate Signaling Using Pulse-Position Modulation

IMPLEMENTATION OF SOFTWARE-BASED 2X2 MIMO LTE BASE STATION SYSTEM USING GPU

Agilent Pulsed Measurements Using Narrowband Detection and a Standard PNA Series Network Analyzer

Transcription:

SIGNAL PROCESSING ALGORITHMS FOR HIGH-PRECISION NAVIGATION AND GUIDANCE FOR UNDERWATER AUTONOMOUS SENSING SYSTEMS Daniel Doonan, Chris Utley, and Hua Lee Imaging Systems Laboratory Department of Electrical and Computer Engineering University of California, Santa Barbara Santa Barbara, California 93106 ABSTRACT This paper presents an alternative approach to high-precision bearing estimation for navigation and guidance in homing and docking of underwater vehicles. This new technique is significantly simpler than the conventional methods in terms of computation complexity and yet produces results of superior precision and consistency. KEY WORDS Polarity estimation, bearing angle, homing and docking, navigation, geolocation. INTRODUCTION The key to the successful execution of autonomous imaging and sensing is the time synchronization and geolocation among the units. In particular, geolocation is an extremely challenging task. In underwater environments, the sensing, imaging, and communication signals are all within the acoustic range, which is more constrained in terms of available bandwidth, propagation speed, and serious multi-path interferences. This makes the geolocation a much more challenging and interesting research topic. Geolocation can be achieved by estimating the relative location with respect to a set of underwater base stations. In three-dimensional underwater geolocation, the objective parameters involved are the range distance and a two-dimensional bearing angle. Because of the multi-path interferences, the estimation of the polarity of the homing signal has been difficult. This paper introduces a new approach to the estimation of polarity with significantly improved accuracy and computational complexity. The presentation of this paper includes system 1

design, signal analysis, development of processing algorithms, and results from full-scale experiments. CONVENTIONAL TECHNIQUE FOR BEARING ESTIMATION As described, one of the key capabilities in mobile autonomous sensing is geolocation for navigation and guidance. This can be achieved by estimating the position of the sensor unit with respect to the underwater base stations. The locations of the underwater base stations are constantly estimated and updated with respect to the interface stations over the ocean surface, which is supported by the GPS systems and microwave mutual reference capability. Thus, the most critical element is the accuracy of a sensor s dynamic estimation of its relative location with respect to the underwater base stations. In three-dimensional underwater geolocation, the objective parameters involved include the range distance and a two-dimensional bearing angle. The focus of this proposed project is the highprecision estimation of the two-dimensional bearing angle for real-time navigation and guidance. Figure (1) is the three-element transmitter prototype for the base stations. With the three transmission elements, the transmitter sends a sequence of three waveforms. The first, from the top transducer element, is an in-phase reference signal. The second, from the middle transducer element, is a pair of signals with a left-right polarity with 180-degree phase offset for the estimation of the bearing angle in the horizontal direction. Similarly, the third signal from the bottom transducer is with a top-bottom polarity for the estimation of the bearing angle in the vertical direction. Figure (1): Three-element transmitter of the guidance system 2

Figure (2): Bearing-angle estimation with polarity errors As shown in Figure (1), the prototype transmission array consists of three transducer elements. At the top of the array, the square transducer element is designed to transmit the full reference signal s(t), which is used as the calibration waveform for bearing-angle estimation as well as the estimation of the range distance. The second transducer, in the middle, consists of two rectangular subelements, separated by a small gap. The two transducer elements are transmitting the same waveform s(t), but with different polarities. The signal detected by a sensor unit can be written in the form of, r x (t) = + [ s(t) s(t - t) ] The time difference _t is directly governed by the off-axis bearing angle. Larger bearing angles produce larger time delay t. When the sensor is moving along the central axis, the time delay term is zero, which results in a full cancellation and the received waveform is zero. This means the beam pattern gives a null along the central axis. This technique is theoretically sound. The fundamental concept is to identify the bearing angle through the accurate estimate of the time differential in the received signal. Yet, in practice, there are serious challenges. When the bearing angle is large, the received signal becomes weak due to the nature of the beam pattern. If the bearing angle is small, s(t) and s(t - t) start to overlap and cancel each other. The accuracy of the estimation of the bearing angle becomes increasingly difficult due to the decreased signal-to-noise ratio, especially in serious multi-path environment, which is common in underwater acoustic propagation. The conventional approach is to estimate the time differential by identifying the peak magnitude of the received signal r(t) and then the phase term at the peak, which indicates the polarity of the transmitted signal. Ideally, the estimate of the bearing angle is a monotonically increasing function. Figure (2) shows the result of the bearing angle estimation experiment with the conventional method. The horizontal axis is the bearing angle and the vertical 3

