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Recent content by peponas

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    Simulating an infinite long current density source using FDTD

    Hi, I face a quite challenging problem...I am interested in simulating a current source with infinite length, inside a waveguide with finite length, terminated by two CFS-PML layers. The current source is in the form of hollow surface with components on x,y, and z axis, varying with the time...
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    About Conformal (or Contour-Path) FDTD and field nullification on PEC boundaries

    Consider a rectangular tapered waveguide, reminiscent a horn antenna. Of course, the inclined PEC walls cannot accurately be represented by the Yee grid due to the staircase approximation. Here comes the CFDTD where in the cut-cells, the integral form of Faraday law for H field is applied...
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    Interpretation of S Balance of lossless structure and resonances

    Hello, As far as I know, S Balance denotes the dissipated power from a structure's ports, and it is equal to unity for a lossless structure. I considered the following simplified structure: A smooth cylindrical waveguide where its middle section has a larger radius compared to that of the...
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    FDTD simulation of cylindrical waveguides and absorption of longitudinal fields

    Hi all, I have developed a FDTD code employing CFS-PML layers for the BC, and simulating waveguide structures. For this reason, the PML conductivity is scaled along z-axis and as a consequence, only the transverse field components (Er,Ephi,Hr,Hphi) "feel" the PML layer. By using a waveguide...
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    Interpretation of am and bm of Lumerical's Mode Expansion Monitors and relation witn S-Parameters in a dual port network

    Hello, According to Lumerical's help for the mode expansion monitor, am and bm coefficients represent complex transmission coefficient for mode m. However such and explanation is not clear to me enough. My first question is how these coefficients are related to the scattering matrix? Can we...
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    Power introduced by FDTD soft sources in a waveguide problems

    Thank you for the detailed reply. I will have a look and in case of any problem I will come back.
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    Power introduced by FDTD soft sources in a waveguide problems

    In other words, PML-SF-TF/SF source, correct?
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    Power introduced by FDTD soft sources in a waveguide problems

    Hello, thank you for the answer. I know the TF/SF technique but I try to avoid it since I have to also deal with a CFS-PML layer.
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    Power introduced by FDTD soft sources in a waveguide problems

    Hi all, I have a simplified model to study, which is the excitation of a smooth cylindrical waveguide usint a TEmp mode. Up to now, I used hard sources and therefore the transverse components of the electric field on the boundary was forced to specific values, according to the mode...
  10. P

    FDTD S parameters - negative sign of S21

    In my case this is not valid. Note that I excite with TE11 and measure the S11 and S21 of the same mode. I have simulated in CST studio a holow waveguide with a "brick" inside, and measure S11 and S21 and |S11|^2 + |S21|^2 = 1 is not the case. I suspect mode conversion due to the obstacle
  11. P

    FDTD S parameters - negative sign of S21

    Hello, I'm trying to calculate scattering parameters from a 3D FDTD code. I consider an "abritrary shaped" scatterer within a smooth waveguide. In order to calculate the S parameters, I express the fields on the basis of modal eigen fields at two different ports as a sum of a forward and a...
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    Sign of S Parameters obtained by an FDTD code

    Hello, I calculate S parameters using an FDTD code. I have monomode excitation and I calculate S-Parameters for more than 1 modes. I see that the |S11| below cutoff frequency of each mode is positive and very large. I know that this is due to the fact that each mode, below cutoff, is purely...
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    Modal analysis from FDTD signal

    Hello, I am looking for analyzing a signal on transverse plane (x,y) to a certain number of modes. I found a paper but I cannot find it anymore. I have a basis of modes and I would like to analyze the transverse field distribution on this basis. I know there is a way to do this using integrals...
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    FDTD measurement of reflection coefficient

    Why square the magnitude? To take the reflection coefficient of Power? But in order to square the magnitude and go from voltages to power calculations, power waves according to Kurokawa have to be supposed
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    FDTD measurement of reflection coefficient

    Thank you for the answer, I suppose the fact that the waves are guided makes the method inappropiate. One more question, in reflection coefficient should I take the magnitude of the ratio \[\frac{Z-Z_0}{Z+Z_0}\] or the ratio of the magnitudes, \[\frac{|Z|-|Z_0|}{|Z|+|Z_0|}\]. I know that these...

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