2011
DOI: 10.1002/zamm.201000228
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Dynamics of mechanical systems with nonlinear nonholonomic constraints – I The history of solving the problem of a material realization of a nonlinear nonholonomic constraint

Abstract: The paper brings forth a detailed analysis of the solution of the problem of the material realization of a nonlinear nonholonomic constraint (NNC). The existing models of the NNC are shown that can be classified into two groups: the first group comprises correctly realized physical models, while the second group contains the so‐called “quasinonlinear” nonholonomic constraints which in fact represent mathematical models. The correctness of the cited models is considered in detail, and the essential nature of su… Show more

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Cited by 8 publications
(9 citation statements)
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“…The axis of the non-stationary coordinate system A ξ is defined by the direction AB , that is, B Aξ  , whereas unit vectors of the non-stationary coordinate system axes are , λ μ   and ν  , respectively. The system is composed of two Chaplygin blades [3], of negligible masses and dimensions, which impose constraint to the motion of particles A and B, of equal masses m , in the form of perpendicularity of the velocities, as shown in Fig. 1.…”
Section: Description Of the Dynamic Model Of Nonlinear Nonholonomic Smentioning
confidence: 99%
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“…The axis of the non-stationary coordinate system A ξ is defined by the direction AB , that is, B Aξ  , whereas unit vectors of the non-stationary coordinate system axes are , λ μ   and ν  , respectively. The system is composed of two Chaplygin blades [3], of negligible masses and dimensions, which impose constraint to the motion of particles A and B, of equal masses m , in the form of perpendicularity of the velocities, as shown in Fig. 1.…”
Section: Description Of the Dynamic Model Of Nonlinear Nonholonomic Smentioning
confidence: 99%
“…q ,q ,q ,q , where 1 q x  and 2 q y  are Cartesian coordinates of the point A, 3 q φ  is the angle between the axis Ox and axis A ξ , while 4 q ξ  is the relative coordinate of point B relative to the nonstationary coordinate system. Further analysis relates to the case when the motion of point A is constrained in the Aξ axis direction, while the motion of point B is constrained in the Aη axis direction, that is, lateral slipping of the points A and B of the system is not permissible in the Aξ and Aη axis directions respectively.…”
Section: Description Of the Dynamic Model Of Nonlinear Nonholonomic Smentioning
confidence: 99%
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“…A nonholonomic mechanical system [3] is composed of two variable mass particles, A and B, whose motion is constrained by the imposition of perpendicularity of the velocities by means of the Chaplygin blades of negligible masses, as shown in Figure 1a. In order to develop the differential equations of motion of a variable mass nonholonomic mechanical system (henceforth referred to as 'the system'), as well as for the needs of further considerations, first, two Cartesian reference coordinate systems must be introduced: the stationary coordinate system Oxyz, whose coordinate plane Oxy coincides with the horizontal plane of motion, and the non-stationary coordinate system Aξηζ that is rigidly attached to point A of the system, so that the coordinate plane Aξη coincides with the plane Oxy (refer to Figure 1a).…”
Section: Introductionmentioning
confidence: 99%