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Creating the k-space grid and defining the medium properties |
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 three-dimensional heterogeneous propagation medium. It builds on the Homogeneous Propagation Medium and Heterogeneous Propagation Medium examples.
Simulations in three-dimensions are performed in an analogous fashion to those in one and two dimensions. The medium discretisation is again performed by makeGrid with two additional inputs for the z-dimension. Similarly, matrices for the medium properties also have an extra dimension. The matrix indexing convention (x, y, z) is an extension to that used in two-dimensions (x, y) where matrix row and column data correspond to the x and y axes, respectively.
% create the computational grid Nx = 64; % number of grid points in the x direction Ny = 64; % number of grid points in the y direction Nz = 64; % number of grid points in the z direction dx = 0.1e-3; % grid point spacing in the x direction [m] dy = 0.1e-3; % grid point spacing in the y direction [m] dz = 0.1e-3; % grid point spacing in the z direction [m] kgrid = makeGrid(Nx, dx, Ny, dy, Nz, dz); % define the properties of the propagation medium medium.sound_speed = 1500*ones(Nx, Ny, Nz); % [m/s] medium.sound_speed(1:Nx/2, :, :) = 1800; % [m/s] medium.density = 1000*ones(Nx, Ny, Nz); % [kg/m^3] medium.density(:, Ny/4:end, :) = 1200; % [kg/m^3]
As in one and two dimensions, the initial pressure distribution is defined as a matrix of arbitrary numbers the same size as the computational grid. Here makeBall is used to create an initial pressure distribution of two small filled balls with different diameters.
% create initial pressure distribution using makeBall ball_magnitude = 10; % [Pa] ball_x_pos = 38; % [grid points] ball_y_pos = 32; % [grid points] ball_z_pos = 32; % [grid points] ball_radius = 5; % [grid points] ball_1 = ball_magnitude*makeBall(Nx, Ny, Nz, ball_x_pos, ball_y_pos, ball_z_pos, ball_radius); ball_magnitude = 10; % [Pa] ball_x_pos = 20; % [grid points] ball_y_pos = 20; % [grid points] ball_z_pos = 20; % [grid points] ball_radius = 3; % [grid points] ball_2 = ball_magnitude*makeBall(Nx, Ny, Nz, ball_x_pos, ball_y_pos, ball_z_pos, ball_radius); source.p0 = ball_1 + ball_2;
Again the sensor mask can be given as a list of Cartesian coordinates, a binary mask, or the grid coordinates of two opposing corners of a cuboid. Several functions for creating three-dimensional shapes are included in the k-Wave toolbox. For example, makeSphere which returns a binary map of single pixel spherical shell created using the midpoint circle algorithm, and makeCartSphere which returns the Cartesian location of an evenly distributed array of an arbitrary number of points on the surface of a sphere. In this example, a linear sensor array is explicitly created.
% define a series of Cartesian points to collect the data x = (-22:2:22)*dx; % [m] y = 22*dy*ones(size(x)); % [m] z = (-22:2:22)*dz; % [m] sensor.mask = [x; y; z];
A visualisation of the initial pressure distribution and the sensor mask using cart2grid and voxelPlot is given below.
The computation is invoked by calling kspaceFirstOrder3D with the inputs defined above. By default, a visualisation of the wave-field in the horizontal, median, and frontal planes are displayed, along with a status bar.
% input arguments
input_args = {'PlotLayout', true, 'PlotPML', false, ...
'DataCast', 'single', 'CartInterp', 'nearest'};
% run the simulation
sensor_data = kspaceFirstOrder3D(kgrid, medium, source, sensor, input_args{:});
By setting the optional input parameter 'PlotLayout' to true, a plot of the initial pressure, and sound speed and density (if heterogenous) are produced. To remove the PML from the display, the optional input 'PlotPML' is also set to false.
As the function runs, status updates and computational parameters are printed to the command line. By setting the optional input 'DataCast' to 'single', the computational time is decreased (see the Optimising k-Wave Performance Example for more details).
Running k-Wave simulation... start time: 18-Oct-2011 09:47:56 reference sound speed: 1800m/s dt: 16.6667ns, t_end: 6.15us, time steps: 370 input grid size: 64 by 64 by 64 grid points (6.4 by 6.4 by 6.4mm) maximum supported frequency: 7.5MHz smoothing p0 distribution... casting variables to single type... precomputation completed in 1.2331s starting time loop... estimated simulation time 23.6016s... simulation completed in 26.9362s reordering Cartesian measurement data... total computation time 28.205s
When the time loop has completed, the function returns the recorded time series at each of sensor locations defined by sensor.mask. The ordering is again dependent on whether a Cartesian or binary sensor mask is used. A visualisation is given below.
If a Cartesian sensor mask is used, the values of the acoustic field at the sensor points are obtained at each time step using interpolation. The interpolation mode can be changed by setting the optional input parameter 'CartInterp' to 'linear' (the default) or 'nearest' (used in this example). During the simulation, there is only a small performance difference between using Cartesian and binary sensor masks. However, if a Cartesian sensor mask with linear interpolation is used, the calculation of the triangulation points can significantly lengthen the precomputation time, particularly for 3D simulations (see the output below for the same example run with 'CartInterp' set to 'linear'). A Cartesian sensor mask can be converted to a binary sensor mask (and vice versa) using the functions cart2grid and grid2cart.
Running k-Wave simulation... start time: 18-Oct-2011 10:08:44 reference sound speed: 1800m/s dt: 16.6667ns, t_end: 6.15us, time steps: 370 input grid size: 64 by 64 by 64 grid points (6.4 by 6.4 by 6.4mm) maximum supported frequency: 7.5MHz smoothing p0 distribution... calculating Delaunay triangulation... precomputation completed in 25.1272s starting time loop... estimated simulation time 44.8s... simulation completed in 50.4407s total computation time 1min 15.598s
In both two and three dimensional simulations, if the optional input 'CartInterp' is set to 'nearest', the Cartesian points are internally mapped onto a binary grid. If more than one Cartesian sensor point maps to the same location, the duplicated points are discarded. Consequently, if the Cartesian sensor mask has a dense array of points, the number of returned time-series may not correspond to the original number of Cartesian sensor points. Details of discarded duplicate points are printed to the command line. This situation can be avoided by increasing the resolution of the computational grid, or by reducing the packing of the Cartesian sensor points.
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Simulations In One Dimension | Photoacoustic Waveforms in 1D, 2D and 3D | |
© 2009-2014 Bradley Treeby and Ben Cox.