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Outline Review of Equations of Motion Rotational Motion Equations of Motion in Rotating coordinates Euler Equations Example: Stability of Torque Free Motion Gyroscopic Motion Euler Angles Steady Precession Steady Precession with M=0 MIT
文档格式:DOC 文档大小:59.5KB 文档页数:9
第十三章沟通 一、名词解释 沟通 二、单项选择题 1.沟通是关于如何使()保持一致的问题。 A.领导方式和激励行为B.领导方式和组织结构 C.绩效考核和激励行为D.绩效考核和组织结构 2.沟通的基础是()。 A.共同的目标B.信息C.计划D.信任
文档格式:DOC 文档大小:39.5KB 文档页数:5
第十七章企业技术创新 一、单项选择题 1.()曾在《经济发展理论》中把创新定义为企业家的职能。 A.波特B.熊彼特C.泰罗D.德鲁克 2.()或迟或早会引起整个技术水平的提高。 A.产品创新B.材料创新C.工艺创新D.手段创新
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d maino int n. 2 long int fac=l printf(\请输入一个正整数:\) scanf(\%d\, &n)
文档格式:DOC 文档大小:26.5KB 文档页数:1
#include #define null o FILE fp; ar a[81.c char*pl=\%oc\,*p2=\%d,%d\,*p3=\%of%f,%f”,*p4=\%s\ float flf2.13 f(fp=fopen(\:: I paper. dat\,\rb\))NULL)
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#defineS sum(int arr[, int); printf(\请输入%d个整数:n\,N), for(i=0; i
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Non-Inertial Reference Frame Gravitational attraction The Law of Universal Attraction was already introduced in lecture D1. The law postulates that the force of attraction between any two particles, of masses M and m, respectively, has a magnitude, F, given by F= (1) where r is the distance between the two particles, and G is the universal constant of gravitation. The value of G is empirically determined to be
文档格式:DOC 文档大小:25.5KB 文档页数:1
void swap(int*a, int*b) int x, y, printf(℃\请输入两个整数ⅹ和y:\) scanf(\%od%d\, &x, &y) printf\交换前x和y的值为:\) printf(x=%dy=%d\\n\x, y);
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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
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#include maino int x=5, y=0, Z=6, result printf(\&&y&&z=%d\\n\,result result=x-3y‖z*5; printf(\x-3 yz*=%d\\n\, result)
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