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Aiming at the characteristic of degree of freedom in multiple input multiple output radars, a scheme for multi-target identification and localization using a monostatic MIMO radar system with L-shape arrays is proposed, as well as the MIMO-Capon method based on Capon waveformer is presented.

针对多输入多输出(multiple input multiple output, MIMO)雷达的自由度特性,提出了一种单基地L型阵列MIMO雷达的空间多目标分辨和定位方案和基于Capon波束形成器的MIMO-Capon二维空间谱估计方法。

Aiming at the characteristic of degree of freedom in multiple input multiple output radars, a scheme for multitarget identification and localization using a monostatic MIMO radar system with L-shape arrays is proposed, as well as the MIMO-Capon method based on Capon waveformer is presented.

针对多输入多输出(multiple input multiple output, MIMO)雷达的自由度特性,提出了一种单基地L型阵列MIMO雷达的空间多目标分辨和定位方案和基于Capon波束形成器的MIMOCapon二维空间谱估计方法。

Secondly, in our methods, the essential geometry of the image single axis geometry may be specified by six parameters and this may be estimated from one conic and one fundamental matrix (a total of 12 parameters) or may be minimally estimated from two conics (a total of 10 parameters).

本文证明了单轴旋转运动的不变量可以通过一个基本矩阵和一条二次曲线来确定,在这种情况下,由于基本矩阵的自由度为7,二次曲线的自由度为5,所需确定的参量个数仅为12,大大减少了不变量的计算量;本文同时证明单轴旋转运动的不变量可以通过最少两条二次曲线来确定,在这种情况下所需确定的参量个数仅为10,该方法是目前同类算法中参数最少的;本文提出了用多条二次曲线求解单轴旋转运动的不变量的最大似然估计算法,其所需确定的参量个数为6+2n,其中n为二次曲线的个数,该公式更深刻地反映了二次曲线与不变量的参数关系。

In physics, human body is a very complex deformable object with many degrees of freedom.

人体是复杂的变形物体,结构自由度多。

This dissertation's main work and innovations is following: 1. The 6DOF kinematic and dynamic equations of motion for multiple thrusters AUV are derived and presented in a compact form using vector notation. The hydrokinetics of the MTAUV is classified anew. The MTAUV has two kinds of work modes which are cruising and hovering. The fluid dynamical mathematics description of the MTAUV is given anew. 2. The kinetics equations of the MTAUV in the low speed hovering are analyzed and studied.

本文主要的工作和创新点主要有以下几个方面:一、采用矢量参数的形式建立了基于多推进器自主水下航行器的六自由度运动学方程和动力学方程;对基于多推进器自主水下航行器的流体动力进行了重新分类,给出了基于多推进器自主水下航行器在巡航工作模式和悬停工作模式两种不同工作状态下流体动力的数学描述。

Because of the nonuniqueness in the positional solution, it's not easy to test the performance of the coordinated control system. So the model of NN was built to convert the vector of the length of 6 jars into the vector of the position of the motion deck. It's fast and accurate for the lengthwise direction. The state space system model of the six degree freedom motion simulator was built by the equations of electrodraulic servo mechanism and the multi-body dynamics equation of the six degree freedom motion simulator,the vector of the length of 6 jars was the control variable.

本文结合六自由度运动模拟器的多体动力学方程和电液伺服驱动机构的特性,经简化得出了具有实际意义的六自由度运动模拟器整体系统的状态空间方程式,通过分析该系统的稳定条件和能控性,采用状态反馈对系统的状态方程式进行合理配置,从而建立了以运动模拟器杆长向量为控制变量的运动模拟器整体控制系统,并将该控制系统输出的杆长向量转换为位置向量。

For a system comprising two or more objects, degrees of freedom are additive .

具有两个或更多个物体的系统,自由度更多。

I contend this is made possible by the method's loosely defined rules and the ability to postulate a large number of nested waves of varying magnitude. This gives the Elliott analyst the same freedom and flexibility that allowed pre-Copernican astronomers to explain all observed planet movements even though their underlying theory of an Earth-centered universe was wrong.

我认为这可能是因为波浪理论中对所定义的规则相对松散以及对诸多不同范围内的巢式波浪所作假设的能力,使艾略特分析人员都拥有相同的自由度和灵活性,正是这种自由度和灵活性,使哥白尼时代之前的天文学家能解释称前人观察到的所有的行星运动甚至他们以地球为中心的宇宙概念而提出的基础理论全部都是错误的。

I contend this is made possible by the method's loosely defined rules and the ability to postulate a large number of nested waves of varying magnitude. This gives the Elliott analyst the same freedom and flexibility that allowed pre-Copernican astronomers to explain all observed planet movements even though their underlying theory of an Earth-centered universe was wrong.

我认为这可能是因为波浪理论中对所定义的规则相对松散以及对诸多不同范围内的巢式波浪所作假设的能力,正因如此,使它们使艾略特分析人员都拥有同样的自由度和灵活性,而正是这种自由度和灵活性,使哥白尼时代之前的天文学家能解释称前人观察到的所有的行星运动甚至对其以地球为中心的宇宙概念而提出的基础理论全部都是错误的。

Because the rigid-body motion includes the translation along with center of mass and the rotation about it, there are couplings between different rigid-bodies, and between different degree-of-freedoms of a single rigid-body.

刚体运动包括质心的平动和绕质心的转动,因而多刚体系统中不仅包括刚体之间的自由度耦合,而且包括刚体本身自由度之间的耦合。

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