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Holonomic systems. / Soltakhanov, Shervani Kh; Yushkov, Mikhail P.; Zegzhda, Sergei A.

Mechanics of non-holonomic systems: A New Class of control systems. ed. / Shervani Soltakhanov; Sergei Zegzhda; Mikhail Yushkov. 2009. p. 1-24 (Foundations in Engineering Mechanics).

Research output: Chapter in Book/Report/Conference proceedingChapterResearchpeer-review

Harvard

Soltakhanov, SK, Yushkov, MP & Zegzhda, SA 2009, Holonomic systems. in S Soltakhanov, S Zegzhda & M Yushkov (eds), Mechanics of non-holonomic systems: A New Class of control systems. Foundations in Engineering Mechanics, pp. 1-24. https://doi.org/10.1007/978-3-540-85847-8_1

APA

Soltakhanov, S. K., Yushkov, M. P., & Zegzhda, S. A. (2009). Holonomic systems. In S. Soltakhanov, S. Zegzhda, & M. Yushkov (Eds.), Mechanics of non-holonomic systems: A New Class of control systems (pp. 1-24). (Foundations in Engineering Mechanics). https://doi.org/10.1007/978-3-540-85847-8_1

Vancouver

Soltakhanov SK, Yushkov MP, Zegzhda SA. Holonomic systems. In Soltakhanov S, Zegzhda S, Yushkov M, editors, Mechanics of non-holonomic systems: A New Class of control systems. 2009. p. 1-24. (Foundations in Engineering Mechanics). https://doi.org/10.1007/978-3-540-85847-8_1

Author

Soltakhanov, Shervani Kh ; Yushkov, Mikhail P. ; Zegzhda, Sergei A. / Holonomic systems. Mechanics of non-holonomic systems: A New Class of control systems. editor / Shervani Soltakhanov ; Sergei Zegzhda ; Mikhail Yushkov. 2009. pp. 1-24 (Foundations in Engineering Mechanics).

BibTeX

@inbook{638b43d6563c4509872f7699d122c0c4,
title = "Holonomic systems",
abstract = "In this chapter we introduce a notion of the point that represents a motion of mechanical system. To generate Lagrange's equations of the first and second kinds we make use of the approach demonstrating their unity and generality. This approach permits us to write Lagrange's equations in the form, which can be used both in the case of one material (mass) point and of arbitrary mechanical system with finite or infinite numbers of degrees of freedom. The notion of ideal holonomic constraints is considered from the different points of view. The connection of the obtained equations of motion with the D'Alembert - Lagrange principle is analyzed. The longitudinal motion of a car with acceleration is considered as an example of motion of a holonomic system with a nonretaining constraint.",
author = "Soltakhanov, {Shervani Kh} and Yushkov, {Mikhail P.} and Zegzhda, {Sergei A.}",
note = "Copyright: Copyright 2009 Elsevier B.V., All rights reserved.",
year = "2009",
doi = "10.1007/978-3-540-85847-8_1",
language = "English",
isbn = "9783540858461",
series = "Foundations in Engineering Mechanics",
pages = "1--24",
editor = "Shervani Soltakhanov and Sergei Zegzhda and Mikhail Yushkov",
booktitle = "Mechanics of non-holonomic systems",

}

RIS

TY - CHAP

T1 - Holonomic systems

AU - Soltakhanov, Shervani Kh

AU - Yushkov, Mikhail P.

AU - Zegzhda, Sergei A.

N1 - Copyright: Copyright 2009 Elsevier B.V., All rights reserved.

PY - 2009

Y1 - 2009

N2 - In this chapter we introduce a notion of the point that represents a motion of mechanical system. To generate Lagrange's equations of the first and second kinds we make use of the approach demonstrating their unity and generality. This approach permits us to write Lagrange's equations in the form, which can be used both in the case of one material (mass) point and of arbitrary mechanical system with finite or infinite numbers of degrees of freedom. The notion of ideal holonomic constraints is considered from the different points of view. The connection of the obtained equations of motion with the D'Alembert - Lagrange principle is analyzed. The longitudinal motion of a car with acceleration is considered as an example of motion of a holonomic system with a nonretaining constraint.

AB - In this chapter we introduce a notion of the point that represents a motion of mechanical system. To generate Lagrange's equations of the first and second kinds we make use of the approach demonstrating their unity and generality. This approach permits us to write Lagrange's equations in the form, which can be used both in the case of one material (mass) point and of arbitrary mechanical system with finite or infinite numbers of degrees of freedom. The notion of ideal holonomic constraints is considered from the different points of view. The connection of the obtained equations of motion with the D'Alembert - Lagrange principle is analyzed. The longitudinal motion of a car with acceleration is considered as an example of motion of a holonomic system with a nonretaining constraint.

UR - http://www.scopus.com/inward/record.url?scp=67049100163&partnerID=8YFLogxK

U2 - 10.1007/978-3-540-85847-8_1

DO - 10.1007/978-3-540-85847-8_1

M3 - Chapter

AN - SCOPUS:67049100163

SN - 9783540858461

T3 - Foundations in Engineering Mechanics

SP - 1

EP - 24

BT - Mechanics of non-holonomic systems

A2 - Soltakhanov, Shervani

A2 - Zegzhda, Sergei

A2 - Yushkov, Mikhail

ER -

ID: 71885084