Effects of a Suspended Bottom Boundary Layer on Sonar Propagation Michael Cornelius June 2004.
-
Upload
lesley-simmons -
Category
Documents
-
view
216 -
download
0
Transcript of Effects of a Suspended Bottom Boundary Layer on Sonar Propagation Michael Cornelius June 2004.
Effects of a Effects of a Suspended Bottom Suspended Bottom Boundary Layer on Boundary Layer on Sonar PropagationSonar Propagation
Michael CorneliusMichael Cornelius
June 2004June 2004
PurposePurpose
Determine the impact of a Determine the impact of a suspended bottom boundary layer suspended bottom boundary layer on the reverberation on the reverberation characteristics of a simulated minecharacteristics of a simulated mine
Determine critical value of volume Determine critical value of volume attenuation that renders mine attenuation that renders mine object undetectableobject undetectable
RelevanceRelevance
Mine WarfareMine Warfare Future investigation of bottom Future investigation of bottom
boundary layers on acoustic boundary layers on acoustic detectiondetection
Mine WarfareMine Warfare
CASS/GRABCASS/GRAB Comprehensive Acoustic Comprehensive Acoustic
Simulation System (CASS)Simulation System (CASS) Gaussian Ray Bundle (GRAB) Gaussian Ray Bundle (GRAB)
Eigenray modelEigenray model Navy standard model for active Navy standard model for active
and passive range dependent and passive range dependent acoustic propagation, acoustic propagation, reverberation and signal excessreverberation and signal excess
Frequency range 600Hz to 100 kHzFrequency range 600Hz to 100 kHz
CASS/GRAB Model CASS/GRAB Model DescriptionDescription
The CASS model is the The CASS model is the range dependent range dependent improvement of the Generic improvement of the Generic Sonar Model (GSM). CASS Sonar Model (GSM). CASS performs signal excess performs signal excess calculations.calculations.
The GRAB model is a subset The GRAB model is a subset of the CASS model and its of the CASS model and its main function is to compute main function is to compute eigenrays and propagation eigenrays and propagation loss as inputs in the CASS loss as inputs in the CASS signal excess calculations.signal excess calculations.
CASSComprehensive Acoustic
System Simulation
Propagation Model 1: FAME
Propagation Model 3: COLOSSUSPropagation Model 4: AMOS equations
Backscatter ModelsReverberationNoise Models
Signal to NoiseSignal Excess
Graphic DisplaysSystem Parameters (Beamforming)
Propagation Model 2: GRAB Gaussian Ray Bundle OAML GRAB v1.0
Environmental Interpolations Environmental Model Interpolations Surface and Bottom Forward Loss Volume Attenuation Sound Speed Algorithms Call GRAB
Comprehensive Acoustic Comprehensive Acoustic Simulation Simulation
System/Guassian Ray System/Guassian Ray Bundle (CASS/GRAB)Bundle (CASS/GRAB)
In the GRAB model, the travel time, source angle, target In the GRAB model, the travel time, source angle, target angle, and phase of the ray bundles are equal to those angle, and phase of the ray bundles are equal to those values for the classic ray path. values for the classic ray path.
