標(biāo)題: Titlebook: Dynamics of Multibody Systems; Robert E. Roberson,Richard Schwertassek Book 1988 Springer-Verlag Berlin Heidelberg 1988 design.dynamical s [打印本頁] 作者: 次要 時間: 2025-3-21 17:23
書目名稱Dynamics of Multibody Systems影響因子(影響力)
書目名稱Dynamics of Multibody Systems影響因子(影響力)學(xué)科排名
書目名稱Dynamics of Multibody Systems網(wǎng)絡(luò)公開度
書目名稱Dynamics of Multibody Systems網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Dynamics of Multibody Systems被引頻次
書目名稱Dynamics of Multibody Systems被引頻次學(xué)科排名
書目名稱Dynamics of Multibody Systems年度引用
書目名稱Dynamics of Multibody Systems年度引用學(xué)科排名
書目名稱Dynamics of Multibody Systems讀者反饋
書目名稱Dynamics of Multibody Systems讀者反饋學(xué)科排名
作者: optic-nerve 時間: 2025-3-21 21:06
Mathematical Preliminariesred. It is common practice to use the . as shown in Fig.1. It is characterized by the . of its origin . and by the . of three perpendicular axes, each of which has a . of distance established by making a correspondence between the real numbers and the Euclidean distance of each point on the axis fro作者: tic-douloureux 時間: 2025-3-22 01:13 作者: 火車車輪 時間: 2025-3-22 04:42
Velocityody can be derived. These variables are called .. Possibilities for describing the velocities of points of a rigid body can be based on the several methods of representing position discussed in Ch.3. Here we examine some of the basic concepts for representing ..作者: Malcontent 時間: 2025-3-22 10:50
Dynamical Equations . {.., e.} such that the mathematical equations based on the laws of Newton and Euler hold, namely: . Here .P is the linear momentum of the body with respect to the inertial frame and .H is the corresponding angular momentum. Dots indicate time derivatives with respect to the inertial frame. Quanti作者: brachial-plexus 時間: 2025-3-22 15:02 作者: brachial-plexus 時間: 2025-3-22 18:47 作者: crucial 時間: 2025-3-22 22:03 作者: 比喻好 時間: 2025-3-23 05:21 作者: 閃光東本 時間: 2025-3-23 05:47 作者: 記憶 時間: 2025-3-23 11:18 作者: 雕鏤 時間: 2025-3-23 16:22
Dynamical Equationsties F and .L are resultants of force and torque on the body, the reference point for the torque being point ... Equations 1 are the basic dynamical equations of motion, founded on independent laws of nature [1]. All subsequent manipulation simply recasts Eqs.1 in alternative forms. Initially we assume that the motions are unconstrained.作者: LUCY 時間: 2025-3-23 19:38 作者: 脊椎動物 時間: 2025-3-24 00:27 作者: cyanosis 時間: 2025-3-24 06:08 作者: 輕觸 時間: 2025-3-24 10:11 作者: optional 時間: 2025-3-24 12:26
vehicles, mechanisms, robots or biomechanical systems. This book adresses the general problem of analysing the behaviour of such multibody systems by digital simulation. This implies that pre-computer analytical methods for deriving the system equations must be replaced by systematic computer orien作者: vasculitis 時間: 2025-3-24 17:46 作者: Terrace 時間: 2025-3-24 19:50
Lynda Measor,Paula Wilcox,Philip Framete space form. Projecting them onto the constrained modes yields the unknown generalized constraint forces. These processes are given separately for systems with tree configurations and for those with closed kinematic chains.作者: 闖入 時間: 2025-3-25 02:14 作者: Basal-Ganglia 時間: 2025-3-25 05:18
John Field,Natalie Morgan-Kleinall other cases as well. But it is not the only requirement when developing a general-purpose multibody computer program. Others might be to minimize storage requirements (especially when implementing on a small computer), portability of code or the amount of time and labor needed to develop the computer code.作者: homocysteine 時間: 2025-3-25 10:47
Linearized Equationsed here, and variables are then separated into those describing the known nominal motion and others describing the unknown small deviations from it. Ultimately, a linearized state space representation of the motion is developed.作者: ostracize 時間: 2025-3-25 12:31
Computer Simulationall other cases as well. But it is not the only requirement when developing a general-purpose multibody computer program. Others might be to minimize storage requirements (especially when implementing on a small computer), portability of code or the amount of time and labor needed to develop the computer code.作者: Flatus 時間: 2025-3-25 18:55 作者: GLIDE 時間: 2025-3-25 22:21
escribing the system model - .solving. those complex equations yielding results ready for design evaluation. Emphasis is on computer based derivation of the system equations thus freeing the user from the time consuming and error-prone task of developing equations of motion for various problems again and again.978-3-642-86466-7978-3-642-86464-3作者: dissolution 時間: 2025-3-26 02:30
