Introduction引言 18-1 The Relativity Postulate of Mechanics伽 利略相对性原理经典力学的时空观 18-2 The Postulates of Special Relativity The Lorentz Transformation狭义相对论的基本原理洛仑兹坐标变换式 18-3 Some Consequences of the Lorentz Transformation狭义相对论的时空观 18-4 The Lorentz Transformation of Velocities相对论速度变换式 18-5 The Relativistic Dynamic theory相对论 动力学基础

4.1 经典自由电子论（Drude-Lorentz) 4.2 量子自由电子论（Sommerfeld） ： 一. 金属中自由电子的运动状态 二. 能态密度 三. 基态能量 四. T>0K 时电子的分布和能量

32-8 Lorentz Transformation (LT) P747-749 (洛沦兹变换) Assume two inertial reference frames: S, S' O,o 'coincide’(重合 superimposed) at time:t=0 S为静系,S以υ沿ox轴向右运动(开始时,两 个坐标系原点重合)

One of the most powerful tools for the analysis of electromagnetics problems is the integral solution to Maxwell’s equations formulated by Stratton and Chu [187, 188]. These authors used the vector Green’s theorem to solve for E˜ and H˜ in much the same way as is done in static fields with the scalar Green’s theorem. An alternative approach is to use the Lorentz reciprocity theorem of § 4.10.2, as done by Fradin [74]. The reciprocity

The Lorentz Force Example: The Closed-Field MassSpectrometer Example:The Hall Effect Example:Magnetic Mirrors

《电动力学》课程参考文献：LORENTZ FORCE ON DIELECTRIC AND MAGNETIC PARTICLES

复旦大学：《电动力学》课程电子讲义（PDF演示版）第八章 狭义相对论 08-0102 旧时空理论、狭义相对论的基本原理、Lorentz变换

中国科学院理论物理研究所：标准模型与高能洛伦兹破坏 Standard Model And High-Energy Lorentz Violation

§9.1 磁感应强度 磁场中的高斯定理 一、基本磁现象 二、磁感应强度 三、磁场的高斯定理 §9.2毕奥-萨伐尔定律及其应用 (Biot-Savart Law and Its Application) §9.3 安培环路定理及其应用(Ampere's Circuital Theorem and Its Application) §9.5 洛仑兹力(Lorentz Force) §9.6 安培力(Ampere Force)

《力学》课程教学资源（参考资料）其它方法推导洛伦兹变换（2/2）Derivation of the Lorentz transformation without the use of Einstein’s second postulate