Communications – electrical: acoustic wave systems and devices – Echo systems – Speed determination
Reexamination Certificate
2000-11-15
2001-11-06
Lobo, Ian J. (Department: 3662)
Communications, electrical: acoustic wave systems and devices
Echo systems
Speed determination
C367S089000, C367S091000
Reexamination Certificate
active
06314053
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to processes for detecting moving underwater objects by means of an active sonar, comprising a directional antenna, by using the Doppler effect attached to the relative movement of the object and of the sonar and by forming directional channels on the basis of the signals from the transducers of the antenna.
2. Discussion of the Background
In order to detect a moving object, called, target a with a sonar, it is known practice to use the Doppler effect produced by the movement of the target. In such processes of the prior art, a pulse of narrow bandwidth compared with the Doppler shift from the target is transmitted, then on reception, the received signals are simultaneously correlated with several frequency-shifted copies of the transmitted pulse. Each correlation copy corresponds to a different possible Doppler shift. The best correlation is obtained with a copy having a frequency shift approximately equal to that caused by the movement of the target. Thus, the correlation by many copies and the use of the signals received make it possible to locate a target by distance and by azimuth and to calculate its radial velocity.
This process amounts to transmitting a bandwidth code which is narrower than the Doppler shift from the targets that one is seeking to detect. To do this, the transmission consists of a pulse of pure frequency f
0
and duration T, amplitude-weighted in order to reduce the level of the secondary lobes of the spectrum transmitted so as to obtain good spectral rejection. The spectral width of such a pulse is then about 4/T for a cos
2
weighting.
It is known that the marine environment is reverberant, especially because of the many local heterogeneities (air bubbles, particles, plankton, etc.) forming scatterers. In addition, at shallow depths, the reverberation coming from the bottom and from the surface is significant. It follows that, when the spectrum of the reverberated signal and the spectrum of the copy are superimposed in the angular sector corresponding to the main lobe of the antenna, the detection performance is very poor.
FIG. 1
shows the value of the frequency f of the signal received as a function of the cosine of the angle &thgr; between the velocity vector of the sonar carrier and the direction of a point in space in the bearing plane.
As the carrier moves with a uniform velocity V and as the transmitted frequency is f
0
, it is known that the received frequency is given by (1+2|V|/c cos &thgr;)f
0
where c is the speed of the acoustic waves in the water. The spread of the spectrum of the signal reverberated by the entire volume subjected to the sound is therefore represented by a sloping straight line
101
of width 4/T. As to the copy, this is independent of &thgr; and is shown by a vertical straight line
102
of width 4/T.
The region denoted A corresponds to the reverberation case indicated above. In this region, the reverberated signal is received in the main receiving lobe
103
. It is not removed either by the directivity, nor by the Doppler filtering.
The regions denoted B correspond to the case in which the spectrum of the reverberated signal and that of the copy are superimposed opposite the secondary lobes
104
of the receiving channel. There are therefore two contributions to the reverberated intensity detected. The first is that of the scatterers in the main lobe of the receiving channel, but at frequencies different from the target. These scatterers are rejected by spectral analysis. As the latter can reach 40 to 50 dB in sonar, this contribution can be ignored. A second contribution corresponds to the scatterers at the same frequency as the target, but attenuated by the secondary lobes of the directivity pattern. The situation in the figure shows the intersection
105
of the straight lines
101
and
102
with the secondary lobe
106
.
The “reverberation/signal” ratio is given by the formula:
R
⁢
.2
⁢
Δθ
⁢
c
⁢
⁢
T
2
⁢
.10
-
N
⁢
⁢
S
10
(
1
)
where R is the distance from the target and NS is the level in dB of the secondary lobes of the directivity pattern.
The angular interval &Dgr;&thgr; corresponding to the spectral overlap between the copy and the reverberated signal is such that &Dgr; cos &thgr;=&lgr;/VT and the ratio (1) does not depend on the duration T of the transmitted pulse: the fact of increasing this duration would not allow the performance to be increased.
The regions denoted C correspond to the case in which there is no scatterer at the frequency of the receiving channel. In this case, the performance is generally very good, but it only corresponds to a limited number of potential targets.
