2.1性质与使用性能 1.基础概念 2.性质与性能的区别与关系 3.材料的失效分析 4.材料(产品)使用性能的设计 5.材料性能数据库 6.其它问题

第一章 室内设计的含义、发展和基本观点 第二章 室内设计的内容、分类和方法步骤 第三章 室内设计的依据、要求和特点 第四章 室内空间设计 第五章 室内照明设计 第七章 家具 第八章 室内陈设 第十章 人体工程学、环境心理学与室内设计 第十一章 室内设计的风格与流派 第十三章 住宅室内环境设计 第十五章 居住空间未来发展趋势

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、掌握设备有形、无形损耗的类型及其对设备价值的影响； – 2、掌握设备折旧的含义、折旧方法与计算； – 3、掌握设备经济寿命概念及其计算； – 4、掌握存在新设备的设备更新原则及方法； – 5、掌握存在税收影响的设备租赁与购买比较决策

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)

现金流量和瓷金等值计算 一、现金流量构成 现金流量( Cash flow,CF) 现金流入( Cash In flow,CI) 销售(经营)收入、资产回收、借款等 现金流出( Cash Out flow,CO) 投资、经营成本、税、贷款本息偿还等 净现金流量(NCF) NCF=CI-CO

第一章 概论 第二章 室内设计与人体工程学 第三章 室内空间设计 第四章 室内空间界面和配套设施的装饰设计 第五章 室内照明设计 第六章 室内色彩设计 第七章 室内陈设与绿化设计

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

In this lecture, we consider the problem of a body in which the mass of the body changes during the motion, that is, m is a function of t, i.e. m(t). Although there are many cases for which this particular model is applicable, one of obvious importance to us are rockets. We shall see that a significant fraction of the mass of a rocket is the fuel, which is expelled during flight at a high velocity and thus, provides the propulsive force for the rocket

In this lecture, we will consider how to transfer from one orbit, or trajectory, to another. One of the assumptions that we shall make is that the velocity changes of the spacecraft, due to the propulsive effects, occur instantaneously. Although it obviously takes some time for the spacecraft to accelerate to the velocity of the new orbit, this assumption is reasonable when the burn time of the rocket is much smaller than the period of the orbit. In such cases, the Av required to do the maneuver is simply the difference between the