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Introduction to Acoustics

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a fac<strong>to</strong>r when there is a reverberant environment and<br />

when one is concerned with estimating target range<br />

and Doppler. A waveform’s potential for range and<br />

Doppler resolution can be ascertained from the ambiguity<br />

function of the transmitted signal. This ambiguity<br />

function is related <strong>to</strong> the correlation process of (5.90)<br />

for a transmitted signal scanned as a function of range<br />

and Doppler,<br />

Θ( ˆT, Tt, fd, ˆ fdt )<br />

��<br />

�<br />

∝ �<br />

� ˜s(t − T)˜st(t − ˆT)e 2πi( fdt − �<br />

fd)t ˆ �2<br />

dt�<br />

� , (5.91)<br />

where Tt and fdt are the true target range (time) and<br />

Doppler, and ˆT and fd ˆ are the scanning estimates of the<br />

range and Doppler. Figure 5.43 are sketches of ambiguities<br />

functions of some typical waveforms. The range<br />

resolution is determined by the reciprocal of the bandwidth<br />

and the Doppler resolution by the reciprocal of<br />

the duration. A coded or pseudo-random (PR) sequence<br />

can attain good resolution of both by appearing as<br />

long-duration noise with a wide bandwidth. Ambiguity<br />

functions can be used <strong>to</strong> design desirable waveforms for<br />

particular situations. However, one must also consider<br />

the randomizing effect of the real ocean. The scattering<br />

function describes how a transmitted signal statistically<br />

redistributes its energy in the reverberant ocean environment<br />

which causes multipath and Doppler spread. In<br />

particular, in a reverberation-limited environment, only<br />

increasing the transmitted power does not change the<br />

signal-<strong>to</strong>-reverberation level. Signal design should minimize<br />

the overlap of the ambiguity function of the target<br />

displaced <strong>to</strong> its range and Doppler and the scattering<br />

function.<br />

5.7.2 Underwater Acoustic Imaging<br />

Imaging can be divided in<strong>to</strong> categories concerned with<br />

water column and bot<strong>to</strong>m properties. Here we describe<br />

several applications of active SONAR <strong>to</strong> imaging the<br />

ocean.<br />

Water Column Imaging. Backscatter from particulate<br />

objects that move along with the water motion (such as<br />

biological matter, bubbles sediments) contains velocity<br />

information because of the Doppler shift. An acoustic<br />

Doppler current profiler (ADCP) might typically consist<br />

of three or four source–receivers pointed in slightly different<br />

directions but generally up (from the bot<strong>to</strong>m) or<br />

down (from a ship). The multiple directions are for resolving<br />

motion in different directions. The Doppler shift<br />

a)<br />

b)<br />

c)<br />

T Ù<br />

T Ù<br />

T Ù<br />

Underwater <strong>Acoustics</strong> 5.7 Active SONAR Processing 187<br />

Fig. 5.43a–c Ambiguity function for several SONAR signals:<br />

(a) rectangular pulse; (b) coded pulses; (c) chirped FM<br />

pulse<br />

of the returning scattered field is simply −2 f (v/c) (as<br />

opposed <strong>to</strong> the more-complicated long-range waveguide<br />

Doppler shift discussed in Sect. 5.4.4), where f is the<br />

acoustic frequency, v is the radial velocity of the scatterer<br />

(water motion), and c is the sound speed. With three<br />

or four narrow-beam transducers, the current vec<strong>to</strong>r can<br />

be ascertained as a function of distance from an ADCP<br />

by gating the received signal and associating a distance<br />

with the time gated segment of the signal. Water-column<br />

motion associated with internal waves can be determined<br />

by this process also where essentially one uses a kind<br />

of ADCP points in the horizontal direction. For elab-<br />

f Ù<br />

d<br />

f Ù<br />

d<br />

f Ù<br />

d<br />

Part A 5.7

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