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 为了更好的帮助您理解掌握查询词或其译词在地道英语中的实际用法，我们为您准备了出自英文原文的大量英语例句，供您参考。 
A complete dynamics of the system has been developed using Hamilton's principle.


Experimental evidence on the complete dynamics, from quasielastic (QE) to completely dissipated orbiting in the19F+27Al system at 5.9 MeV/A is presented.


The complete dynamics of the system is given by a coupled set of ordinary and partial differential equations.


After formulating the governing nonlinear boundary value problem, it is reduced by a oneterm truncation to a system of nonlinear ordinary differential equations representing the complete dynamics of the electromechanical system.


It is shown how the complete dynamics of the system is described by means of the generalized FaddeevJackiw quatum brackets.

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If the complete dynamic range of the flame ionisation detector (FID) amplifier signal is to be integrated during trace analysis, the computer used for this purpose must have an effective dynamic range of at least six decades.


As a result, a systematic and complete dynamic model for the welding mobile robot was constructed.


After a summary of the complete dynamic equations, an application is given via an example which shows that planar aligned layers of smectic A subjected to an arbitrary periodic disturbance are linearly stable.


However, blood exhibits a constant viscosity at highshear rates and to obtain complete dynamic similarity between largescale experiments and lifescale flows, the highshear viscosity also needs to be included in the analysis.


The integrated fuzzyenhanced adaptive control is well tested via computer simulations using the new complete dynamic friction model recently suggested by Canudas de Wit et al.

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A complete dynamics of the system has been developed using Hamilton's principle.


Experimental evidence on the complete dynamics, from quasielastic (QE) to completely dissipated orbiting in the19F+27Al system at 5.9 MeV/A is presented.


The complete dynamics of the system is given by a coupled set of ordinary and partial differential equations.


After formulating the governing nonlinear boundary value problem, it is reduced by a oneterm truncation to a system of nonlinear ordinary differential equations representing the complete dynamics of the electromechanical system.


It is shown how the complete dynamics of the system is described by means of the generalized FaddeevJackiw quatum brackets.

 更多 
A complete dynamics of the system has been developed using Hamilton's principle.


Experimental evidence on the complete dynamics, from quasielastic (QE) to completely dissipated orbiting in the19F+27Al system at 5.9 MeV/A is presented.


The complete dynamics of the system is given by a coupled set of ordinary and partial differential equations.


After formulating the governing nonlinear boundary value problem, it is reduced by a oneterm truncation to a system of nonlinear ordinary differential equations representing the complete dynamics of the electromechanical system.


It is shown how the complete dynamics of the system is described by means of the generalized FaddeevJackiw quatum brackets.

 更多 


 In this paper, the unified formula of system statespace equation is derived. The general procedure to give the system bond graph model which includes the coupling of rigidity, flexibility and multiple energy domains is provided. To overcome the algebraic difficulty brought by differential causality in formulating system statespace equation, the constraint force at a joint can be considered as unknown effort source and added to the corresponding 0junction in system bond graph model. Finally, the practical... In this paper, the unified formula of system statespace equation is derived. The general procedure to give the system bond graph model which includes the coupling of rigidity, flexibility and multiple energy domains is provided. To overcome the algebraic difficulty brought by differential causality in formulating system statespace equation, the constraint force at a joint can be considered as unknown effort source and added to the corresponding 0junction in system bond graph model. Finally, the practical example is used to illustrate the generality and validity of the given procedure.  介绍了柔性机械系统完全动力学问题的键合图法，推导出了系统状态方程的统一公式。给出了综合考虑刚、弹性及多种能域相互耦合的柔性机械系统键合图模型的建立方法。为克服微分因果关系给系统状态方程建立所带来的代数困难，将约束反力视作未知势源加在系统键合图相应的０结处。最后，通过实例来说明本文方法的有效性及通用性。  The bond graph method for the complete dynamic problem of mechanical system is introduced.The unified formula of system statespace equations is derived.To overcome the algebraic difficulty brought by differential causality in formulating system statespace equations,the constraint forces at joints can be considered as unknown effort source and added to the corresponding oJunction in system bond graph model.Finally,a practical example is used to illustrate the generality and validity of this procedure.  介绍了机械系统完全动力学问题的键合图法，推导出系统状态方程的统一公式。为克服微分因果关系给系统状态方程建立所带来的代数困难，将约束反力视做未知势源加在系统键合图相应的０－结处。最后，通过实例来说明本文方法的有效性及通用性。  The bond graph method for the complete dynamics of planar linkage systems in accelerating reference frames is introduced. The unified formula of system state space equations is derived, and the general procedure to set up the bond graph model of planar linkage system in accelerating reference frames which includes the coupling of multiple energy domains is suggested. To overcome the algebraic difficulty brought by differential causality in formllating ststem staet space equations, the comstraint forces at... The bond graph method for the complete dynamics of planar linkage systems in accelerating reference frames is introduced. The unified formula of system state space equations is derived, and the general procedure to set up the bond graph model of planar linkage system in accelerating reference frames which includes the coupling of multiple energy domains is suggested. To overcome the algebraic difficulty brought by differential causality in formllating ststem staet space equations, the comstraint forces at joints can be considered as unknown effort sources and added to the corresponding o junctions in sysytem bond graph model. Finally, a practical example is user to illustrate the generality and ualidity of this procedure.  介绍非惯性系平面机构系统完全动力学问题的键合图法，推导出系统状态方程的统一公式，给出了多种能域相互耦合的非惯性系统平面机构系统键合图模型的建立方法。为克服微分因果关系给系统状态方程建立所带来的代数困难，将约束反力视做未知势源加在系统键合图相应的０－结处。最后，通过实例来说明本文方法的有效性及通用性。   << 更多相关文摘 
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