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Program 11 1D FDTD Vector update with Sparse matrix update
1D unitless FDTD with vector and sparse matrix update

oltre 14 anni fa | 406 download |

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Program 10 Unitless 1D FDTD without For Loops using Vector update for better computation speed
1D FDTD with no for loops for E & H fields update. For loop only for time steps.

quasi 15 anni fa | 427 download |

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Program 9A, 9B 1D FDTD with Handling of Material Properties - Different Permittivities
1D FDTD showing how to model difference in permittivities and what to observe

quasi 15 anni fa | 722 download |

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Program 8 Unitless 1D FDTD Open Boundary with Courant Factor Greater than 1 & Hard source
1D FDTD with Courant factor > 1 results in instability and ultimately results in blow up

quasi 15 anni fa | 355 download |

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Program 7A & 7B Unitless 1D FDTD Open Boundary with Courant Factor less than 1
Evolution of high frequency ripples along with signal decay in 1D FDTD with Courant factor < 1

quasi 15 anni fa | 355 download |

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Program 6A,6B,6C Unitless 1D FDTD Open Boundary with Different sources
1D unitless FDTD with open boundaries to compute propagation of fields

quasi 15 anni fa | 485 download |

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Program 5 Finite Difference Method Poisson Solver using both normal and SOR iterations
Solve for steady state voltage using Poisson when a charge density is specified

quasi 15 anni fa | 1055 download |

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Finite Difference Method solution to Laplace's Equation
Objective of the program is to solve for the steady state DC voltage using Finite Difference Method

quasi 15 anni fa | 2143 download |

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Potential & Field Distribution in Microstrip Line - Application of FDM solution to Laplace Equation
Objective of the program is to solve for the steady state voltage an field in a microstrip line

quasi 15 anni fa | 789 download |

Inviato

Successive Over Relaxation (SOR) of Finite Difference Method solution to Laplace's Equation
Objective of the program is to solve for the steady state DC voltage using SOR in FDM

quasi 15 anni fa | 1276 download |