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Lecture 2 Differential geometry of curves 2.1 Definition of curves 2.1.1 Plane curves Implicit curves f(, y)=0 Example:x2+y2=a2 It is difficult to trace implicit curves It is easy to check if a point lies on the curve Multi-valued and closed curves can be represented
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Lecture 6 B-splines(Uniform and Non-uniform) 6.1 Introduction The formulation of uniform B-splines can be generalized to accomplish certain objectives These include Non-uniform parameterization Greater general flexibility Change of one polygon vertex in a Bezier curve or of one data point in a cardinal(or interpolatory) spline curve changes entire curve(global schemes) Remove necessity to increase degree of Bezier curves or construct composite Bezier curves
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Lecture 1 Introduction and classification of geometric modeling forms 1.1 Motivation Geometric modeling deals with the mathematical representation of curves, surfaces, and solids necessary in the definition of complex physical or engineering objects. The associated field of computational geometry is concerned with the development, analysis, and computer implemen tation of algorithms encountered in geometric modeling. The objects we are concerned with in engineering range from the simple
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LECTURE+ 12 RIGID BODY OYNAAICS 工 MPLICAT IONsF GENERAL ROTATIONAL OYWMICS EJLER's EQUATIN of MOTION TORQVE FREE SPECIAL CASES. PRIMARY LESSONS: 30 ROTATONAL MOTION MUCH MORE COMPLEX THAN PLANAR (20) EULER'S E.o.M. PROVIOE STARTING POINT FoR ALL+ OYwAmIcs SOLUTINS To EvlER's EQuATIONS ARE COMPLEX BUT WE CAN OEVE LOP GooO GEOMETRIC VISUALIZATION TOOLS
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FURTHER BASICS 5-1 · LINEAR MOMENTUM m NEWTON'S LAW ∴F=P ow TAKE THE MOMENT OF MDMENTUM ANGULAR MOMENTUM MUST EXPLICITLY OEFINE
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第二章习题 2.4解:x:女孩是大学生 y:女孩身高1.6m以上
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图和子图 图和简单图 关联矩阵 M(G)与邻接矩阵 A(G) 顶点的度 路和连通性 最短路问题 割边和键 生成树的计数及 Caley 公式 连线问题 连通度问题 连通度 可靠通信网的建设 Vizing 定理
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.4极限存在准则与两个重要极限 本节先介绍极限存在准则利用它们来导出两个重要极限. 一、极限存在准则 准则I(夹逼定理)若Vx∈U(x,)(或|x>M),均有g(x)≤f(x)≤h(x)且limg(x)=limh(x)=A,则有limf(x)=A
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1.1.将布洛赫函数中的调制因子k(r)展成付里叶级数,对于近自由电子,当电子波矢远 离和在布里渊区边界上两种情况下,此级数有何特点?在紧束缚模型下,此级数又有什么特 点? 解答 由布洛赫定理可知,晶体中电子的波函数 :(r)=e uk() 对比本教科书(5.1)和(5.39)式可得 (r)= m -a()\ 对于近自由电子,当电子波矢远离布里渊区边界时它的行为与自由电子近似,“()近似 一常数.因此,k(r)的展开式中,除了a(0)外,其它项可忽略 当电子波矢落在与倒格矢Kn正交的布里渊区边界时,与布里渊区边界平行的晶面族对 布洛赫波产生了强烈的反射,“k(r)展开式中
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《大学物理》课程PPT教学课件(二)第19章 近独立子系的统计规律 19.2 近独立子系的统计规律 19.3 M-B 统计在理想气体中的应用
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