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41.
潭邵高速公路岩溶与采空区路基处理方法 总被引:3,自引:0,他引:3
在探讨高速公路岩溶及采空区路基稳定性的合理评价方法的基础上,提出了潭邵高速公路岩溶与采空区路基处理范围的确定方法,进而,针对潭邵高速公路岩溶及采空区路基的工程及工程地质特点,提出了适合于潭邵高速公路岩溶及采空区路基特点的处理方法,应用于潭邵高速公路工程实践并取得成功,取得了相当的社会与经济效益。 相似文献
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对POLO、BORA、PASSAT等车载收放机的使用进行研究;对收放机如何进行改装以使得外部音频信号可以输入收放机,以及充分利用车载音响系统来播放进行了详细的说明和阐述。 相似文献
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Spatial Dynamics of Multibody Tracked Vehicles Part II: Contact Forces and Simulation Results 总被引:1,自引:0,他引:1
H. C. Lee J. H. Choi A.A. Shabana 《Vehicle System Dynamics: International Journal of Vehicle Mechanics and Mobility》1998,29(2):113-137
In this part of the paper, three dimensional computational capabilities, that includes significant details, are developed for the nonlinear dynamic analysis of large scale spatial tracked vehicles. Three dimensional nonlinear contact force models that describe the interaction between the track links and the vehicle components such as the rollers, sprockets, and idlers as well as the interaction between the track links and the ground are developed and used to define the generalized contact forces associated with the vehicle generalized coordinates. Tangential friction and contact forces are developed in order to maintain the stability of the track motion and avoid the slippage of the track or its rotation as a rigid body. Body and surface coordinate systems are introduced in order to define the spatial contact conditions. The nonlinear equations of motion of the tracked vehicle are solved using the velocity transformation procedure developed in the first part of this paper. This procedure is used in order to obtain a minimum set of differential equations, and avoid the use of the iterative Newton-Raphson algorithm. A computer simulation of a tracked vehicle that consists of one hundred and six bodies and has one hundred and sixteen degrees of freedom is presented in order to demonstrate the use of the formulations presented in this study. 相似文献
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J.H. Choi H.C. Lee A.A. Shabana 《Vehicle System Dynamics: International Journal of Vehicle Mechanics and Mobility》1998,29(1):27-49
In this paper, the nonlinear dynamic equations of motion of the three dimensional multibody tracked vehicle systems are developed, taking into consideration the degrees of freedom of the track chains. To avoid the solution of a system of differential and algebraic equations, the recursive kinematic equations of the vehicle are expressed in terms of the independent joint coordinates. In order to take advantage of sparse matrix algorithms, the independent differential equations of the three dimensional tracked vehicles are obtained using the velocity transformation method. The Newton-Euler equations of the vehicle components are defined and used to obtain a sparse matrix structure for the system dynamic equations which are represented in terms of a set of redundant coordinates and the joint forces. The acceleration solution obtained by solving this system of equations is used to define the independent joint accelerations. The use of the recursive equations eliminates the need of using the iterative Newton-Raphson algorithm currently used in the augmented multibody formulations. The numerical difficulties that result from the use of such augmented formulations in the dynamic simulations of complex tracked vehicles are demonstrated. In this investigation, the tracked vehicle system is assumed to consist of three kinematically decoupled subsystems. The first subsystem consists of the chassis, the rollers, the sprockets, and the idlers, while the second and third subsystems consist of the tracks which are modeled as closed kinematic chains that consist of rigid links connected by revolute joints. The singular configurations of the closed kinematic chains of the tracks are also avoided by using a penalty function approach that defines the constraint forces at selected secondary joints of the tracks. The kinematic relationships of the rollers, idlers, and sprockets are expressed in terms of the coordinates of the chassis and the independent joint degrees of freedom, while the kinematic equations of the track links of a track chain are expressed in terms of the coordinates of a selected base link on the chain as well as the independent joint degrees of freedom. Singularities of the transformations of the base bodies are avoided by using Euler parameters. The nonlinear three dimensional contact forces that describe the interaction between the vehicle components as well as the results of the numerical simulations are presented in the second part of this paper. 相似文献
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