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In this lecture, we consider the problem of a body in which the mass of the body changes during the motion, that is, m is a function of t, i.e. m(t). Although there are many cases for which this particular model is applicable, one of obvious importance to us are rockets. We shall see that a significant fraction of the mass of a rocket is the fuel, which is expelled during flight at a high velocity and thus, provides the propulsive force for the rocket
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Lecture D33: Forced Vibration Fosinwt m Spring Force Fs =-kx, k>0 Dashpot Fd =-ci, c>0 Forcing Fext Fo sin wt Newton's Second Law (mix =CF) mx+cx+kx= Fo sin wt =k/m,=c/(2mwn)
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Lecture D32: Damped Free Vibration Spring-Dashpot-Mass System k Spring Force Fs =-kx, k>0 Dashpot Fd =-cx, c>0 Newton's Second Law (mx =EF) mx +cx+kx (Define)Natural Frequency wn=k/m,and
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When the only force acting on a particle is always directed to- wards a fixed point, the motion is called central force motion. This type of motion is particularly relevant when studying the orbital movement of planets and satellites. The laws which gov- ern this motion were first postulated by Kepler and deduced from observation. In this lecture, we will see that these laws are a con- sequence of Newton's second law. An understanding of central
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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 this lecture, we will particularize the conservation principles presented in the previous lecture to the case in which the system of particles considered is a 2D rigid body. Mass Moment of Inertia In the previous lecture, we established that the angular momentum of a system of particles relative to the center of mass, G, was
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In this lecture we will look at some applications of Newton's second law, expressed in the different coordinate systems that were introduced in lectures D3-D5. Recall that Newton's second law F=ma, (1) is a vector equation which is valid for inertial observers. In general, we will be interested in determining the motion of a particle given
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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
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AutoCAD是由美国Autodesk公司开发的通用计算机辅助设计(Computer Aided Design,CAD)软件,具有易于掌握、使用方便、体系结构开放等优点, 能够绘制二维图形与三维图形、标注尺寸、渲染图形以及打印输出图纸,目前 已广泛应用于机械、建筑、电子、航天、造船、石油化工、土木工程、冶金、 地质、气象、纺织、轻工、商业等领域
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AutoCAD是由美国Autodesk公司开发的通用计算机辅助设计(Computer Aided Design,CAD)软件,具有易于掌握、使用方便、体系结构开放等优点, 能够绘制二维图形与三维图形、标注尺寸、渲染图形以及打印输出图纸,目前 已广泛应用于机械、建筑、电子、航天、造船、石油化工、土木工程、冶金、 地质、气象、纺织、轻工、商业等领域。 AutoCAD 2007是AutoCAD系列软件的最新版本,与AutoCAD先前的版本相比, 它在性能和功能方面都有较大的增强,同时保证与低版本完全兼容
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