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In this lecture, we will derive expressions for the angular momentum and kinetic energy of a 3D rigid body. We shall see that this introduces the concept of the Inertia Tensor. Angular Momentum We start form the expression of the angular momentum of a system of particles about the center of mass
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In the previous lectures we have described particle motion as it would be seen by an observer standing still at a fixed origin. This type of motion is called absolute motion. In many situations of practical interest, we find ourselves forced to describe the motion of bodies while we are simultaneously moving with respect to a more basic reference. There are many examples were such situations occur. The absolute motion of a passenger inside an aircraft is best
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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
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《工程热力学》课程教学资源(习题解答)第九章 气体动力循环
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《工程热力学》课程教学资源(例题讲解)第10章 动力循环及制冷循环
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《工程热力学》课程教学课件(PPT讲稿)第10章 动力循环
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《工程热力学》课程教学课件(教案讲义)第10章 动力循环
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《工程热力学》课程教学资源(习题解答)第十章 蒸汽动力装置循环
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运用FLAC有限差分程序,建立了一个边坡动力数值分析模型,对不同动力参数及岩土参数条件下的边坡响应规律进行数值模拟研究.结果表明,边坡动力响应放大系数与加载频率不是简单的线性关系,而是存在一个主导频率,即在该频率的动载作用下,边坡动力响应放大系数较大.进一步研究表明,主导频率主要受边坡岩土体剪切模量和密度的影响.提出了边坡动力响应放大系数与输入动力参数以及岩体力学参数间的函数关系
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一、提高热效率 二、减小汽轮机低压缸尺寸,末级叶片变短
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