第一节风蚀工程防治技术 第二节水蚀工程防治技术 第三节盐渍荒漠化的工程防治技术 第四节道路矿区荒漠化防治技术

一、操纵装置的特征编码与识别 二、旋纽、手柄、按纽、按键设计 三、工作椅设计的主要依据 四、手握式工具的设计

一、人体测量的基本知识 Foudamentals of Anthropometry 二、人体测量的基本术语 三、常用的人体测量数据 四、人体尺寸的应用

第一节切削运动和切削要素 第二节刀具的几何角度和结构 第三节切削层参数 第四节刀具材料

第一节基本概念 第二节定位基准的选择 第三节工艺路线的拟定 第四节加工余量及工序间尺寸的确定 第五节工艺尺寸链的计算 第六节时间定额及劳动生产率 第七节典型零件工艺

In this course we will study Classical Mechanics. Particle motion in Classical Mechanics is governed by Newton's laws and is sometimes referred to as Newtonian Mechanics. These laws are empirical in that they combine observations from nature and some intuitive concepts. Newton's laws of motion are not self evident. For instance, in Aristotelian mechanics before Newton, force was thought to be required in order

is a vector equation that relates the magnitude and direction of the force vector, to the magnitude and direction of the acceleration vector. In the previous lecture we derived expressions for the acceleration vector expressed in cartesian coordinates. This expressions can now be used in Newton's second law, to produce the equations of motion expressed in cartesian coordinates

In lecture D2 we introduced the position velocity and acceleration vectors and referred them to a fixed cartesian coordinate system. While it is clear that the choice of coordinate system does not affect the final answer, we shall see that, in practical problems, the choice of a specific system may simplify the calculations considerably. In previous lectures, all the vectors at all points in the trajectory were expressed in the

We have seen that the work done by a force F on a particle is given by dw =. dr. If the work done by F, when the particle moves from any position TI to any position T2, can be expressed as, W12=fdr=-(V(r2)-V(1)=V-v2, (1) then we say that the force is conservative. In the above expression, the scalar

In addition to the equations of linear impulse and momentum considered in the previous lecture, there is a parallel set of equations that relate the angular impulse and momentum. Angular Momentum We consider a particle of mass, m, with velocity v, moving under the influence of a force F. The angular momentum about point O is defined as the \moment\ of the particle's linear