The main difference between the GRAB model and a classic The main difference between the GRAB model and a classic ray path is that the amplitude of the Gaussian ray bundles ray path is that the amplitude of the Gaussian ray bundles is global, affecting all depths to some degree whereas is global, affecting all depths to some degree whereas classic ray path amplitudes are local. GRAB calculates classic ray path amplitudes are local. GRAB calculates amplitude globally by distributing the amplitudes according amplitude globally by distributing the amplitudes according to the Gaussian equationto the Gaussian equation
,
,
exp . ( ) /0
22
205
p rz z
r
Klein 5000 SonarKlein 5000 Sonar
Klein specifics: Klein specifics: 455 KHz455 KHz
5 beams per side5 beams per side
Resolution: 20cm@75mResolution: 20cm@75m
36cm@150m36cm@150m
Can be towed at 15ktsCan be towed at 15kts
Source Level 240dBSource Level 240dB
Klein 5000 SonarKlein 5000 Sonar
Image From Klein 5000Image From Klein 5000Image: X=50.462m
Y=61.672mSilty clay bottom
Object: 5m x 3m x 2mAssumed Steel
X= 30m Y= 28m
Bathymetric DataResolution- 3m in Y 2.5m in X
Image From Klein 5000Image From Klein 5000Sonar: Depth 30.4m
Range of Depths:
95m-77m
Sound Velocity ProfileSound Velocity ProfileSound Velocity Profile
-100
-90
-80
-70
-60
-50
-40
-30
-20
-10
0
1508 1510 1512 1514 1516 1518 1520 1522
Sound Speed (m/s)
De
pth
(m
)
Bottom Type Geoacoustic Bottom Type Geoacoustic PropertiesProperties
Suspended sediment layer Suspended sediment layer changes the volume scattering changes the volume scattering strength, …strength, …
CASS/GRAB Input CASS/GRAB Input ParametersParameters
Bottom depthBottom depth Target depthTarget depth Transducer depthTransducer depth Wind speedWind speed Bottom type grain Bottom type grain
size indexsize index Frequency min/maxFrequency min/max Self noiseSelf noise
Source levelSource level Pulse lengthPulse length Target strength/depthTarget strength/depth Transmitter tilt angleTransmitter tilt angle Surface scattering Surface scattering
/reflection model/reflection model Bottom scattering Bottom scattering
/reflection model/reflection model
Difference in Input FilesDifference in Input Files
1. Normal Bathymetry- No Synthetic Mine1. Normal Bathymetry- No Synthetic Mine 41 files, batch file, 41 files, batch file, PlotCASSReverb_all.mPlotCASSReverb_all.m
WorkingwithoutWorkingwithout2. Altered Bathymetry- Mine inserted2. Altered Bathymetry- Mine inserted
1-17 same, 17-22 mine, 22-41 same1-17 same, 17-22 mine, 22-41 same WorkingWorking3. Altered Bathymetry-Mine inserted3. Altered Bathymetry-Mine inserted Bottom Boundary Layer PresentBottom Boundary Layer Present WorkingwithlayerWorkingwithlayer
Input Type 1Input Type 1Normal Bathymetry-No MineNormal Bathymetry-No Mine
Input Type 2Input Type 2Altered Bathymetry- MineAltered Bathymetry- Mine
Adding LayerAdding Layer
• Object in 87 meters of water• Approx. 2 meters high• Layer inserted at 78 meters
Suspended Bottom Boundary Suspended Bottom Boundary LayerLayer
VOLUME SCATTERING STRENGTH TABLE
M DB//M 0.00 -95.00 77.00 -95.00 78.00 -65.00 95.00 -65.00 EOT
Acoustic impact of bottom Acoustic impact of bottom suspended layer is to increase the suspended layer is to increase the volume scattering strength (XXXX, volume scattering strength (XXXX, 199x), 199x),
Increase of the volume scattering Increase of the volume scattering strength -> increase of the strength -> increase of the volume reverberationvolume reverberation
Input Type 3 Input Type 3 Altered Bathymetry- Mine-Layer Altered Bathymetry- Mine-Layer
(-30 dB/m)(-30 dB/m)
Input Type 3Input Type 3Altered Bathymetry- Mine-Layer Altered Bathymetry- Mine-Layer
(-27 dB/m)(-27 dB/m)
Input Type 3Input Type 3Altered Bathymetry- Mine-LayerAltered Bathymetry- Mine-Layer
(-22 dB/m)(-22 dB/m)
ConclusionsConclusions
A side scan sonar image can be A side scan sonar image can be represented through reverb represented through reverb characteristics.characteristics.
Labor intensive changing of input Labor intensive changing of input files.files.
Critical values of Volume Scattering Critical values of Volume Scattering Strength for this situation were -30 to Strength for this situation were -30 to
-22 dB/m-22 dB/m
Where to Next?Where to Next?
Finer resolution and a more Finer resolution and a more complex object could produce complex object could produce more useful results.more useful results.
Field measurements of layer to Field measurements of layer to limit assumptions.limit assumptions.
Impact of layer on SVP and Volume Impact of layer on SVP and Volume Attenuation?Attenuation?