نتایج جستجو برای: fdtd مشخصات تشعشعی
تعداد نتایج: 16969 فیلتر نتایج به سال:
In this paper, we present a new model using a Fourdimensional (4D) Element-Oriented physical concepts based on a topological approach in electromagnetism. Its general finite formulation on dual staggered grids reveals a flexible Finite-Difference Time-Domain (FDTD) method with reasonable local approximating functions. This flexible FDTD method is developed without recourse to the traditional Ta...
In this paper, a new finite-difference time-domain (FDTD) algorithm is investigated to analyze electromagnetic structures with curved boundaries using a Cartesian coordinate system. The new algorithm is based on a nonorthogonal FDTD method. However, only those cells near the curved boundaries are calculated by nonorthogonal FDTD formulas; most of the grid is orthogonal and can be determined by ...
توسعه سیگنال های صوتی و تصویری با کیفیت بالا و افزایش تعداد وسایل ارتباطی در منازل اخیرا باعث افزایش تقاضا برای مخابرات بیسیم با نرخ تبادل اطلاعات بالا در فواصل نزدیک شده است. فرکانس های موج میلیمتری (30 تا 300 گیگا هرتز) یکی از بهترین گزینه ها برای این منظور می باشد. باند فرکانس موج میلیمتری بعلت پهنای باند وسیع، امکان تبادل اطلاعات تا نرخ 5 گیگا بیت بر ثانیه را فراهم می سازد. بهرحال به علت تل...
A new method modifying the frequency dependent alternating direction implicit finite difference time domain (FD–ADI– FDTD) is presented. The method can improve the accuracy of FD–ADI–FDTD without significant increase of computational costs. The proposed method is validated by numerical tests. Index Terms ADI–FDTD, Debye media, Accuracy of FDTD
در این مطالعه، میزان انتقال حرارت بین دو استوانه هم محور، ضخیم و طویل با استفاده از روش های تحلیلی و با توجه به مفاهیم انتقال حرارت تشعشعی و انتقال حرارت هدایت و معادله تعادل انرژی در مرزها، بررسی شده است. همچنین با توجه به اهمیت کاربرد سپرهای تشعشعی در شرایط مختلف، میزان انتقال حرارت، درصد کاهش انتقال حرارت، دما و ضریب صدور مربوط به هر یک از سطوح در حضور یک، دو و سه سپر تشعشعی ضخیم با ضریب صدو...
The accuracy of improved two dimensional finite difference time domain method (2D FDTD) is verified by comparing with 3D FDTD method and experimental data. The optimized 60° photonic crystal waveguide bend, used in this study as a test case, is composed of InPGaAs/InP material and air holes and TE polarization is considered. The photonic crystal waveguide bend transmission data was measured...
To overcome the Courant limit on the time step size of the conventional finite-difference time-domain (FDTD) method, some weakly conditionally stable and unconditionally stable FDTD methods have been developed recently. To analyze the relations between these methods theoretically, they are all viewed as approximations of the conventional FDTD scheme in present discussion. The errors between the...
The time-to-frequency-domain conversion is often required in many applications of the finite-difference time-domain (FDTD) method. This paper presents a new FDTD time-to-frequencydomain conversion algorithm based on the optimization of nonuniform fast Fourier transform (NUFFT) with several redundancy-reduction techniques. The proposed algorithm can perform the FDTD conversion at multiple desire...
This paper presents an unconditionally stable leapfrog alternating-direction-implicit finite-difference time-domain (ADIFDTD) method for lossy media. Conductivity terms of lossy media are incorporated into the leapfrog ADI-FDTD method in an analogous manner as the conventional explicit FDTD method since the leapfrog ADI-FDTD method is a perturbation of the conventional explicit FDTD method. Imp...
Traditional finite difference time domain (FDTD) is classic numerical method for solving wave propagation problems such as electromagnetic wave, seismic wave and acoustic wave. As for airborne GPR simulation, modeling space is so large that memory consuming is pretty huge; on the other hand, the area between source antenna and ground surface is homogenous medium – air, where analytic solution c...
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