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Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA [email protected]

Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA [email protected]

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Page 1: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Advanced Acoustical Modeling Tools for ESME

Martin Siderius and Michael Porter Science Applications Int. Corp.

10260 Campus Point Dr., San Diego, CA [email protected]

[email protected]

Page 2: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Acoustic Modeling Goals

Through modeling, try to duplicate sounds heard by marine mammals (e.g. SONAR, shipping)

Develop both high fidelity and very efficient simulation tools

Page 3: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Acoustic Modeling Goals• Accurate field predictions in 3 dimensions• Computational efficiency (i.e. fast run times)• Propagation ranges up to 200 km• R-D bathymetry/SSP/seabed with depths 0-5000 m• Frequency band 0-10 kHz (or higher)• Moving receiver platform• Arbitrary waveforms (broadband time-series)• Directional sources

Difficult task for any single propagation code

Approach is to use PE, Rays and Normal Modes

Page 4: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Model Comparisons

Frequency

Com

puta

tion

Tim

e

Rays

NM and PE

Frequency

Acc

urac

yRays

NM and PE

Page 5: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Motivation

Page 6: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Fast Coupled NM Method

• Range dependent environment is treated as series of range independent sectors

• Each sector has a set of normal modes• Modes are projected between sectors allowing for

transfer of energy between modes (matrix multiply)• Algorithm marches through sectors • Speeds up in flat bathymetry areas• Pre-calculation of modes allows for gains in run-

time (important for 3D calculation)• Very fast at lower frequencies and shallow water

Page 7: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Mid Atlantic Bight: Example

Page 8: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com
Page 9: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Mammal Risk Mitigation Map

SD = 50 m

SL = 230 dB

Freq = 400 Hz

Lat = 49.0o N

Long = 61.0o W

5 dB more loss5 dB less loss

Page 10: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Shipping Simulator

• Using the fast coupled normal-mode routine shipping noise can be simulated

• This approach can rapidly produce snapshots of acoustic data (quasi-static approximation)

• Self noise can also be simulated (i.e. on a towed array)

• Together with a wind noise model this can predict the background ambient noise level

Page 11: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Example: Simulated BTR• Input environment, array geometry (e.g. towed

array hydrophone positions) and specify ship tracks (SL, ranges, bearings, time)

Page 12: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Example: BTR from SWELLEX96

Page 13: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Computing Time-Series Data for Moving Receiver

1. How is the impulse response interpolated between grid points?

2. How are these responses “stitched” together?

Page 14: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

1. Interpolating the Impulse Response

• In most cases the broad band impulse response cannot be simply interpolated

• For example, take responses from 2 points at slightly different ranges:

Page 15: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

2. “Stitching” the Responses Together

• Even if the impulse response is calculated on a fine grid, there can be glitches in the time-series data (due to discrete grid points)

• For example, take the received time-series data at points 1 m apart:

Page 16: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Solution: Interpolate in Arrival Space

• The arrival amplitudes and delays can be computed on a very course grid and since these are well behaved, they can be interpolated for positions in between.

• Using the “exact” arrival amplitudes and delays at each point, the convolution with the source function is always smooth.

Page 17: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Ray/Beam Arrival Interpolation

Endpoint #1

Endpoint #2

Interpolated

j

ttij

jeAzrp )(),,( Advantage: very fast and broadband

Page 18: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Test Case: Determine Long Time Series Over RD Track

• Source frequency is 3500 Hz

• Source depth is 7 m

• Environment taken from ESME test case

• Receiver depth is 7-100 m

• Receiver is moving at 5 knots

Page 19: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

TL

Page 20: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Received Time-Series

Page 21: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Received Time-Series

Page 22: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Received Time-Series (with Source Functions)

Page 23: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Computing TL Variance

• Fast Coupled Mode approach allows for:– TL computations in 3D (rapid enough to

compute for several environments)– Changing source/receiver geometry

• Ray arrivals interpolation allows for Monte-Carlo simulations of TL over thousands of bottom types to arrive at TL variance

Page 24: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Ray/Beam Arrival Interpolation

Endpoint #1

Endpoint #2

Interpolated

j

ttij

jeAzrp )(),,( Advantage: very fast and broadband

Page 25: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Does it work? TL example

• 100-m shallow water test case:– Source depth 40-m– Receiver depth 40-m– Downward refracting sound speed profile– 350 Hz

• 3 parameters with uncertainty:– Sediment sound speed 1525-1625 m/s– Sediment attenuation 0.2-0.7 dB/– Water depth 99-101 m

Page 26: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

Does it work? TL example

Interpolated (red) is about 100X faster than calculated (black)

Page 27: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

TL Variance

Page 28: Advanced Acoustical Modeling Tools for ESME Martin Siderius and Michael Porter Science Applications Int. Corp. 10260 Campus Point Dr., San Diego, CA sideriust@saic.com

TL Variance