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This example provides a simple demonstration of using k-Wave for the simulation and detection of the pressure field generated by an initial pressure distribution within a two-dimensional heterogeneous propagation medium. It builds on the Homogeneous Propagation Medium Example.
For a homogeneous propagation medium, the sound speed is specified as a single scalar value in SI units. If the propagation medium is heterogeneous, medium.sound_speed
and medium.density
are instead given as matrices with the same dimensions as the computational grid (i.e., with Nx
rows and Ny
columns). These matrices can be created in several fashions, including explicitly (as given below), from external image maps, or using spatial or volume data from other simulations or experimental imaging modalities.
% define the properties of the propagation medium medium.sound_speed = 1500*ones(Nx, Ny); % [m/s] medium.sound_speed(1:Nx/2, :) = 1800; % [m/s] medium.density = 1000*ones(Nx, Ny); % [kg/m^3] medium.density(:, Ny/4:end) = 1200; % [kg/m^3]
The computation is again invoked by running kspaceFirstOrder2D
with the inputs defined above. Rather than manually producing a plot of the initial pressure distribution, sensor mask, and medium properties, it is also possible to use the inbuilt plotting functionality of kspaceFirstOrder2D
by setting the optional input 'PlotLayout'
to true
. This produces a plot of the simulation inputs as shown below. Optional inputs for k-Wave functions are given after the main inputs as 'string'
, value
pairs. The 'string'
identifies the optional input parameter that is being modified, and the value
is the user setting for this parameter. To remove the PML from the display, the optional input 'PlotPML'
is also set to false
.
% run the simulation with optional inputs for plotting the simulation % layout in addition to removing the PML from the display sensor_data = kspaceFirstOrder2D(kgrid, medium, source, sensor, 'PlotLayout', true, 'PlotPML', false);
A plot of the recorded time series is given below. The shape of the main wave-front has been perturbed compared to the homogeneous example, and weak reflections from the heterogeneous interfaces can also be seen.
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© 2009-2014 Bradley Treeby and Ben Cox.