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عدد الرسائل : 127 العمر : 37 الموقع : https://ahu-club.ahlamontada.com تاريخ التسجيل : 13/10/2007
| موضوع: Rigid body motion السبت 27 أكتوبر 2007, 11:13 am | |
| Rigid body motionA rigid body is a system of particles in which the distances between the particles do not vary. To describe the motion of a rigid body we use two systems of coordinates, a space-fixed system X, Y, Z, and a moving system x, y, z, which is rigidly fixed in the body and participates in its motion.Let the origin of the body-fixed system be the body’s center of mass (CM). The orientation of the axes of that system relative to the axes of the space-fixed system is given by three independent angles. The vector R points from the origin of the spaced-fixed system to the CM of the body. Thus a rigid body is a mechanical system with six degrees of freedom.Let r denote the position of an arbitrary point P in the body-fixed system. In the space fixed system its position is given by r + R, and its velocity isv = d(R + r)/dt = dR/dt + dr/dt = V + W ´ r.Here V is the velocity of the CM and W is the angular velocity of the body. The direction of W is along the axis of rotation and W = df/dt.The kinetic energy of the body isT = (1/2)Smivi2 = (1/2)Smi(V + W ´ r)2.We rewriteT = (1/2)MV2 + (1/2)Smi(W2ri2 - (W×ri)2), M = Smi, Smiri = 0.We find T = TCM + Trot, i.e. the kinetic energy is the sum of the kinetic energy of the motion of the CM and the kinetic energy of the rotation about the CM. In component form we write.Hereis the inertia tensor. The Wi are the components of W along the axis of the body fixed system. For a continuous system .By appropriate choice of the orientation of the body-fixed coordinate system the inertia tensor can be reduced to diagonal form. The directions of the axes xi are then called the principal axes of inertia and the diagonal components of the tensor are then called theprincipal moments of inertia. Then.Definitions: Asymmetrical top: Symmetrical top: Spherical top: Let L denote the angular momentum about the CM of the body.,which in component form yields.If x1, x2, and x3 are the principal axes of inertia, thenL1 = I1W1, L2 = I2W2, L3 = I3W3.The Lagrangian of a rigid body is .The equations of motionThe equations of motion of a rigid body are dP/dt = F, where P = total momentum and F = external forces, and dL/dt = t , where L = angular momentum about CM and t = total torque produced by external forces.Let A be an arbitrary vector and dA/dt its rate of change with respect to the space fixed axes, d'A/dt its rate of change with respect to the body fixed axes.dA/dt = d'A/dt + W ´ A.ThereforedP/dt = d'P/dt + W ´ P = F and dL/dt = d'L/dt + W ´ L = t .Let the body fixed axes be the principal axes of inertia of the body. ThenLi = IiWi and d'Li/dt = IidWi/dt,and we have Euler’s equations:The Eulerian anglesThe orientation of the body-fixed coordinate system with respect to the space-fixed coordinate system is described by three angles. These angles are often taken as the Eulerian angles, defined in the figure.We can express the components of the angular velocity W along the body-fixed axes x, y, z in terms of the Eulerian angles and their derivatives.FormulasCenter of mass:رابط هذه الصفحة http://electron6.phys.utk.edu/phys594/Tools/mechanics/summary/rigid/rigid.htm | |
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