Spring 2003 1661AC22 Longitudinal Dynamics For notational simplicity, let X=Fn, Y= Fu, and Z= F aF Longitudinal equations(1-15 )can be rewritten as mi=X+X2- mg cos(0+△X

ATTITUDE MOTION -TORQVE FeEE MANE 0ISCUSSED THE ROTATIONAL MOTION FRDn 1 ERSPECTvE。FE”6o0 FRAME 一NE0T0F1A0 A WAy TO CONNECT THE MOTION To THE INEATIAL FRAME So WE CAN DESCRI BE THE ACTUAL MOTION TYPICALLY DoNE 6y DESC RI BING MOTION oF NEHICLE ABoVT THE

Spring 2003 Generalized forces revisited Derived Lagrange s equation from d'Alembert's equation ∑m(8x+16y+22)=∑(Fx+F+F。=) Define virtual displacements sx Substitute in and noting the independence of the 8q,, for each

Spring 2003 Example Given: Catapult rotating at a constant rate(frictionless, in the horizontal plane) Find the eom of the particle as it leaves the tube

Introduction We started with one frame (B) rotating and accelerating with respect to another(), and obtained the following expression for the absolute acceleration

CoRIoLIS ACcELERAT0 EMYSTIF∈p CONSIOER CASE oF CONSTANT ROTA ToN.No AT0 N OF MME⊙AGUA,ANDc°srAT RADIAL VELOCITY ( As sEEN IN THE RomTIwG

NEWTONs L丹WS ① BoDY CoNTINUES玉 N TTS STATE OF MOT(0N DR REST UNLESS FORCED DI RECTIoNs IMPoRTA. 儿L M5T3 E AN NIERT升L ACELERATION

用 MATLAB求解问题时,一般要经历建模和编程两个过程,只有在建模正确的前提下,方能得出正确的结果。 单自由度系统有阻尼自由振动 1.建立计算模型 由动力学可知,单自由度有阻尼自由振动的振动方程为:

燃烧焓的测定 液体饱和蒸气压的测定 双液系汽－液平衡相图 界面移动法测离子迁移数 电导法测定弱电解质的电离平衡常数 丙酮碘化反应动力学 复相催化－甲醇分解 流动吸附法测定多孔性物质的比表面 黏度法测定高聚物平均摩尔质量 偶极矩的测定

第二章质点组力学 本章研究质点组的动力学规律。重点掌握: (1)质心的概念和计算 (2)质点组的三个基本定理(动量定理、动量矩定理、动能定理)在基本系和质心坐标系中的数学表示。 (3)质心坐标系的重要性和特殊性