1) finite horizon
有限时域
1.
This paper analyzes the optimal replenishment policy,when a buyer faces imminent price increase under finite horizon.
研究了有限时域下采购商面对价格上升时的订货策略问题。
4) finite-difference time-Domain
时域有限差分法
1.
This paper studies the EM Radiation and shield of monopole handset with the extrapolation which is suitable for the Finite-Difference Time-Domain(FDTD).
用时域有限差分法(FDTD)的一种外推法研究了单极天线手机近场辐射及屏蔽。
2.
In this paper,the in- fluence of the coupling aperture on the sound energy decay and coupling constant in the primary room is investigated by means of the finite-difference time-domain method,and the investigation is limited within the low-frequency range.
文中运用时域有限差分法,在低频范围内模拟了耦合窗面积的改变对主厅中不同位置的耦合常数和声能衰减的影响。
3.
The compact finite-difference time-domain(CFDTD) method was employed to simulate the dispersion properties in an electromagnetic band gap(EBG) waveguide which was uniform in the propagation direction.
建立了紧凑格式二维时域有限差分法(CFDTD)模型,利用二维网格划分计算三维传播问题,简化了计算量。
5) FDTD method
时域有限差分法
1.
A fast equivalence algorithm of RCS based on FDTD method;
计算二维雷达散射截面的一种快速等效算法——时域有限差分法
2.
The Application Study of FDTD Method to Simulate of Electromagnetic Field Around EHV Transmission Line;
时域有限差分法在超高压输电线电磁场仿真中的应用研究
3.
By employing FDTD method and simulating the effects of electromagnetic on the heart of human body, the eddy-currents of the heart of human body induced by MRI time-varying gradient fields are computed and compared with the recommended threshold.
运用时域有限差分法(FDTD),通过电磁场对人体心脏影响的模型仿真,计算出心脏体段由磁共振成像(MRI)时变梯度场感应的涡流,并与已有的心脏刺激阈值进行比较。
6) FDTD
时域有限差分
1.
The Transmission Properties Research of Photonic Crystal Slab W3 Waveguide With The Use of The Parallel 3D FDTD Algorithm;
用三维并行时域有限差分算法研究光子晶体薄板W3波导传输特性
2.
A New Setup Method of Electric Dipole Source in FDTD Grids;
电偶极子源在时域有限差分网格中设置的一种新方法
3.
FDTD FOR EMP FIELD ANALYSIS IN DIELECTRIC CYLINDER;
利用时域有限差分法分析和计算介质柱内瞬态场分布
补充资料：超导电性的局域和非局域理论（localizedandnon-localizedtheoriesofsuperconductivity）
超导电性的局域和非局域理论（localizedandnon-localizedtheoriesofsuperconductivity）
伦敦第二个方程（见“伦敦规范”）表明，在伦敦理论中实际上假定了js(r)是正比于同一位置r的矢势A(r)，而与其他位置的A无牵连；换言之，局域的A(r)可确定该局域的js(r)，反之亦然，即理论具有局域性，所以伦敦理论是一种超导电性的局域理论。若r周围r'位置的A(r')与j(r)有牵连而影响j(r)的改变，则A(r)就为非局域性质的。由于`\nabla\timesbb{A}=\mu_0bb{H}`，所以也可以说磁场强度H是非局域性的。为此，超导电性需由非局域性理论来描绘，称超导电性的非局域理论。皮帕德非局域理论就是典型的超导电性非局域唯象理论。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条