| k-Wave Toolbox |
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Fast time-domain simulation of wave propagation for homogeneous media
sensor_data = kspaceSecondOrder(kgrid, medium, source, sensor) sensor_data = kspaceSecondOrder(kgrid, medium, source, sensor, ...) [sensor_data, field_data] = kspaceSecondOrder(kgrid, medium, source, sensor) [sensor_data, field_data] = kspaceSecondOrder(kgrid, medium, source, sensor, ...)
kspaceSecondOrder simulates the time-domain propagation of linear compressional waves through a one, two, or three dimensional homogeneous acoustic medium given four input structures: kgrid, medium, source, and sensor. The computation is based on an exact second-order k-space model for media with power law absorption. At each time-step (defined by kgrid.t_array), the pressure at the positions defined by sensor.mask are recorded and stored. If kgrid.t_array is set to 'auto', this array is automatically generated using makeTime. To prevent wave wrapping, the computational domain can be automatically expanded by a factor of two by setting the optional input 'ExpandGrid' to true.
An initial pressure distribution can be specified by assigning a matrix (the same size as the computational grid) of arbitrary numeric values to source.p0. An initial pressure gradient can similarly be specified using source.dp0dt. The pressure is returned as an array of time series at the sensor locations defined by sensor.mask. This is specified as a binary matrix (i.e., a matrix of 1's and 0's the same size as the computational grid) representing the grid points within the computational grid that will collect the data. The sensor_data is returned using MATLAB's standard column-wise linear matrix index ordering with the recorded data indexed as sensor_data(sensor_position, time). The final pressure field over the complete computational grid can also be obtained by setting sensor.record to {'p', 'p_final'}. In this case, the output sensor_data is returned as a structure with the outputs appended as the structure fields sensor_data.p and sensor_data.p_final.
Compared to the first-order simulation functions kspaceFirstOrder1D, kspaceFirstOrder2D, and kspaceFirstOrder3D, kspaceSecondOrder is restricted to homogeneous media and has less functionality. However, it is also more computationally efficient and allows an initial pressure gradient to be specified.
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k-Wave grid structure returned by |
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evenly spaced array of time values [s] (set to |
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homogeneous sound speed within the acoustic medium [m/s] |
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power law absorption exponent |
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power law absorption coefficient [dB/(MHz^y cm)] |
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initial pressure within the acoustic medium |
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initial pressure gradient within the acoustic medium |
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binary grid specifying where the pressure is recorded at each time-step |
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cell array of the acoustic parameters to record in the form |
Optional 'string', value pairs that may be used to modify the default computational settings.
| Input | Valid Settings | Default | Description |
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(Boolean scalar) |
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Boolean controlling whether the grid size is expanded on two sides to delay the time before wave wrapping occurs. |
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(Boolean scalar) |
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Boolean controlling whether |
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(Boolean scalar) |
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Boolean controlling whether the pressure field for each time step is plotted in a new window. |
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(integer numeric scalar) |
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The number of iterations which must pass before the simulation plot is updated. |
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(numeric two element vector) |
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[min, max] values used to control the scaling for |
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(Boolean scalar) |
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Boolean controlling whether the simulation iterations are progressively plotted. |
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(Boolean scalar) |
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Boolean controlling whether |
If sensor.record is not defined by the user:
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time varying pressure recorded at the sensor positions given by |
If sensor.record is defined by the user:
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time varying pressure recorded at the sensor positions given by |
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final pressure field at all grid points within the domain (returned if |
kspaceFirstOrder1D, kspaceFirstOrder2D, kspaceFirstOrder3D, makeGrid, makeTime, smooth
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kspacePlaneRecon | loadImage | ![]() |
© 2009-2014 Bradley Treeby and Ben Cox.