Changes

EM.Tempo

231 bytes added, 15:38, 13 September 2016
/* EM.Tempo's Simulation Data & Observables */
=== Examining the Near Fields in Time and Frequency Domains ===
[[Image:FDTD77.png|thumb|400px|Time-domain evolution of the electric field at a given point.]]
EM.Tempo's FDTD time marching loop computes all the six electric and magnetic field components at every Yee cell of your structure's mesh at every time step. This amounts to a formidable amount of data that is computationally very inefficient to store. Instead, you can instruct EM.Tempo to save a small potion of these data for visualization and plotting purposes. Using a '''Field Probe''' at a specified point, you can record the a time-domain field component over the entire FDTD loop. The time-domain results are also transformed to the frequency domain within the specified bandwidth using a discrete Fourier transform (DFT).
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[[Image:FDTD77.png|thumb|left|480px|Time-domain evolution of the electric field at a given point.]]</td>
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In EM.Tempo, you can visualize the near fields at a specific frequency in a specific plane of the computational domain. To do so, you need to define a '''Field Sensor''' observable. EM.Tempo's field sensor defines a plane across the entire computational domain parallel to one of the three principal planes. The magnitude and phase of all the six components of the electric and magnetic fields on the mesh grid points on the sensor plane are computed and displayed.
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<td> [[Image:FDTD_FS2.png|thumb|360pxleft|420px|EM.Tempo's Field Sensor dialog.]] </td></tr><tr><td> [[Image:FDTD_FS1_new.png|thumb|360pxleft|420px|Three field sensor planes defined around a PEC ellipsoid illuminated by a plane wave source.]] </td>
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<td> [[Image:FDTD_FS3_new.png|thumb|360pxleft|420px|Electric field distribution above the PEC plate.]] </td></tr><tr><td> [[Image:FDTD_FS4_new.png|thumb|360pxleft|420px|Magnetic field distribution above the PEC plate.]] </td>
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<td> [[Image:FDTD_FF1.png|thumb|360pxleft|480px|EM.Tempo's Radiation Pattern dialog.]] </td></tr><tr><td> [[Image:FDTD_FF3.png|thumb|360pxleft|480px|EM.Tempo's Radar Cross Section dialog.]] </td>
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[[Image:FDTD_FF2.png|thumb|400px|EM.Tempo's Far Field Acceleration dialog.]]
The default radiation box is placed at an offset of 0.1&lambda;<sub>0</sub> from the largest bounding box of your physical structure. You can change the offset value from the "Far Field Acceleration" dialog, which can be accessed by clicking the {{key|Acceleration...}} button of EM.Tempo's Radiation Pattern dialog. Calculation of far-field characteristics at high angular resolutions can be a very time consuming computational task. You can accelerate this process by setting a lower '''Max. Far Field Sampling Rate''' from the same dialog. The default sampling rate is 30 samples per wavelength. A low sampling rate will under-sample the mesh grid points on the radiation box.
<table><tr><td> [[Image:FDTD133FDTD_FF2.png|thumb|350pxleft|Far Field Background Medium 480px|EM.Tempo's far field acceleration dialog.]]</td></tr></table>  
=== Radiation Pattern Above a Half-Space Medium ===
# Free space background terminated in an infinite PMC ground plane at the bottom
# Free space background terminated in an infinite dielectric half-space medium
 
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<td> [[Image:FDTD133.png|thumb|left|480px|EM.Tempo's far field background medium dialog.]] </td>
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In other words, EM.Tempo lets you calculate the far field radiation pattern of a structure in the presence of any of the above four background structure types. You can set these choices in EM.Tempo's "Far Field Background Medium" dialog. To access this dialog, open the Radiation Pattern dialog and click the button labeled {{key|Background...}}. From this dialog, you can also set the Z-coordinate of the top of the terminating half-space medium. If you set the -Z boundary condition of your computational domain to PEC or PMC types, the cases of infinite PEC or PMC ground planes from the above list are automatically selected, respectively, and the Z-coordinates of the ground plane and the bottom face of the computational domain will be identical.
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<td> [[Image:fdtd_out36_tn.png|thumb|300pxleft|360px|Radiation pattern of a vertical dipole above PEC ground.]] </td><td> [[Image:fdtd_out37_tn.png|thumb|300pxleft|360px|Radiation pattern of a vertical dipole above PMC ground.]] </td>
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<td> [[Image:fdtd_out38_tn.png|thumb|300pxleft|360px|Radiation pattern of a horizontal dipole above PEC ground.]] </td><td> [[Image:fdtd_out39_tn.png|thumb|300pxleft|360px|Radiation pattern of a horizontal dipole above PMC ground.]] </td>
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