2017
DOI: 10.1115/1.4036117
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Steering a Chaplygin Sleigh Using Periodic Impulses

Abstract: The control of the motion of nonholonomic systems is of practical importance from the perspective of robotics. In this paper, we consider the dynamics of a cartlike system that is both propelled forward by motion of an internal momentum wheel. This is a modification of the Chaplygin sleigh, a canonical nonholonomic system. For the system considered, the momentum wheel is the sole means of locomotive thrust as well the only control input. We first derive an analytical expression for the change in the heading an… Show more

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Cited by 18 publications
(19 citation statements)
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“…Various generalizations of the problem of the Chaplygin sleigh were considered by many authors [20,21,22,23,24,25,26,27,28]. In particular, attention was given to problems of the motion of the sleigh in the presence of periodic impulse impacts [20,21], with periodic switchovers of the nonholonomic constraint to different locations [23,24], and with periodic transfers of the massive load placed on the sleigh [25,26]. Analysis was also made of the motion of the sleigh under the action of random forces which model a fluctuating continuous medium [28], when, according to the authors, the motion resembles random walks of bacterial cells with a diffusion component.…”
Section: Introductionmentioning
confidence: 99%
“…Various generalizations of the problem of the Chaplygin sleigh were considered by many authors [20,21,22,23,24,25,26,27,28]. In particular, attention was given to problems of the motion of the sleigh in the presence of periodic impulse impacts [20,21], with periodic switchovers of the nonholonomic constraint to different locations [23,24], and with periodic transfers of the massive load placed on the sleigh [25,26]. Analysis was also made of the motion of the sleigh under the action of random forces which model a fluctuating continuous medium [28], when, according to the authors, the motion resembles random walks of bacterial cells with a diffusion component.…”
Section: Introductionmentioning
confidence: 99%
“…The equations of motion of the Chaplygin sleigh without the internal rotor, [6,12,18] can be obtained from (13) and (14) by setting ε = 0,…”
Section: Simulation Resultsmentioning
confidence: 99%
“…3 Equations (22) and (25) represent the leading order equations for the evolution of the velocity of the sleigh. These equations are the same as those that describe the motion of the Chaplygin sleigh without an internal rotor, (17), (18). The leading order solutions u 0 and Ω 0 are shown in Fig.…”
Section: Transient Dynamics Of the Sleigh And Regular Perturbation Exmentioning
confidence: 99%
“…On the other hand, if n < N − m then the system's motion involves dynamics, and is governed by interaction between the nonholonomic constraints and balance of generalized momentum variables. Examples of such systems are the snakeboard [9,10], roller racer [11,12], and several actuated variants of Chaplygin's sleigh [13,14,15]. There have been many works on dynamics and control of nonholonomic locomotion systems, exploiting their geometric structure for analyzing periodic control inputs [16,17].…”
Section: Scientific Backgroundmentioning
confidence: 99%