axis is the estimate. The ideal result is a monotonically increasing function. As it can be seen, accuracy of the estimates was limited and the estimation of the polarity of the signal is particularly challenging. ALTERNATIVE APPROACH Therefore, it is highly important and desirable to design and develop high-precision signal processing algorithms for accurate geolocation. The main objective of the polarity method is to accurately estimate the bearing angle of the source of the transmitted signals. Because the range distance can be determined through time delay estimation, the accurate estimation of the bearing angles will effectively complete the geolocation process, in the three-dimensional polar coordinate system, which is the key to underwater navigation and guidance. As described, the conventional technique conducts the estimation process based on the maximum of the received signal. That implies the entire result of the estimation process lies on one single data point. Noise and multi-path interferences can introduce serious errors. To optimize the accuracy of bearing-angle estimation, an alternative procedure is proposed. Prior to the estimation procedure, we first (a) decode the received signal and down shift it to the base band, (b) remove the negative sideband to obtain the single-sideband version, and (c) integrate the single-sideband signal. The combined transmitted signal can be represented alternatively in the form of a convolution of the designated waveform with two impulses with temporal offset, r(t) = s(t) * [ + (_(t) _(t _t))] After demodulation and matched filtering, the signal is in the form of _(t) = a ss (t) * [+(_(t) _(t - _t))] where a ss (t) is the auto-correlation of s(t). Then it can be seen that the most critical element for the polarity estimation is the second term of the equation. If we integrate the signal, it becomes where the gate function g(t) is _ 1 (t) = a ss (t) * [+ g(t)] g(t) = u(t) u(t _t) For positive polarity, the auto-correlation function a ss (t) will be convolving with +g(t) and g(t) for negative polarity. Since g(t) is non-negative and the point-like auto-correlation a ss (t) is real and even, the results of the integral gives an accurate estimate of the polarity. In addition, the duration of the 4

gate function is governed by _t, which is directly related to dsin_, where d is the separation of the transducer elements and _ is the bearing angle. Thus, the magnitude of the subsequent integration produces the estimate of the bearing. For performance evaluation purposes, the new method is applied to several data sets obtained form full-scale field tests. Multi-path interferences exist in these data sets and the conventional technique was unable to accurately estimate the signal polarity. Typically, the bearing angles of these data sets range from -30 to 30 degrees. To isolate the polarity estimation problem, the range distance was kept constant. As previously described, the received signals were first down shifted to the base band. The left-side band was removed to convert it to the single-side band version. A matched filter of s(t) was then applied to produce the time-delay profile. Subsequently, a double-integral procedure was applied to obtain the estimates of the polarity a well as the separation of signal pair. Figure (3) shows the results obtained by the new algorithm. The polarity estimation achieved 100% accuracy rate with a very high-degree of consistency. The estimation of the bearing also showed significant potential. With simple calibration procedure based on the beam patterns, this method can be fully implemented as a standard bearing estimation technique, not only for the accuracy of the estimation, but also the simplicity of the procedure for real-time processing. CONCLUSION In this paper, a simple algorithm was presented for the accurate estimation of the polarity of the transmitted signal for the underwater homing and docking systems. This new technique was successfully tested with several field-test data sets, which the conventional failed to achieve accurate estimation of the polarity. With extensions and modifications, for the accuracy and simplicity, this new technique can be implemented for real-time three-dimensional underwater navigation and guidance. Figure (3): Results of polarity estimation by using the new method 5

ACKNOWLEDGMENT This project is supported by Sonatech through the UC MICRO Program. REFERENCES (1) H. Lee and G. Wade, Imaging Technology. New York, New York: IEEE Press, 1986. (2) A. S. C. Wright, "The wide swath, deep towed seamarc," Oceans 88, pp. 323-328, 1988. (3) C. D. Loggins, "Advanced sonar imaging techniques," Advanced Techniques in the Processing of Active Sensor Data, 1987. (4) J. T. Christoff, C. D. Loggins, and E. L. Pipkin, "Measurement of the temporal phase stability of the medium," Journal of the Acoustical Society of America, vol. 71, no. 6, pp. 1606-1607, 1982. (5) J. C. Kirk, "Motion compensation for synthetic aperture radar," IEEE Transactions on Aerospace and Electronic Systems, vol. AES- 11, no. 3, 1975. (6) B. L. Douglas and H. Lee, "Synthetic aperture active sonar imaging," Proceedings of the 1992 International Conference on Acoustics, Speech, and Signal Processing, vol. 3, pp. 37-40, 1992. (7) J. C. Curlander and R. N. McDonough, Synthetic Aperture Radar. New York, New York: John Wiley & Sons, 1991. (8) H. Lee and G. Wade, Modern Acoustical Imaging, IEEE Press, New York, 1986. (9) C. Dorme and M. Fink, Matched Filter Imaging Through Inhomogeneous Media, Acoustical Imaging, Vol. 22, Plenum Press, pp. 1-8, 1996. 6