Patent application Ser. No. 92/01499, filed on Feb. 11, 1992 by the Thomson-CSF company and published on Aug. 13, 1993 under U.S. Pat. No. 2,687,226 describes a process for detecting moving targets in which a series of pulses at pure frequencies is transmitted. Its drawbacks stem from the fact that the performance in regions B remain poor and that the transmitted frequencies depend on the speed of the target.
SUMMARY OF THE INVENTION
In order to be able to obtain good performance equally in the A and B regions, while retaining the performance of the C regions, the invention proposes a process for detecting moving objects by an active sonar moving at a velocity V, in which a signal of duration T is transmitted, which signal is reverberated by the transmission medium, presenting a spectral spread due to the actual speed of the sonar and this reverberated signal is processed by correlation with a set of the frequency-shifted copies of the transmission signal in order to correspond to the set of Doppler shifts capable of affecting the reverberated signal, mainly characterized in that the transmitted signal is broadband encoded in order to present a spectrum having a comb-of-lines structure at successive frequencies f
i
, the interval separating two successive lines f
i
and f
i+1
of which is a function of the velocity V in order to be at least equal to the spectrum spread by satisfying the formula:
(
1
-
2
⁢
V
c
)
⁢
f
i
+
1
-
a
T
≥
(
1
+
2
⁢
V
c
)
⁢
f
i
+
a
T
where a is an integer between 1 and 2.
According to another characteristic, the encoded signal is formed by N pulses, each of which occupies a frequency band B centered on a frequency f
0
, where N is greater than or equal to:
N
≅
4
⁢
V
⁢
⁢
T
c
⁢
(
f
0
+
B
2
)
.
According to another characteristic, the transmission signal furthermore comprises two pulses at pure frequences f
m
and f
M
intended to make it possible to detect fast moving objects, the echoes from which are located beyond the frequency band occupied by the reverberated signal both when receding and when approaching, these frequencies being given by the equations:
(
1
+
2
⁢
V
c
+
2
⁢
&LeftBracketingBar;
V
c
max
&RightBracketingBar;
c
)
⁢
f
m
+
2
T
≤
(
1
-
2
⁢
V
c
)
⁢
f
1
-
2
T
⁢
⁢
and
⁢


(
1
+
2
⁢
V
c
)
⁢
f
1
+
2
T
≤
(
1
-
2
⁢
V
c
+
2
⁢
&LeftBracketingBar;
v
c
max
&RightBracketingBar;
c
)
⁢
f
M
-
2
T
.
According to another characteristic, in order for the moving objects, whose speed is approximately equal to one of the blind speeds of the broadband encoded signals, to be detected by the pure-frequency signals, the frequencies f
m
and f
M
are chosen to satisfy, in addition, the equations:
f
M
=
q
⁢
N
T
⁢
⁢
and
⁢
⁢
f
m
=
(
p
±
Δ
2
)
⁢
N
T
where &Dgr; corresponds to the smallest interval separating the arithmetic series of the p/q ratio from the series of integers.
According to another characteristic, a process is used in which f
m
and f
M
are chosen so as to satisfy the equations:
{
(
1
+
2
⁢
V
c
)
⁢
f
1
+
2
T
≤
(
1
-
2
⁢
V
c
-
2
⁢
&LeftBracketingBar;
V
c
max
&RightBracketingBar;
c
)
⁢
f
m
-
2
T
(
1
+
2
⁢
V
c
)
⁢
f
1
+
2
T
≤
(
1
-
2
⁢
V
c
-
2
&it
Doisy Yves
Metivier Pierre
Lobo Ian J.
Oblon & Spivak, McClelland, Maier & Neustadt P.C.
Thomson Marconi Sonar SAS
LandOfFree
Method for detecting mobile objects with active sonar does not yet have a rating. At this time, there are no reviews or comments for this patent.
If you have personal experience with Method for detecting mobile objects with active sonar, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Method for detecting mobile objects with active sonar will most certainly appreciate the feedback.
Profile ID: LFUS-PAI-O-2606017