Broadband LFM signal source for a module-based diver detection sonar
BROADBAND LFM SIGNAL SOURCE FOR A MODULE-BASED
DIVER DETECTION SONAR
KRZYSZTOF ZACHARIASZ*, WALDEMAR LIS*,
ANDRZEJ ELMINOWICZ**
* Gdansk University of Technology, Faculty of Electronics, Telecommunications
and Informatics, Department of Marine Electronic Systems
Narutowicza 11/12, 80-233 GdaĔsk Poland
,
**OBR Centrum Techniki Morskiej S.A.
Dickmana 62, 81-109 Gdynia, Poland
A new approach to design of the diver detection sonar’s sounding pulse source is presented. It is based on modules comprising 8 or 16 elements of the transducer grouped on the
transmitting channel. The basic advantage of this solution is that it reduces significantly the
number of group transmitters. The required output power and topology of the transmitters
were determined through theoretical estimation and measurements in a four terminal network.
Measurements were taken of the frequency characteristics in the transducer modules including the compensation system used. It is demonstrated that the source level is most irregular in
the transducer under examination when the transducer’s voltage has a constant amplitude,
i.e. with parallel compensation. It is also demonstrated that by appropriately selecting elements for a series compensation of the transducer, the frequency characteristics becomes
more regular and source level is increased at the extreme ends of the working bandwidth. The
result is a compensated characteristics on the receiving side.
INTRODUCTION
In recent years the threat of terrorism has led to the launch of a number of initiatives designed to improve the security of marine sites, in particular sea ports, anchorages and offshore facilities. Underwater security relies on active and passive sonars for the detection of
divers, small underwater vehicles and submerged diver delivery vehicles. The sonars are
manufactured by a number of companies worldwide.
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Installed at the Polish Navy Port, the Active Stationary Sonar [1] has been in operation
for several years with very good results. It was built by OBR CTM in a project called KRYL.
The company is currently working on a new generation modular sonar [2] for the detection of
underwater objects in ports and anchorages. Its special feature is that it can be adapted to the
geometry of the site it is surveilling (the shape of the pool, configuration of the quays and
breakwaters and the type of bottom). The sonar is easy to install, portable or stationary, can be
installed on quays, ships and in open bodies of water. It is protected from disturbances and
changing conditions of sound propagation. One of the research problems the project is addressing is the development of methods for integrating sonars and modules of acoustic barriers. The objective is to build a cost effective and efficient system of underwater security
which can successfully operate in a variety of large-scale sites and ensure that mutual disturbances and reverberation levels are kept to a minimum.
Because sonar parameters must be changed in a wide range (especially the observation
sector), a module-based design is required. Modules are primarily used in the transducer,
transmitter, receiver and signal processing. The number and type of modules in the sonar depend solely on the parameters of the site and its conditions. Special software is used to connect the modules.
1. SONAR CHARACTERISTICS
The diver detection sonar (DDS) uses a broadband piezzocomposite transducer [3] a
product of a US-based company MSI. It has 128 transmit-receive sections placed on the side
of a cylindrical casing. Vertical beam pattern has a constant width at 12° because it operates in
shallow waters. The horizontal width of the sounding beam and its orientation, however, must
be adapted flexibly to the geometry of the area under surveillance.
To build a modular structure of the sonar’s source of transmitting pulses, the elementary
sections of the transducer are grouped (on the transmitting side) into modules operated by individual group transmitters. With this structure it is easy to configure that part of the array
which is excited. The operation of the individual transmitters within the group can be easily
controlled by low voltage settings made in the main level system.
The dimensions of the transducer module determine the minimal angle by which the
transmit sector width and position can be changed. The sector’s highest level of precision is
achieved with single section modules. This, however, would require a 128 channel transmitter.
While the stroke angle for 8 or 16 element modules is wider, it is still acceptable (22.5° or
45°). This structure is matched by lower numbers of group transmitters (16 or 8) but with
a higher output power.
The ease of observation sector changes is not the only factor speaking in favour of the
modular design of the sonar’s transmitting channel. It was also important to consider whether
the following can be corrected depending on the size of the module:
• dispersion of the transmit patterns for the elementary sections of the transducer;
• irregularity of the frequency characteristics in the working bandwidth.
The need for correcting the characteristics became apparent from the results of measurements taken by the manufacturer of the transducer. They showed (Fig.1) significant fluctuation of source level SL in the sections with some as high as 8 dB in the middle of the working
bandwidth.
270
148
146
SL[dB]
144
142
140
138
136
0
8
16
24
32
40
elements number
48
56
64
Fig.1. Spread of source level SL [dB ref. 1µP/V/1m] for 64 array elements
The dispersion of source level can be corrected separately for each section using single
element transmit modules. But this is not necessary because the beam patterns of the transducer’s elementary sections are wide and for the practical widths of the scan sector many adjacent sections have to be excited (40 for a 90° sector). This leads to averaging on the acoustic
side. As a result, even if non-identical sections are connected in parallel – just like in a multiple elements module - the beam pattern is slightly smoothened out. Its shape and level of ripple resemble that of the theoretical pattern which was obtained for identical elements. This is
confirmed by the results of measurements taken by MSI, as seen in Fig.2.
170
SL [dB]
160
150
140
130
120
-100
-75
-50
-25
0
25
50
75
100
Angle[deg]
Fig.2. Horizontal transmit beam patterns for a 16 element module of the cylindrical transducer
Figure 3 shows the irregularity of the frequency characteristics. As you can see the drop in
SL at the edges of the working bandwidth (60÷80kHz) reaches 6 dB. A similar irregularity is
seen in the receiving sensitivity which adds up to the drop of 12 dB for the transmit-receive
frequency characteristics.
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170
b
160
S L [dB ]
c
150
a
140
130
50
60
70
80
90
100
f[kH z ]
Fig.3. Normalized source level SL in the frequency function for a single element (a) and modules with
8 (b) and 16 (c) elements
The decr (...truncated)