Acoustic backscatter from a single target or organism is expressed as
the intensity of an echo typically denoted as the backscattering
cross-section (σbs, m2). Target strength (TS, dB
re. 1 m2) is the logarithmic representation of σbs
where: TS = 10 log10 (σbs). TS can be used to
convert integrated (e.g. nautical area scattering coefficient,
SA, dB re. 1(m2 nmi-2) or volumetric
backscatter (e.g. Sv, dB re. 1 m-1) collected from
fisheries acoustic surveys into units of number density, such as the
volumetric density of a fish school (i.e. animals m-3). This
parameter can also aid in classifying backscatter based on the
multifrequency response of targets, such as separating likely echoes of
large predatory fish from smaller prey. While there are several
approaches for estimating TS, one common method is to apply
physics-based models to predict theoretical TS that comprise exact and
approximate solutions. The models provided in the acousticTS
package
can help provide TS estimates parameterized using broad statitsical
distributions of inputs. This package is in a constant state of
development with updates to the available model library, computational
efficiency, and quality-of-life improvements.
Latest release DOI https://doi.org/10.5281/zenodo.7600659
You can install the current released version of acousticTS via:
devtools::install_github("brandynlucca/acousticTS")
Or you can install the development version of acousticTS like so:
devtools::install_github("brandynlucca/acousticTS@test-branch")
Stanton, T.K., Clay, C.S., and Chu, D. (1993). Ray representation of sound scattering by weakly scattering deformed fluid cylinders: Simple physics and application to zooplankton. J. Acoust. Soc. Am., 94, 3454-3462.
Stanton, T.K., Chu, D., and Wiebe, P.H. (1998). Sound scattering by several zooplankton groups. II. Scattering models. J. Acoust. Soc. Am., 103, 236-253.
Demer, D.A., and Conti, S.G. 2003. Reconciling theoretical versus empirical target strengths of krill: effects of phase variability on the distorted-wave Born approximation. ICES J. Mar. Sci., 60, 429-434.
Demer, D.A., and Conti, S.G. 2003. Reconciling theoretical versus empirical target strengths of krill: effects of phase variability on the distorted-wave Born approximation. ICES J. Mar. Sci., 60, 429-434.
Stanton, T.K., Chu, D., and Wiebe, P.H. (1998). Sound scattering by several zooplankton groups. II. Scattering models. J. Acoust. Soc. Am., 103, 236-253.
Clay C.S. and Horne J.K. (1994). Acoustic models of fish: The Atlantic cod (Gadus morhua). J. Acoust. Soc. Am., 96, 1661-1668.
Anderson, V.C. (1950). Sound scattering from a fluid sphere. J. Acoust. Soc. Am., 22, 426-431.
MacLennan D. N. (1981). The theory of solid spheres as sonar calibration targets. Scottish Fisheries Research No. 22, Department of Agriculture and Fisheries for Scotland.
Below are examples of different models used to predict TS for a sardine with a gas-filled swimbladder, a tungsten carbide calibration sphere, a crustacean modeled as a prolate spheroid, and a generic gas-filled bubble.
library( acousticTS )
##
## Attaching package: 'acousticTS'
## The following object is masked from 'package:base':
##
## kappa
### Call in the built-in sardine shape dataset
data( sardine )
### Inspect the object
print( sardine )
## SBF-object
## Fluid-like scatterer
## ID: Sardinops sagax caerulea (Conti and Demer, 2003)
## Body dimensions:
## Length: 0.21 m (n = 379 cylinders)
## Mean radius: 0.0097 m | Max radius: 0.0133 m
## Bladder dimensions:
## Length: 0.085 m (n = 154 cylinders)
## Mean radius: 0.0048 m | Max radius: 0.0078 m
## Body material properties:
## Density: 1070 kg m^-3 | Sound speed: 1570 m s^-1
## Bladder fluid material properties:
## Density: 1.24 kg m^-3 | Sound speed: 345 m s^-1
## Body orientation (relative to transducer face/axis): 1.571 radians
plot( sardine )
### We will now define a frequency range to predict TS over
frequency <- seq( 1e3 , 400e3 , 1e3 )
### And now we use the target_strength(...) function to model TS for this fish
sardine <- target_strength( sardine,
frequency = frequency,
model = "KRM" )
