11-1 Classifications of Magnetic Media Magnetic Permeability 磁介质的分类磁导率 11-2 Molecular Theory of Paramagnetism& Diamagnetism顺磁质和抗磁质磁化的分子理论 11-3 Ampere's Law in the magnetic matter and magnetic intensity H 磁介质中的安培环路定理和磁场强度H 11-4 Ferromagnetism铁磁质

§ 12-1 Nonelectrostatic Force Source & Electromotive Force 非静电力 电源 电动势 § 12-2 Faraday’s Law of Induction 电磁感应定律 § 12-3 Motional Electromotive Force 动生电动势 § 12-4 Induced Electric Field 感生电动势 涡旋电场 § 12-5 Self-induction & Mutual-induction 自感和互感 § 12-6 Energy of the Magnetic Field 磁场的能量

北京大学：《宪法学 Constitutional Law》精品课程电子教案_第一章 基本概念（张千帆）

§4.1 序言、热力学概论 §4.2 热力学基本概念及术语 §4.3 热力学第一定律(first law of thermodynamics) §4.4 恒容热、恒压热与焓 §4.5 热容(heat capacity) §4.6 热力学第一定律的一些应用 §4.7 第一定律对化学反应的应用——热化学

Inertial reference frames In the previous lecture, we derived an expression that related the accelerations observed using two reference frames, A and B, which are in relative motion with respect to each other. aA =aB+(aA/ B)'y'' 22 x (DA/ B) 'y'2'+ TA/B+ X TA/B). (1) Here, aA is the acceleration of particle A observed by one observer, and

When the only force acting on a particle is always directed to- wards a fixed point, the motion is called central force motion. This type of motion is particularly relevant when studying the orbital movement of planets and satellites. The laws which gov- ern this motion were first postulated by Kepler and deduced from observation. In this lecture, we will see that these laws are a con- sequence of Newton's second law. An understanding of central

Lecture D32: Damped Free Vibration Spring-Dashpot-Mass System k Spring Force Fs =-kx, k>0 Dashpot Fd =-cx, c>0 Newton's Second Law (mx =EF) mx +cx+kx (Define)Natural Frequency wn=k/m,and

1.性质:本课程是法学专业本科段必修课程 2.任务:本课程的内容包括环境与资源保护法的概述、发展、体系、法学基础理论以及其基本原则,基本制度,自然资源保护法,环境污染防治法,环境管理体制和监督管理制度,环境法律责任和国际环境法

Lecture D33: Forced Vibration Fosinwt m Spring Force Fs =-kx, k>0 Dashpot Fd =-ci, c>0 Forcing Fext Fo sin wt Newton's Second Law (mix =CF) mx+cx+kx= Fo sin wt =k/m,=c/(2mwn)

In this lecture, we will revisit the application of Newton's second law to a system of particles and derive some useful relationships expressing the conservation of angular momentum. Center of Mass Consider a system made up of n particles. A typical particle, i, has mass mi, and, at the instant considered, occupies the position Ti relative to a frame xyz. We can then define the center of mass, G, as the point