Multibody Systems part, by the end of the Sixteenth Century. Thereafter, the early goals were to understand and describe in mathematical terms the translational motion of material bodies, usually idealized as particles.作者: esoteric 時間: 2025-3-26 04:52 作者: Terminal 時間: 2025-3-26 11:23 作者: Fracture 時間: 2025-3-26 13:43
Special Topics this are interconnections with dry friction and with feedback control. In the former case the known interactions depend on the unknown constraint forces and torques. In the latter case they depend on additional states of the multibody system and the control system.作者: 溫順 時間: 2025-3-26 20:05 作者: agitate 時間: 2025-3-27 00:32 作者: FLIRT 時間: 2025-3-27 03:25
John Field,Natalie Morgan-KleinTo provide the modeling options for both kinematic and dynamic reference frames, the location of any body must be described with respect to points .. or .. respectively.作者: syring 時間: 2025-3-27 05:32 作者: 改變 時間: 2025-3-27 12:20 作者: periodontitis 時間: 2025-3-27 14:21
KinematicsTo provide the modeling options for both kinematic and dynamic reference frames, the location of any body must be described with respect to points .. or .. respectively.作者: HUMID 時間: 2025-3-27 20:14 作者: 極大痛苦 時間: 2025-3-28 01:36 作者: ATP861 時間: 2025-3-28 02:53 作者: 鴕鳥 時間: 2025-3-28 07:31 作者: 步履蹣跚 時間: 2025-3-28 12:27 作者: 他日關(guān)稅重重 時間: 2025-3-28 18:38
John Field,Natalie Morgan-Kleiner of mass is designated .. and its inertia dyadic with respect to the center of mass is l.. Internal angular momentum is h., nonzero for a gyrostat and zero for a rigid body. All vector bases are orthonormal and dextral. Base vectors e.= [e.] are rigidly embedded in the body at .., establishing a b作者: Paleontology 時間: 2025-3-28 19:54 作者: Nebulizer 時間: 2025-3-28 23:51
Lynda Measor,Paula Wilcox,Philip Framestem equations which still contain the constraint forces and torques. Projecting those equations onto the free modes of motion they are reduced to state space form. Projecting them onto the constrained modes yields the unknown generalized constraint forces. These processes are given separately for s作者: Confirm 時間: 2025-3-29 03:15
Mary Stuart,Catherine Lido,Jessica Morgan this are interconnections with dry friction and with feedback control. In the former case the known interactions depend on the unknown constraint forces and torques. In the latter case they depend on additional states of the multibody system and the control system.作者: angina-pectoris 時間: 2025-3-29 07:53 作者: aggrieve 時間: 2025-3-29 14:45
John Field,Natalie Morgan-Kleinis useful for system . and ., for . of system parameters and for . of assumptions on the modeling. Important approaches to system . involve the addition of feedback control based on real time plant models. In such cases and in situations where simulation is used to evaluate a cost function to be min作者: 不能平靜 時間: 2025-3-29 19:33 作者: AFFIX 時間: 2025-3-29 20:19
978-3-642-86466-7Springer-Verlag Berlin Heidelberg 1988作者: 反省 時間: 2025-3-30 02:00
http://image.papertrans.cn/e/image/284132.jpg作者: Badger 時間: 2025-3-30 05:56
Muslims as the Internal and External Enemy part, by the end of the Sixteenth Century. Thereafter, the early goals were to understand and describe in mathematical terms the translational motion of material bodies, usually idealized as particles.作者: asthma 時間: 2025-3-30 10:49 作者: 奇思怪想 時間: 2025-3-30 12:33
Mary Stuart,Catherine Lido,Jessica Morgand matrices .. by any suitable set of coordinates and velocities . those vector-dyadic equations go over into corresponding matrix equations whose general forms are . The specific forms of matrix .. in the kinematical equations, Eqs.2, and of matrices ., and Λ in the dynamical equations, Eqs.3, depend on the choice of variables .. and ...作者: 清晰 時間: 2025-3-30 19:42 作者: 顛簸下上 時間: 2025-3-30 23:24
Mathematical Preliminaries both location and orientation, we use the term . with this generalized meaning. As regards the numbering of the triad axes, in this book we use only . or . frames. A dextral frame is one in which a rotation about the 3-axis in a positive sense given by the right-hand rule moves the 1-axis toward th作者: ABOUT 時間: 2025-3-31 03:45
Location and Orientation the two frames as a function of time. Motion during which the relative orientation of the triads e. and e. does not change is called .. When .. remains in a fixed location with respect to .. the motion is called .. The most general motion of a rigid body can be composed of these two simple motions.