## KRM model for SBF-object: Sardinops sagax caerulea (Conti and Demer, 2003) initialized.
### Plot results
plot( sardine, type = 'model' )
### Extract model results
sardine_ts <- extract( sardine , "model") $KRM
### Let's create a calibration sphere
### Default inputs here are a 38.1 mm diameter and a tungsten carbide
### (WC) material properties.
cal_sphere <- cal_generate( )
### We will use the same frequency range as the previous example
### Calculate TS
cal_sphere <- target_strength( object = cal_sphere,
frequency = frequency,
model = "calibration" )
## CALIBRATION model for CAL-object: Calibration sphere initialized.
### Plot results
plot( cal_sphere , type = 'model' )
### Extract model results
calibration_ts <- extract( cal_sphere , "model" )$calibration
### Let's create a gas-filled bubble with a raidus of 4 mm
### This defaults to a density contrast, g_body, of 0.0012
### This defaults to a soundspeed contrast, h_body, of 0.220
bubble <- gas_generate( radius = 4e-3 ,
ID = "gas bubble" )
print( bubble )
## GAS-object
## Gas- and fluid-filled scatterer
## ID: gas bubble
## Body dimensions:
## Diameter: 0.008 m
## Radius: 0.004 m
## Material properties:
## g: 0.0012
## h: 0.22
### Model TS using the Anderson (1950) model
bubble <- target_strength( bubble,
frequency = seq( 1e3 , 300e3 , 0.5e3 ) ,
model = "MSS_anderson" )
## MSS_ANDERSON model for GAS-object: gas bubble initialized.
### Plot results
plot( bubble , type = 'model' )
### First let's create a prolate spheroid shape
### 25 mm long with a length-to-radius ratio of 16
crustacean <- fls_generate( shape = "prolate_spheroid" ,
length_body = 25.0e-3 ,
length_radius_ratio = 16 ,
radius_curvature_ratio = 3.3 ,
g_body = 1.03 ,
h_body = 1.02 )
print( crustacean )
## FLS-object
## Fluid-like scatterer
## ID: UID
## Body dimensions:
## Length: 0.025 m (n = 19 cylinders)
## Mean radius: 0.0011 m
## Max radius: 0.0016 m
## Shape parameters:
## Defined shape: prolate_spheroid
## L/a ratio: 16
## Taper order:
## Material properties:
## g: 1.03
## h: 1.02
## Body orientation (relative to transducer face/axis): 1.571 radians
plot( crustacean )
### Model TS using the ray-path deformed cylinder model (DCM), distorted wave
### Born approximation (DWBA), the stochastic variation of the DWBA (SDWBA) ,
### and specifically curved versions of both the DWBA and SDWBA
crustacean <- target_strength( crustacean ,
frequency = seq( 1e3 , 200e3 , 1e3 ) ,
model = c( "DCM" , "DWBA" , "SDWBA" ,
"DWBA_curved" , "SDWBA_curved" ) )
## DCM model for FLS-object: UID initialized.
##
## DWBA model for FLS-object: UID initialized.
##
## SDWBA model for FLS-object: UID initialized.
##
## DWBA_CURVED model for FLS-object: UID initialized.
##
## SDWBA_CURVED model for FLS-object: UID initialized.
##
## Beginning TS modeling via DCM model for FLS-object: UID
## DCM TS model predictions for FLS-object: UID complete.
##
## Beginning TS modeling via DWBA model for FLS-object: UID
## DWBA TS model predictions for FLS-object: UID complete.
##
## Beginning TS modeling via SDWBA model for FLS-object: UID
## SDWBA TS model predictions for FLS-object: UID complete.
##
## Beginning TS modeling via DWBA_CURVED model for FLS-object: UID
## DWBA_CURVED TS model predictions for FLS-object: UID complete.
##
## Beginning TS modeling via SDWBA_CURVED model for FLS-object: UID
## SDWBA_CURVED TS model predictions for FLS-object: UID complete.
### Plot results
plot( crustacean , type = 'model' )